{"artifacts":{"doi:10.1007/s10973-014-4189-1/p7/tab-6":{"artifact":"table","caption":"Comparison of the experimental and calculated reactions of the holium–nickel system","label":"6","page":7},"doi:10.1007/s11661-020-05963-2/p12/tab-v":{"artifact":"table","caption":"A Summary of Results from the First-Principles Calculations","label":"V","page":12},"doi:10.1007/s11664-015-4272-9/p2/tab-ii":{"artifact":"table","caption":"Summary of crystallographic data for solid phases in Bi–Ni system","label":"II","page":2},"doi:10.1016/j.actamat.2010.09.055/p5/tab-1":{"artifact":"table","caption":"The present ab initio equilibrium lattice parameter, mean magnetic moments and site projected magnetic moments for ferromagnetic bcc Fe– Ni alloys.","label":"1","page":5},"doi:10.1016/j.calphad.2008.10.005/p10/tab-2":{"artifact":"table","caption":"Enthalpies of formation at 0 K of the end-members of the stable and metastable phases of the Fe–Nb–Ni system; our final choices of enthalpies at 0 K, A of our TDB, (magnetic effect excluded for the pure elements references) for all the CEF compounds; the A deduced from our AI results; the other possible A from the literature; the magnetic moments entered in our TDB; the magnetic moment obtained from our AI calculations; the ones proposed in the literature; our AI energies at 0 K including the magnetic effect of the pure elements references; the ones from the literature. The numbers (n) are for magnetism: (1) = FM (or NFM); (2) = NM; (3) = AFM; (4) = PM.","label":"2","page":10},"doi:10.1016/j.calphad.2017.09.004/p26/tab-3":{"artifact":"table","caption":"First-principles predictions of lattice parameters, enthalpies of formation, entropies of formation, zero point vibrational energies of the intermetallic compounds in the Yb-Ni system at 0K (marked by *) and ambient conditions, and their Standard Element Reference states, fcc-Yb and fcc-Ni. Available experimental data [12,13,17] are also included for comparison. The experimental data are all measured at ambient conditions.","label":"3","page":26},"doi:10.1016/j.intermet.2010.02.026/p7/tab-3":{"artifact":"table","caption":"Results of the atomistic calculations performed in this work, compared to the available literature data.","label":"3","page":7},"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1":{"artifact":"table","caption":"Enthalpy of mixing �H (J/mol), equilibrium lattice parameter a (Å) and mag- netic moment β (␮ B /atom) for Ba–Ni system obtained from first-principles calculations using SQS","label":"1","page":2},"doi:10.1016/j.jallcom.2014.08.200/p4/tab-5":{"artifact":"table","caption":"Calculated energy of formation (in kJ/mol-atom) of end members of Ni 3 Ti and NiTi phase by ﬁrst-principle method.","label":"5","page":4},"doi:10.1016/j.jallcom.2024.174011/p5/tab-4":{"artifact":"table","caption":"Enthalpy of formation values for sigma phases from the present work’s DFT- based calculations at 0 K.","label":"4","page":5},"doi:10.1016/j.msea.2005.02.037/p4/tab-2":{"artifact":"table","caption":"First-principles calculation results","label":"2","page":4},"doi:10.1016/j.tca.2018.08.011/p4/tab-1":{"artifact":"table","caption":"Calculated entropies at 298.15 K, S 298.15 , and enthalpies of formation at 298.15 K, ΔH 298.15 K . Comparison is made to calculated values by Berche et al.","label":"1","page":4},"sha256:01e2c117c65fb968/p2/tab-1":{"artifact":"table","caption":"Calculated total energies ( E ) and lattice parameters for fcc Co, Fe, Ni and Pt.","label":"1","page":2},"sha256:1d912ff9ab64cea0/p8/tab-2":{"artifact":"table","caption":"Comparison between SGTE and DFT lattice stabilities","label":"2","page":8},"sha256:66d905f81bb74d58/p5/tab-3":{"artifact":"table","caption":"Crystal structure of phases in the La–Ni–H system.","label":"3","page":5},"sha256:7a34c631d852730b/p3/tab-1":{"artifact":"table","caption":"Fe–Ni–Ti solid phases considered in this work: crystal structure data, temperature and composition ranges of stability, sublattice models.","label":"1","page":3},"sha256:864a974ee9a34cd4/p4/tab-2":{"artifact":"table","caption":"Calculated enthalpy of formation and cell parameters of pure elements and binary phases in Hf-Ni and Hf-Sn.","label":"2","page":4},"sha256:bcd69fa868b68ab2/p7/tab-6":{"artifact":"table","caption":"A summary of results from the first-principles calculations.","label":"6","page":7},"sha256:d74c2ece3dfbcad3/p5/tab-2":{"artifact":"table","caption":"The crystallographic data of solid phases in the La–Ni–Cu system.","label":"2","page":5},"sha256:fa1f9d709d911f4a/p42/tab-4":{"artifact":"table","caption":"The reported Curie temperature T C and magnetic moment β of fcc Ni.","label":"4","page":42}},"cite_as":{"also_cite":["the original source of every value you use (paper_citation / paper_doi, and cited_dois for values the paper cites from earlier work)"],"bibtex":"@misc{orchid_literature_2026,\n  author    = {Arr{\\'o}yave, Raymundo and Saal, James and Shin, Dongwon},\n  title     = {{ORCHID-Values: thermodynamic and phase-equilibrium values read from the literature}},\n  version   = {2026.10},\n  publisher = {Zenodo},\n  year      = {2026},\n  doi       = {10.5281/zenodo.23735569},\n  url       = {https://doi.org/10.5281/zenodo.23735569},\n  note      = {Version 1, machine-extracted}\n}","dataset":"literature","doi":"10.5281/zenodo.23735569","license":"CC-BY-4.0","part_of":{"bibtex":"@misc{orchid_data_2026,\n  author    = {Arr{\\'o}yave, Raymundo and Saal, James and Shin, Dongwon},\n  title     = {{ORCHID data: umbrella record of the ORCHID datasets}},\n  version   = {2026.10},\n  publisher = {Zenodo},\n  year      = {2026},\n  doi       = {10.5281/zenodo.23736065},\n  url       = {https://doi.org/10.5281/zenodo.23736065},\n  note      = {Version 1, machine-extracted}\n}","doi":"10.5281/zenodo.23736065","text":"R. Arróyave, J. Saal, D. Shin, ORCHID data: umbrella record of the ORCHID datasets (version 2026.10; Version 1, machine-extracted), Zenodo (2026). https://doi.org/10.5281/zenodo.23736065","title":"ORCHID data: umbrella record of the ORCHID datasets","url":"https://doi.org/10.5281/zenodo.23736065"},"release_tag":"v2026.10","status":"Version 1, machine-extracted: values were read by language-model readers constrained to quote their source and checked automatically, and the release was then audited on the printed pages by adversarial audits, an independent second review of fit-facing records and a preliminary human review of a frozen sample. Flags such as accepted and ESPEI-ready record screening results, not certification; known issues are listed in the release notes.","text":"R. Arróyave, J. Saal, D. Shin, ORCHID-Values: thermodynamic and phase-equilibrium values read from the literature (version 2026.10; Version 1, machine-extracted), Zenodo (2026). https://doi.org/10.5281/zenodo.23735569","title":"ORCHID-Values: thermodynamic and phase-equilibrium values read from the literature","url":"https://doi.org/10.5281/zenodo.23735569","version":"2026.10"},"contexts":{},"elements":["NI"],"licence":"CC BY 4.0 (ORCHID data; quotes are short excerpts kept for verification, the publishers' copyright, not relicensed)","models":{"M5e03aef9":{"catalog_entry":{"license":"CC BY 4.0","name":"HoNi-15Kar.tdb","source_url":"https://doi.org/10.1016/j.calphad.2025.102833","tier":"bundled"},"link_basis":"reporting_paper_own_model","model_citation":"J. Thermal Anal. Calorim., 119, 1225-34(2015).","model_doi":"10.1007/s10973-014-4189-1","reproduced_by_calculation":false,"tdb":"HoNi-15Kar.tdb","tdb_path":"databases/sgte-binary/HoNi-15Kar.tdb","tdb_sha256":"177f346c93bb88945400851e6f44de49db5f152086d2da69dc4ed49ef84fdb43"},"Mbcd30acd":{"catalog_entry":{"license":"CC BY 4.0","name":"HfNi-18Ros.tdb","source_url":"https://doi.org/10.1016/j.calphad.2025.102833","tier":"bundled"},"link_basis":"reporting_paper_own_model (TDB header cites this paper)","model_citation":"S.L. Shang, B. Gleeson, Z.-K. Liu, Thermochim. Acta, 668, 142-51(2018).","model_doi":"10.1016/j.tca.2018.08.011","tdb":"HfNi-18Ros.tdb","tdb_path":"databases/sgte-binary/HfNi-18Ros.tdb","tdb_sha256":"24edb198273bee61bfc8b65c445acb22ade2438aab084333b01f5a434c0a9d98"}},"note":"records[].locator.ref -> artifacts; records[].model -> models (full records: orchid-literature.jsonl.gz)","papers":{"doi:10.1002/pssa.2210470160":{"authors":["M. Maszkiewicz"],"citation":"M. Maszkiewicz, Specific heat of high purity nickel single crystal near the critical temperature, Phys. Stat. Sol. (a) 47, K77-K80 (1978).","container":"Phys. Stat. Sol. (a)","doi":"10.1002/pssa.2210470160","doi_url":"https://doi.org/10.1002/pssa.2210470160","id":"doi:10.1002/pssa.2210470160","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Specific heat of high purity nickel single crystal near the critical temperature","year":1978},"doi:10.1007/bf02665782":{"authors":["A. Bolcavage","U. R. Kattner"],"citation":"A. Bolcavage, U. R. Kattner, A reassessment of the calculated Ni-Nb phase diagram, JPE 17, 92-100 (1996).","container":"JPE","doi":"10.1007/bf02665782","doi_url":"https://doi.org/10.1007/bf02665782","id":"doi:10.1007/bf02665782","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"6466926aef8f5145","roles":["cited_source","reporting_paper"],"source_kinds":["journal_article"],"title":"A reassessment of the calculated Ni-Nb phase diagram","year":1996},"doi:10.1007/s10973-014-4189-1":{"authors":["S. Kardellass","C. Servant","N. Selhaoui"],"citation":"S. Kardellass, C. Servant, N. Selhaoui, Thermodynamic description of the holmium–nickel system, J Therm Anal Calorim 119, 1225-1234 (2015).","container":"J Therm Anal Calorim","doi":"10.1007/s10973-014-4189-1","doi_url":"https://doi.org/10.1007/s10973-014-4189-1","id":"doi:10.1007/s10973-014-4189-1","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"1e32bbadbeae410f","roles":["cited_source","reporting_paper"],"source_kinds":["journal_article"],"title":"Thermodynamic description of the holmium–nickel system","year":2015},"doi:10.1007/s11661-020-05963-2":{"authors":["Chenyang Zhou","Cuiping Guo","Jingbo Li","Changrong Li","Zhenmin Du"],"citation":"Chenyang Zhou, Cuiping Guo, Jingbo Li, Changrong Li, Zhenmin Du, Key Experiments and Thermodynamic Description of the Co-Nb-Ni System, Metall Mater Trans A 51, 5892-5911 (2020).","container":"Metall Mater Trans A","doi":"10.1007/s11661-020-05963-2","doi_url":"https://doi.org/10.1007/s11661-020-05963-2","id":"doi:10.1007/s11661-020-05963-2","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"a58c4cb851471e14","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Key Experiments and Thermodynamic Description of the Co-Nb-Ni System","year":2020},"doi:10.1007/s11664-015-4272-9":{"authors":["Yuling Liu","Shuhong Liu","Cong Zhang","Xingxu Lu","Chong Chen","Yong Du","Dragana Živković"],"citation":"Yuling Liu, Shuhong Liu, Cong Zhang, Xingxu Lu, Chong Chen, Yong Du et al., Thermodynamic Assessment of the Bi–Ni and Bi–Ni–X (X = Ag, Cu) Systems, Journal of Elec Materi 45, 1041-1056 (2016).","container":"Journal of Elec Materi","doi":"10.1007/s11664-015-4272-9","doi_url":"https://doi.org/10.1007/s11664-015-4272-9","id":"doi:10.1007/s11664-015-4272-9","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"efa089306722bbef","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Thermodynamic Assessment of the Bi–Ni and Bi–Ni–X (X = Ag, Cu) Systems","year":2016},"doi:10.1007/s11669-023-01079-3":{"authors":["Júlio César Pereira dos Santos","Sean Griesemer","Nathalie Dupin","Ursula R. Kattner","Chuan Liu","Daniela Ivanova","Thomas Hammerschmidt","Suzana G. Fries","Chris Wolverton","Carelyn E. Campbell"],"citation":"Júlio César Pereira dos Santos, Sean Griesemer, Nathalie Dupin, Ursula R. Kattner, Chuan Liu, Daniela Ivanova et al., Applying the Effective Bond Energy Formalism (EBEF) to Describe the Sigma (σ) Phase in the Co-Cr-Ni-Re System, J. Phase Equilib. Diffus. 45, 330-357 (2024).","container":"J. Phase Equilib. Diffus.","doi":"10.1007/s11669-023-01079-3","doi_url":"https://doi.org/10.1007/s11669-023-01079-3","id":"doi:10.1007/s11669-023-01079-3","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"1d912ff9ab64cea0","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Applying the Effective Bond Energy Formalism (EBEF) to Describe the Sigma (σ) Phase in the Co-Cr-Ni-Re System","year":2024},"doi:10.1016/0022-3697(81)90174-8":{"authors":["Peter J. Meschter","James W. Wright","Charlie R. Brooks","Thomas G. Kollie"],"citation":"Peter J. Meschter, James W. Wright, Charlie R. Brooks, Thomas G. Kollie, Physical contributions to the heat capacity of nickel, Journal of Physics and Chemistry of Solids 42, 861-871 (1981).","container":"Journal of Physics and Chemistry of Solids","doi":"10.1016/0022-3697(81)90174-8","doi_url":"https://doi.org/10.1016/0022-3697(81)90174-8","id":"doi:10.1016/0022-3697(81)90174-8","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Physical contributions to the heat capacity of nickel","year":1981},"doi:10.1016/0022-5088(72)90082-3":{"authors":["K.H.J. Buschow"],"citation":"K.H.J. Buschow, Note on the structure and occurrence of ytterbium transition metal compounds, Journal of the Less Common Metals 26, 329-333 (1972).","container":"Journal of the Less Common Metals","doi":"10.1016/0022-5088(72)90082-3","doi_url":"https://doi.org/10.1016/0022-5088(72)90082-3","id":"doi:10.1016/0022-5088(72)90082-3","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Note on the structure and occurrence of ytterbium transition metal compounds","year":1972},"doi:10.1016/0022-5088(73)90188-4":{"authors":["A. Palenzona","S. Cirafici"],"citation":"A. Palenzona, S. Cirafici, The ytterbium-nickel system, Journal of the Less Common Metals 33, 361-367 (1973).","container":"Journal of the Less Common Metals","doi":"10.1016/0022-5088(73)90188-4","doi_url":"https://doi.org/10.1016/0022-5088(73)90188-4","id":"doi:10.1016/0022-5088(73)90188-4","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"The ytterbium-nickel system","year":1973},"doi:10.1016/0364-5916(91)90030-n":{"authors":["A.T. Dinsdale"],"citation":"A.T. Dinsdale, SGTE data for pure elements, Calphad 15, 317-425 (1991).","container":"Calphad","doi":"10.1016/0364-5916(91)90030-n","doi_url":"https://doi.org/10.1016/0364-5916(91)90030-n","id":"doi:10.1016/0364-5916(91)90030-n","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"SGTE data for pure elements","year":1991},"doi:10.1016/0925-8388(92)90217-w":{"authors":["Zeng Kejun","Zeng Xianzhang","Jin Zhanpeng"],"citation":"Zeng Kejun, Zeng Xianzhang, Jin Zhanpeng, A thermodynamic calculation of the Ni-Nb phase diagram, Journal of Alloys and Compounds 179, 177-185 (1992).","container":"Journal of Alloys and Compounds","doi":"10.1016/0925-8388(92)90217-w","doi_url":"https://doi.org/10.1016/0925-8388(92)90217-w","id":"doi:10.1016/0925-8388(92)90217-w","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"A thermodynamic calculation of the Ni-Nb phase diagram","year":1992},"doi:10.1016/j.actamat.2010.09.055":{"authors":["W. Xiong","H. Zhang","L. Vitos","M. Selleby"],"citation":"W. Xiong, H. Zhang, L. Vitos, M. Selleby, Magnetic phase diagram of the Fe–Ni system, Acta Materialia 59, 521-530 (2011).","container":"Acta Materialia","doi":"10.1016/j.actamat.2010.09.055","doi_url":"https://doi.org/10.1016/j.actamat.2010.09.055","id":"doi:10.1016/j.actamat.2010.09.055","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"657f8eb449bcd089","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Magnetic phase diagram of the Fe–Ni system","year":2011},"doi:10.1016/j.calphad.2008.10.003":{"authors":["Jozefien De Keyzer","Gabriele Cacciamani","Nathalie Dupin","Patrick Wollants"],"citation":"Jozefien De Keyzer, Gabriele Cacciamani, Nathalie Dupin, Patrick Wollants, Thermodynamic modeling and optimization of the Fe–Ni–Ti system, Calphad 33, 109-123 (2009).","container":"Calphad","doi":"10.1016/j.calphad.2008.10.003","doi_url":"https://doi.org/10.1016/j.calphad.2008.10.003","id":"doi:10.1016/j.calphad.2008.10.003","kind":"corpus_paper","metadata_source":"crossref","roles":["cited_source","reporting_paper"],"source_kinds":["cited_work","journal_article"],"title":"Thermodynamic modeling and optimization of the Fe–Ni–Ti system","year":2009},"doi:10.1016/j.calphad.2008.10.005":{"authors":["Muriel Mathon","Damien Connétable","Bo Sundman","Jacques Lacaze"],"citation":"Muriel Mathon, Damien Connétable, Bo Sundman, Jacques Lacaze, Calphad-type assessment of the Fe–Nb–Ni ternary system, Calphad 33, 136-161 (2009).","container":"Calphad","doi":"10.1016/j.calphad.2008.10.005","doi_url":"https://doi.org/10.1016/j.calphad.2008.10.005","id":"doi:10.1016/j.calphad.2008.10.005","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"8546f9af08ff8ad5","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Calphad-type assessment of the Fe–Nb–Ni ternary system","year":2009},"doi:10.1016/j.calphad.2009.06.006":{"authors":["S.H. Zhou","Y. Wang","L.-Q. Chen","Z.-K. Liu","R.E. Napolitano"],"citation":"S.H. Zhou, Y. Wang, L.-Q. Chen, Z.-K. Liu, R.E. Napolitano, Solution-based thermodynamic modeling of the Ni–Ta and Ni–Mo–Ta systems using first-principle calculations, Calphad 33, 631-641 (2009).","container":"Calphad","doi":"10.1016/j.calphad.2009.06.006","doi_url":"https://doi.org/10.1016/j.calphad.2009.06.006","id":"doi:10.1016/j.calphad.2009.06.006","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"bcd69fa868b68ab2","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Solution-based thermodynamic modeling of the Ni–Ta and Ni–Mo–Ta systems using first-principle calculations","year":2009},"doi:10.1016/j.calphad.2011.04.005":{"authors":["DongEung Kim","James E. Saal","Liangcai Zhou","ShunLi Shang","Yong Du","Zi-Kui Liu"],"citation":"DongEung Kim, James E. Saal, Liangcai Zhou, ShunLi Shang, Yong Du, Zi-Kui Liu, Thermodynamic modeling of fcc order/disorder transformations in the Co–Pt system, Calphad 35, 323-330 (2011).","container":"Calphad","doi":"10.1016/j.calphad.2011.04.005","doi_url":"https://doi.org/10.1016/j.calphad.2011.04.005","id":"doi:10.1016/j.calphad.2011.04.005","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"01e2c117c65fb968","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Thermodynamic modeling of fcc order/disorder transformations in the Co–Pt system","year":2011},"doi:10.1016/j.calphad.2011.10.004":{"authors":["Xuehui An","Qian Li","Jieyu Zhang","Shuanglin Chen","Ying Yang"],"citation":"Xuehui An, Qian Li, Jieyu Zhang, Shuanglin Chen, Ying Yang, Phase equilibria of the La–Ni–Cu ternary system at 673 K: Thermodynamic modeling and experimental validation, Calphad 36, 8-15 (2012).","container":"Calphad","doi":"10.1016/j.calphad.2011.10.004","doi_url":"https://doi.org/10.1016/j.calphad.2011.10.004","id":"doi:10.1016/j.calphad.2011.10.004","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"d74c2ece3dfbcad3","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Phase equilibria of the La–Ni–Cu ternary system at 673 K: Thermodynamic modeling and experimental validation","year":2012},"doi:10.1016/j.calphad.2012.12.002":{"authors":["X.H. An","Q.F. Gu","J.Y. Zhang","S.L. Chen","X.B. Yu","Q. Li"],"citation":"X.H. An, Q.F. Gu, J.Y. Zhang, S.L. Chen, X.B. Yu, Q. Li, Experimental investigation and thermodynamic reassessment of La–Ni and LaNi5–H systems, Calphad 40, 48-55 (2013).","container":"Calphad","doi":"10.1016/j.calphad.2012.12.002","doi_url":"https://doi.org/10.1016/j.calphad.2012.12.002","id":"doi:10.1016/j.calphad.2012.12.002","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"66d905f81bb74d58","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Experimental investigation and thermodynamic reassessment of La–Ni and LaNi5–H systems","year":2013},"doi:10.1016/j.calphad.2017.09.004":{"authors":["Yong-Jie Hu","Yi Wang","Samad A. Firdosy","Kurt E. Star","Jean-Pierre Fleurial","Vilupanur A. Ravi","Zi-Kui Liu"],"citation":"Yong-Jie Hu, Yi Wang, Samad A. Firdosy, Kurt E. Star, Jean-Pierre Fleurial, Vilupanur A. Ravi et al., First-principles calculations and thermodynamic modeling of the Yb-Ni binary system, Calphad 59, 207-217 (2017).","container":"Calphad","doi":"10.1016/j.calphad.2017.09.004","doi_url":"https://doi.org/10.1016/j.calphad.2017.09.004","id":"doi:10.1016/j.calphad.2017.09.004","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"19054f532b8d407b","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"First-principles calculations and thermodynamic modeling of the Yb-Ni binary system","year":2017},"doi:10.1016/j.calphad.2021.102268":{"authors":["Liangyan Hao","Andrei Ruban","Wei Xiong"],"citation":"Liangyan Hao, Andrei Ruban, Wei Xiong, CALPHAD modeling based on Gibbs energy functions from zero kevin and improved magnetic model: A case study on the Cr–Ni system, Calphad 73, 102268 (2021).","container":"Calphad","doi":"10.1016/j.calphad.2021.102268","doi_url":"https://doi.org/10.1016/j.calphad.2021.102268","id":"doi:10.1016/j.calphad.2021.102268","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"fa1f9d709d911f4a","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"CALPHAD modeling based on Gibbs energy functions from zero kevin and improved magnetic model: A case study on the Cr–Ni system","year":2021},"doi:10.1016/j.commatsci.2016.08.042":{"authors":["A. Berche","J.C. Tédenac","P. Jund"],"citation":"A. Berche, J.C. Tédenac, P. Jund, Phase diagram and enthalpy of formation of Hf-Ni-Sn, Computational Materials Science 125, 271-277 (2016).","container":"Computational Materials Science","doi":"10.1016/j.commatsci.2016.08.042","doi_url":"https://doi.org/10.1016/j.commatsci.2016.08.042","id":"doi:10.1016/j.commatsci.2016.08.042","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"864a974ee9a34cd4","roles":["cited_source","reporting_paper"],"source_kinds":["journal_article"],"title":"Phase diagram and enthalpy of formation of Hf-Ni-Sn","year":2016},"doi:10.1016/j.intermet.2010.02.026":{"authors":["G. Cacciamani","A. Dinsdale","M. Palumbo","A. Pasturel"],"citation":"G. Cacciamani, A. Dinsdale, M. Palumbo, A. Pasturel, The Fe–Ni system: Thermodynamic modelling assisted by atomistic calculations, Intermetallics 18, 1148-1162 (2010).","container":"Intermetallics","doi":"10.1016/j.intermet.2010.02.026","doi_url":"https://doi.org/10.1016/j.intermet.2010.02.026","id":"doi:10.1016/j.intermet.2010.02.026","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"fe6d9732a0155b00","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"The Fe–Ni system: Thermodynamic modelling assisted by atomistic calculations","year":2010},"doi:10.1016/j.jallcom.2006.03.096":{"authors":["Shunli Shang","Zhi-Jie Liu","Zi-Kui Liu"],"citation":"Shunli Shang, Zhi-Jie Liu, Zi-Kui Liu, Thermodynamic modeling of the Ba–Ni–Ti system, Journal of Alloys and Compounds 430, 188-193 (2007).","container":"Journal of Alloys and Compounds","doi":"10.1016/j.jallcom.2006.03.096","doi_url":"https://doi.org/10.1016/j.jallcom.2006.03.096","id":"doi:10.1016/j.jallcom.2006.03.096","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"49b672c4721851fc","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Thermodynamic modeling of the Ba–Ni–Ti system","year":2007},"doi:10.1016/j.jallcom.2014.08.200":{"authors":["K. Santhy","K.C. Hari Kumar"],"citation":"K. Santhy, K.C. Hari Kumar, Thermodynamic reassessment of Nb-Ni-Ti system with order–disorder model, Journal of Alloys and Compounds 619, 733-747 (2015).","container":"Journal of Alloys and Compounds","doi":"10.1016/j.jallcom.2014.08.200","doi_url":"https://doi.org/10.1016/j.jallcom.2014.08.200","id":"doi:10.1016/j.jallcom.2014.08.200","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"ee2f0144eb04347f","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Thermodynamic reassessment of Nb-Ni-Ti system with order–disorder model","year":2015},"doi:10.1016/j.jallcom.2024.174011":{"authors":["Beril Tonyali","Hui Sun","Brandon Bocklund","John Paul Borgonia","Richard A. Otis","Shun-Li Shang","Zi-Kui Liu","Allison M. Beese"],"citation":"Beril Tonyali, Hui Sun, Brandon Bocklund, John Paul Borgonia, Richard A. Otis, Shun-Li Shang et al., Additively manufactured Ni-20Cr to V functionally graded material: Computational predictions and experimental verification of phase formations, Journal of Alloys and Compounds 985, 174011 (2024).","container":"Journal of Alloys and Compounds","doi":"10.1016/j.jallcom.2024.174011","doi_url":"https://doi.org/10.1016/j.jallcom.2024.174011","id":"doi:10.1016/j.jallcom.2024.174011","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"ba8a69e2f735607c","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"Additively manufactured Ni-20Cr to V functionally graded material: Computational predictions and experimental verification of phase formations","year":2024},"doi:10.1016/j.jmmm.2006.10.240":{"authors":["Ying Zhu","Ping Yu","Xiaofeng Jin","Ding-sheng Wang"],"citation":"Ying Zhu, Ping Yu, Xiaofeng Jin, Ding-sheng Wang, Curie temperature of body-centered-tetragonal Ni, Journal of Magnetism and Magnetic Materials 310, e301-e303 (2007).","container":"Journal of Magnetism and Magnetic Materials","doi":"10.1016/j.jmmm.2006.10.240","doi_url":"https://doi.org/10.1016/j.jmmm.2006.10.240","id":"doi:10.1016/j.jmmm.2006.10.240","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Curie temperature of body-centered-tetragonal Ni","year":2007},"doi:10.1016/j.msea.2005.02.037":{"authors":["S.H. Zhou","Y. Wang","C. Jiang","J.Z. Zhu","L.-Q. Chen","Z.-K. Liu"],"citation":"S.H. Zhou, Y. Wang, C. Jiang, J.Z. Zhu, L.-Q. Chen, Z.-K. Liu, First-principles calculations and thermodynamic modeling of the Ni–Mo system, Materials Science and Engineering: A 397, 288-296 (2005).","container":"Materials Science and Engineering: A","doi":"10.1016/j.msea.2005.02.037","doi_url":"https://doi.org/10.1016/j.msea.2005.02.037","id":"doi:10.1016/j.msea.2005.02.037","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"846e8e90422f237b","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"First-principles calculations and thermodynamic modeling of the Ni–Mo system","year":2005},"doi:10.1016/j.scriptamat.2004.09.007":{"authors":["Y. Wang","C. Woodward","S.H. Zhou","Z.-K. Liu","L.-Q. Chen"],"citation":"Y. Wang, C. Woodward, S.H. Zhou, Z.-K. Liu, L.-Q. Chen, Structural stability of Ni–Mo compounds from first-principles calculations, Scripta Materialia 52, 17-20 (2005).","container":"Scripta Materialia","doi":"10.1016/j.scriptamat.2004.09.007","doi_url":"https://doi.org/10.1016/j.scriptamat.2004.09.007","id":"doi:10.1016/j.scriptamat.2004.09.007","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Structural stability of Ni–Mo compounds from first-principles calculations","year":2005},"doi:10.1016/j.ssc.2007.01.001":{"authors":["Jian-Min Zhang","Hai-Tao Li","Ke-Wei Xu"],"citation":"Jian-Min Zhang, Hai-Tao Li, Ke-Wei Xu, The stability of FCC crystal Ni under uniaxial loading, Solid State Communications 141, 535-540 (2007).","container":"Solid State Communications","doi":"10.1016/j.ssc.2007.01.001","doi_url":"https://doi.org/10.1016/j.ssc.2007.01.001","id":"doi:10.1016/j.ssc.2007.01.001","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"The stability of FCC crystal Ni under uniaxial loading","year":2007},"doi:10.1016/j.tca.2018.08.011":{"authors":["A.J. Ross","T. Gheno","P.K. Ray","M.J. Kramer","X.L. Liu","G. Lindwall","B. Zhou","S.L. Shang","B. Gleeson","Z-K. Liu"],"citation":"A.J. Ross, T. Gheno, P.K. Ray, M.J. Kramer, X.L. Liu, G. Lindwall et al., A first-principles based description of the Hf-Ni system supported by high-temperature synchrotron experiments, Thermochimica Acta 668, 142-151 (2018).","container":"Thermochimica Acta","doi":"10.1016/j.tca.2018.08.011","doi_url":"https://doi.org/10.1016/j.tca.2018.08.011","id":"doi:10.1016/j.tca.2018.08.011","kind":"corpus_paper","metadata_source":"crossref","pdf_sha256_prefix":"619ca4f00babd65b","roles":["reporting_paper"],"source_kinds":["journal_article"],"title":"A first-principles based description of the Hf-Ni system supported by high-temperature synchrotron experiments","year":2018},"doi:10.1016/s0925-8388(00)01472-9":{"authors":["A. Watson","F.H. Hayes"],"citation":"A. Watson, F.H. Hayes, Some experiences modelling the sigma phase in the Ni–V system, Journal of Alloys and Compounds 320, 199-206 (2001).","container":"Journal of Alloys and Compounds","doi":"10.1016/s0925-8388(00)01472-9","doi_url":"https://doi.org/10.1016/s0925-8388(00)01472-9","id":"doi:10.1016/s0925-8388(00)01472-9","kind":"corpus_paper","metadata_source":"crossref","roles":["cited_source","reporting_paper"],"source_kinds":["cited_work","journal_article"],"title":"Some experiences modelling the sigma phase in the Ni–V system","year":2001},"doi:10.1080/14786443409462519":{"authors":["Alan W. Foster"],"citation":"Alan W. Foster, XLIV.<i>The temperature variation of the thermoelectric properties and the specific heat of nickel-chromium alloys</i>, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science 18, 470-488 (1934).","container":"The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science","doi":"10.1080/14786443409462519","doi_url":"https://doi.org/10.1080/14786443409462519","id":"doi:10.1080/14786443409462519","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"XLIV.<i>The temperature variation of the thermoelectric properties and the specific heat of nickel-chromium alloys</i>","year":1934},"doi:10.1098/rspa.1963.0045":{"authors":["J. Crangle","G. C. Hallam"],"citation":"J. Crangle, G. C. Hallam, The magnetization of face-centred cubic and body-centred cubic iron + nickel alloys, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences 272, 119-132 (1963).","container":"Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences","doi":"10.1098/rspa.1963.0045","doi_url":"https://doi.org/10.1098/rspa.1963.0045","id":"doi:10.1098/rspa.1963.0045","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"The magnetization of face-centred cubic and body-centred cubic iron + nickel alloys","year":1963},"doi:10.1103/physrev.136.a1626":{"authors":["James S. Kouvel","Michael E. Fisher"],"citation":"James S. Kouvel, Michael E. Fisher, Detailed Magnetic Behavior of Nickel Near its Curie Point, Phys. Rev. 136, A1626-A1632 (1964).","container":"Phys. Rev.","doi":"10.1103/physrev.136.a1626","doi_url":"https://doi.org/10.1103/physrev.136.a1626","id":"doi:10.1103/physrev.136.a1626","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Detailed Magnetic Behavior of Nickel Near its Curie Point","year":1964},"doi:10.1103/physrevb.16.4872":{"authors":["T. G. Kollie"],"citation":"T. G. Kollie, Measurement of the thermal-expansion coefficient of nickel from 300 to 1000 K and determination of the power-law constants near the Curie temperature, Phys. Rev. B 16, 4872-4881 (1977).","container":"Phys. Rev. B","doi":"10.1103/physrevb.16.4872","doi_url":"https://doi.org/10.1103/physrevb.16.4872","id":"doi:10.1103/physrevb.16.4872","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Measurement of the thermal-expansion coefficient of nickel from 300 to 1000 K and determination of the power-law constants near the Curie temperature","year":1977},"doi:10.1103/physrevb.77.054431":{"authors":["P. Yu","X. F. Jin","J. Kudrnovský","D. S. Wang","P. Bruno"],"citation":"P. Yu, X. F. Jin, J. Kudrnovský, D. S. Wang, P. Bruno, Curie temperatures of fcc and bcc nickel and permalloy: Supercell and Green’s function methods, Phys. Rev. B 77 (2008).","container":"Phys. Rev. B","doi":"10.1103/physrevb.77.054431","doi_url":"https://doi.org/10.1103/physrevb.77.054431","id":"doi:10.1103/physrevb.77.054431","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Curie temperatures of fcc and bcc nickel and permalloy: Supercell and Green’s function methods","year":2008},"doi:10.1143/jpsj.50.454":{"authors":["Hatsuo Tange","Takeshi Yonei","Mitita Goto"],"citation":"Hatsuo Tange, Takeshi Yonei, Mitita Goto, Forced Volume Magnetostriction of Ni-Cr Alloys, J. Phys. Soc. Jpn. 50, 454-460 (1981).","container":"J. Phys. Soc. Jpn.","doi":"10.1143/jpsj.50.454","doi_url":"https://doi.org/10.1143/jpsj.50.454","id":"doi:10.1143/jpsj.50.454","kind":"cited_work","metadata_source":"crossref","roles":["cited_source"],"source_kinds":["cited_work"],"title":"Forced Volume Magnetostriction of Ni-Cr Alloys","year":1981}},"part":1,"parts":1,"records":[{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"CO-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["fcc(Ni)"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-6I27XH5CWH","locator":{"ref":"doi:10.1007/s11661-020-05963-2/p12/tab-v","row":3},"method":"first-principles calculations","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1007/s11661-020-05963-2","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1007/s11661-020-05963-2","paper_id":"doi:10.1007/s11661-020-05963-2","phases":[{"label":"fcc(Ni)","model_phase":"FCC_A1"}],"pid":"doi:10.1007/s11661-020-05963-2/p12/tab-v/r03#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"MOLAR_VOLUME","property_group":"crystal structure","property_printed":"V0","reader_agreement":"single_reader","reader_agreement_label":"unconfirmed (single reader)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","text_layer"],"record_kind":"general_table","source_system":"CO-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (static calculation)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.544},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.3264,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/VOLUME","floor":0.03,"floor_unit":"relative (fraction of the value)","value":0.3264},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"Å3/atom","value_type":"VOLUME"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å3/atom","unit_basis":"column_header","unit_printed":"Å3/atom","value":10.88,"value_printed":10.88},{"chemical_system":"NI","cited_sources":[{"first_author":"Massalski","kind":"assessment","label":"47","reference":"T.B. Massalski, Binary Alloy Phase Diagrams, 2nd ed. (Metals Park: ASM International, 1990).","status":"resolved","year":"1990"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"corrections":[{"after":"NI","before":"BI-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["fcc(Ni)"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-VHADNQ7HST","locator":{"ref":"doi:10.1007/s11664-015-4272-9/p2/tab-ii","row":6},"model_unlinked_reason":"linked TDB not the reporting paper's own model (link basis: None)","observation_type":"structural_property","origin":{"basis":"cited_reference_is_assessment","class":"model_value","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1007/s11664-015-4272-9","paper_id":"doi:10.1007/s11664-015-4272-9","phases":[{"label":"fcc(Ni)"}],"pid":"doi:10.1007/s11664-015-4272-9/p2/tab-ii/r06#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"BI-NI","structure":{"pearson_symbol":"cF4","prototype":"Cu"},"system":"NI","temperature_K":298.15,"temperature_basis":"assumed_room_temperature","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02713,"sigma_method":{"basis":"calibrated","ci95":[0.005826,0.012707],"class":"model_calculated","entry":"model/LATTICE_LENGTH","floor":0.0077,"floor_unit":"relative (fraction of the value)","n_pairs":175,"value":0.02713},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"nm","value":3.524,"value_stored":0.3524},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"FE-NI","evidence":{"basis":"printed_overall_composition","overall_composition":{"FE":0.0,"NI":1.0},"phases":["bcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:T_K_explicit","state:computation_context","temperature not stated"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-4U4NGDPV44.22c972","locator":{"ref":"doi:10.1016/j.actamat.2010.09.055/p5/tab-1","row":16},"merged_ids":["ORC-4U4NGDPV44.33d45e"],"observation_type":"structural_property","origin":{"basis":"caption_names_first_principles_only","class":"computed","measured_in":"doi:10.1016/j.actamat.2010.09.055","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_stored":{"FE":0.0,"NI":1.0},"paper":"doi:10.1016/j.actamat.2010.09.055","paper_id":"doi:10.1016/j.actamat.2010.09.055","phases":[{"label":"bcc","model_phase":"BCC_A2"}],"pid":"doi:10.1016/j.actamat.2010.09.055/p5/tab-1/r16#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"FE-NI","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":5e-05},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02804,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.02804},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":5e-05},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"nm","value":2.8041,"value_stored":0.28041},{"chemical_system":"NI","cited_sources":[{"doi":"10.1007/bf02665782","first_author":"Bolcavage","kind":"assessment","label":"17","paper":"doi:10.1007/bf02665782","reference":"A. Bolcavage, U.R. Kattner, J. Phase Equilibria 17 (1996) 92–100.","status":"resolved","year":"1996"},{"doi":"10.1016/0925-8388(92)90217-w","first_author":"Kejun","kind":"unknown","label":"41","paper":"doi:10.1016/0925-8388(92)90217-w","reference":"Z. Kejun, Z. Xianzhang, J. Zhanpeng, J. Alloy Compd. 179 (1–2) (1992) 177–185.","status":"resolved","year":"1992"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_a"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-SOVSORX6GL.2596b2","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":6},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_a"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r06#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"A (TDB)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1.0},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":20.0,"value_printed":20000,"value_stored":20000.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1007/bf02665782","first_author":"Bolcavage","kind":"assessment","label":"17","paper":"doi:10.1007/bf02665782","reference":"A. Bolcavage, U.R. Kattner, J. Phase Equilibria 17 (1996) 92–100.","status":"resolved","year":"1996"},{"doi":"10.1016/0925-8388(92)90217-w","first_author":"Kejun","kind":"unknown","label":"41","paper":"doi:10.1016/0925-8388(92)90217-w","reference":"Z. Kejun, Z. Xianzhang, J. Zhanpeng, J. Alloy Compd. 179 (1–2) (1992) 177–185.","status":"resolved","year":"1992"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_a"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-SOVSORX6GL.679bf3","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":6},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_a"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r06#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref FM, FM)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.4613},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":9.226,"value_printed":9226,"value_stored":9226.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1007/bf02665782","first_author":"Bolcavage","kind":"assessment","label":"17","paper":"doi:10.1007/bf02665782","reference":"A. Bolcavage, U.R. Kattner, J. Phase Equilibria 17 (1996) 92–100.","status":"resolved","year":"1996"},{"doi":"10.1016/0925-8388(92)90217-w","first_author":"Kejun","kind":"unknown","label":"41","paper":"doi:10.1016/0925-8388(92)90217-w","reference":"Z. Kejun, Z. Xianzhang, J. Zhanpeng, J. Alloy Compd. 179 (1–2) (1992) 177–185.","status":"resolved","year":"1992"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_a"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-SOVSORX6GL.744ece","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":6},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_a"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r06#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref GHSER)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.0244},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":0.488,"value_printed":488,"value_stored":488.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/s0925-8388(00)01472-9","first_author":"Watson","kind":"assessment","label":"50","paper":"doi:10.1016/s0925-8388(00)01472-9","reference":"A. Watson, F.H. Hayes, J. Alloys Compd. 320 (2001) 199–206.","status":"resolved","year":"2001"},{"doi":"10.1016/j.ssc.2007.01.001","first_author":"Zhang","kind":"assessment","label":"58","paper":"doi:10.1016/j.ssc.2007.01.001","reference":"J.-M. Zhang, H.-T. Li, K.-W. Xu, Solid State Commun. 141 (2007) 535–540.","status":"resolved","year":"2007"},{"doi":"10.1016/j.jmmm.2006.10.240","first_author":"Zhu","kind":"unknown","label":"57","paper":"doi:10.1016/j.jmmm.2006.10.240","reference":"Y. Zhu, P. Yu, X. Jin, D.-S. Wang, J. Magn. Magn. Mater. 310 (2007) 301–303.","status":"resolved","year":"2007"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_22"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-RC3BSYWH7Y.2970ec","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":15},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_22"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r15#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref FM, NM)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":2.09625},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":41.925,"value_printed":41925,"value_stored":41925.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/s0925-8388(00)01472-9","first_author":"Watson","kind":"assessment","label":"50","paper":"doi:10.1016/s0925-8388(00)01472-9","reference":"A. Watson, F.H. Hayes, J. Alloys Compd. 320 (2001) 199–206.","status":"resolved","year":"2001"},{"doi":"10.1016/j.ssc.2007.01.001","first_author":"Zhang","kind":"assessment","label":"58","paper":"doi:10.1016/j.ssc.2007.01.001","reference":"J.-M. Zhang, H.-T. Li, K.-W. Xu, Solid State Commun. 141 (2007) 535–540.","status":"resolved","year":"2007"},{"doi":"10.1016/j.jmmm.2006.10.240","first_author":"Zhu","kind":"unknown","label":"57","paper":"doi:10.1016/j.jmmm.2006.10.240","reference":"Y. Zhu, P. Yu, X. Jin, D.-S. Wang, J. Magn. Magn. Mater. 310 (2007) 301–303.","status":"resolved","year":"2007"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_22"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-RC3BSYWH7Y.2cd403","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":15},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_22"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r15#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref FM, FM)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1.7891},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":35.782,"value_printed":35782,"value_stored":35782.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/s0925-8388(00)01472-9","first_author":"Watson","kind":"assessment","label":"50","paper":"doi:10.1016/s0925-8388(00)01472-9","reference":"A. Watson, F.H. Hayes, J. Alloys Compd. 320 (2001) 199–206.","status":"resolved","year":"2001"},{"doi":"10.1016/j.ssc.2007.01.001","first_author":"Zhang","kind":"assessment","label":"58","paper":"doi:10.1016/j.ssc.2007.01.001","reference":"J.-M. Zhang, H.-T. Li, K.-W. Xu, Solid State Commun. 141 (2007) 535–540.","status":"resolved","year":"2007"},{"doi":"10.1016/j.jmmm.2006.10.240","first_author":"Zhu","kind":"unknown","label":"57","paper":"doi:10.1016/j.jmmm.2006.10.240","reference":"Y. Zhu, P. Yu, X. Jin, D.-S. Wang, J. Magn. Magn. Mater. 310 (2007) 301–303.","status":"resolved","year":"2007"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_22"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-RC3BSYWH7Y.b9c91b","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":15},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_22"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r15#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"A (TDB)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1.0},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":20.0,"value_printed":20000,"value_stored":20000.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/s0925-8388(00)01472-9","first_author":"Watson","kind":"assessment","label":"50","paper":"doi:10.1016/s0925-8388(00)01472-9","reference":"A. Watson, F.H. Hayes, J. Alloys Compd. 320 (2001) 199–206.","status":"resolved","year":"2001"},{"doi":"10.1016/j.ssc.2007.01.001","first_author":"Zhang","kind":"assessment","label":"58","paper":"doi:10.1016/j.ssc.2007.01.001","reference":"J.-M. Zhang, H.-T. Li, K.-W. Xu, Solid State Commun. 141 (2007) 535–540.","status":"resolved","year":"2007"},{"doi":"10.1016/j.jmmm.2006.10.240","first_author":"Zhu","kind":"unknown","label":"57","paper":"doi:10.1016/j.jmmm.2006.10.240","reference":"Y. Zhu, P. Yu, X. Jin, D.-S. Wang, J. Magn. Magn. Mater. 310 (2007) 301–303.","status":"resolved","year":"2007"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_22"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-RC3BSYWH7Y.ba0343","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":15},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_22"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r15#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref GHSER, NM)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1.65935},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":33.187,"value_printed":33187,"value_stored":33187.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/s0925-8388(00)01472-9","first_author":"Watson","kind":"assessment","label":"50","paper":"doi:10.1016/s0925-8388(00)01472-9","reference":"A. Watson, F.H. Hayes, J. Alloys Compd. 320 (2001) 199–206.","status":"resolved","year":"2001"},{"doi":"10.1016/j.ssc.2007.01.001","first_author":"Zhang","kind":"assessment","label":"58","paper":"doi:10.1016/j.ssc.2007.01.001","reference":"J.-M. Zhang, H.-T. Li, K.-W. Xu, Solid State Commun. 141 (2007) 535–540.","status":"resolved","year":"2007"},{"doi":"10.1016/j.jmmm.2006.10.240","first_author":"Zhu","kind":"unknown","label":"57","paper":"doi:10.1016/j.jmmm.2006.10.240","reference":"Y. Zhu, P. Yu, X. Jin, D.-S. Wang, J. Magn. Magn. Mater. 310 (2007) 301–303.","status":"resolved","year":"2007"}],"conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"FE-NB-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NB":0.0,"NI":1.0},"phases":["D0_22"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-RC3BSYWH7Y.ecb543","locator":{"ref":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2","row":15},"observation_type":"equilibrium_property","origin":{"basis":"this_work_kind_unstated_modelling_paper","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2008.10.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NB":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2008.10.005","paper_id":"doi:10.1016/j.calphad.2008.10.005","phases":[{"label":"D0_22"}],"pid":"doi:10.1016/j.calphad.2008.10.005/p10/tab-2/r15#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH (AI ref GHSER, FM)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NB":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"FE-NB-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1.3522},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.5,"sigma_method":{"basis":"calibrated","ci95":[2.41122,4.298262],"class":"unknown","entry":"value_types/HM_FORM/classes/unknown","floor":3.5,"floor_unit":"kJ/mol-atom","n_pairs":290,"value":3.5},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"J/mol","unit_stored":"J/mol (basis unstated)","value":27.044,"value_printed":27044,"value_stored":27044.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0022-5088(72)90082-3","first_author":"Buschow","kind":"unknown","label":"17","paper":"doi:10.1016/0022-5088(72)90082-3","reference":"K.H.J. Buschow, Note on the structure and occurrence of ytterbium transition metal compounds, Journal of the Less Common Metals, 26 (1972) 329–333.","status":"resolved","year":"1972"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"corrections":[{"after":298.15,"before":0.0,"evidence":{"caption":"First-principles predictions of lattice parameters, enthalpies of formation, entropies of formation, zero point vibrational energies of the intermetallic compou","why":"0 K is the temperature of the first-principles columns of the table, not of this cited experimental value; formation quantities are standard (298.15 K), others unstated"},"field":"temperature_K","gate":"R2","rule":"experimental_value_from_0K_caption","visual_check":{"checked":"2026-10-24","image_sha256":"797bae5146d08da7016bcf863d95822304e3e45ac67e031a49aad7fa228cf482","page":3,"pdf_sha256_prefix":"664f945fea949860","seen":"Cited experimental values in tables captioned 0 K / first-principles took 0 K; formation quantities are standard (298.15 K), ambient when the caption says so, unstated otherwise.","verdict":"rule_confirmed"}},{"after":"NI","before":"NI-YB","evidence":{"basis":"phase_formula","overall_composition":{"YB":0.0},"phases":["fcc-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":{"NI":1.0},"before":{},"evidence":{"class":"temperature","decision_file":"temperature_t060.json","doi":"10.1016/j.calphad.2017.09.004","pdf_page":26,"pdf_sha256":"19054f532b8d407b6f98e4a3ae0ddc78fce961078dfc9ae8e0b1884b2bc95bf9","printed":"fcc-Ni XRD 3.524 [17]; XRD 3.525 [12]; FP PBE 3.531* This work","rationale":"phase is pure fcc-Ni; chemical_system NI; unary convention {X: 1.0} as sibling fcc-Yb {YB: 1.0}","report_id":"ORCHID-TD-20261028-v1","table":"3","table_key":"t060"},"field":"overall_composition","gate":"TD20261028","rule":"source_adjudicated_table_defect","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1","image_sha256":"bbffca4f9b09a7132f84cdb35382023da39fa82f07a8711f97afd5bc0a1671e2","page":26,"pdf_sha256_prefix":"19054f532b8d407b","seen":"fcc-Ni group rows 1-3 (pure Ni)","verdict":"confirmed"}}],"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"awaiting_reader","specification_gaps":["table_defect_correction_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"id":"ORC-ZFHGIWUYEC.261581","locator":{"ref":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3","row":1},"merged_ids":["ORC-ZFHGIWUYEC.7273c4"],"method":"XRD","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"YB":0.0},"paper":"doi:10.1016/j.calphad.2017.09.004","paper_id":"doi:10.1016/j.calphad.2017.09.004","phases":[{"label":"fcc-Ni","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3/r01#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"NI":{"phase":"FCC_A1"},"YB":{"phase":"FCC_A1"}},"source_system":"NI-YB","system":"NI","temperature_K":298.15,"temperature_K_stored":0.0,"temperature_basis":"caption_ambient","temperature_printed":"0K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.1762},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.004581,"sigma_method":{"basis":"calibrated","ci95":[0.000866,0.003941],"class":"xrd","entry":"value_types/LATTICE_LENGTH/classes/xrd","floor":0.0013,"floor_unit":"relative (fraction of the value)","n_pairs":30,"value":0.004581},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.524,"value_printed":3.524,"value_stored":3.524},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0022-5088(73)90188-4","first_author":"Palenzona","kind":"unknown","label":"12","paper":"doi:10.1016/0022-5088(73)90188-4","reference":"A. Palenzona, S. Cirafici, The ytterbium-nickel system, Journal of the Less Common Metals, 33 (1973) 361–367.","status":"resolved","year":"1973"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"corrections":[{"after":298.15,"before":0.0,"evidence":{"caption":"First-principles predictions of lattice parameters, enthalpies of formation, entropies of formation, zero point vibrational energies of the intermetallic compou","why":"0 K is the temperature of the first-principles columns of the table, not of this cited experimental value; formation quantities are standard (298.15 K), others unstated"},"field":"temperature_K","gate":"R2","rule":"experimental_value_from_0K_caption","visual_check":{"checked":"2026-10-24","image_sha256":"797bae5146d08da7016bcf863d95822304e3e45ac67e031a49aad7fa228cf482","page":3,"pdf_sha256_prefix":"664f945fea949860","seen":"Cited experimental values in tables captioned 0 K / first-principles took 0 K; formation quantities are standard (298.15 K), ambient when the caption says so, unstated otherwise.","verdict":"rule_confirmed"}},{"after":"NI","before":"NI-YB","evidence":{"basis":"phase_formula","overall_composition":{"YB":0.0},"phases":["fcc-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":{"NI":1.0},"before":{},"evidence":{"class":"temperature","decision_file":"temperature_t060.json","doi":"10.1016/j.calphad.2017.09.004","pdf_page":26,"pdf_sha256":"19054f532b8d407b6f98e4a3ae0ddc78fce961078dfc9ae8e0b1884b2bc95bf9","printed":"fcc-Ni XRD 3.524 [17]; XRD 3.525 [12]; FP PBE 3.531* This work","rationale":"phase is pure fcc-Ni; chemical_system NI; unary convention {X: 1.0} as sibling fcc-Yb {YB: 1.0}","report_id":"ORCHID-TD-20261028-v1","table":"3","table_key":"t060"},"field":"overall_composition","gate":"TD20261028","rule":"source_adjudicated_table_defect","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1","image_sha256":"bbffca4f9b09a7132f84cdb35382023da39fa82f07a8711f97afd5bc0a1671e2","page":26,"pdf_sha256_prefix":"19054f532b8d407b","seen":"fcc-Ni group rows 1-3 (pure Ni)","verdict":"confirmed"}}],"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["table_defect_correction_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"id":"ORC-TDHPQBYUMS.127862","locator":{"ref":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3","row":2},"merged_ids":["ORC-TDHPQBYUMS.237403"],"method":"XRD","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"printed_source_experimental","class":"experimental","measured_in":"doi:10.1016/0022-5088(73)90188-4","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"YB":0.0},"paper":"doi:10.1016/j.calphad.2017.09.004","paper_id":"doi:10.1016/j.calphad.2017.09.004","phases":[{"label":"fcc-Ni","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3/r02#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"Lattice parameter a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"NI":{"phase":"FCC_A1"},"YB":{"phase":"FCC_A1"}},"source_system":"NI-YB","system":"NI","temperature_K":298.15,"temperature_K_stored":0.0,"temperature_basis":"caption_ambient","temperature_printed":"0K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.17625},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.004582,"sigma_method":{"basis":"calibrated","ci95":[0.000866,0.003941],"class":"xrd","entry":"value_types/LATTICE_LENGTH/classes/xrd","floor":0.0013,"floor_unit":"relative (fraction of the value)","n_pairs":30,"value":0.004582},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.525,"value_printed":3.525,"value_stored":3.525},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"NI-YB","evidence":{"basis":"phase_formula","overall_composition":{"YB":0.0},"phases":["fcc-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":{"NI":1.0},"before":{},"evidence":{"class":"temperature","decision_file":"temperature_t060.json","doi":"10.1016/j.calphad.2017.09.004","pdf_page":26,"pdf_sha256":"19054f532b8d407b6f98e4a3ae0ddc78fce961078dfc9ae8e0b1884b2bc95bf9","printed":"fcc-Ni XRD 3.524 [17]; XRD 3.525 [12]; FP PBE 3.531* This work","rationale":"phase is pure fcc-Ni; chemical_system NI; unary convention {X: 1.0} as sibling fcc-Yb {YB: 1.0}","report_id":"ORCHID-TD-20261028-v1","table":"3","table_key":"t060"},"field":"overall_composition","gate":"TD20261028","rule":"source_adjudicated_table_defect","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1","image_sha256":"bbffca4f9b09a7132f84cdb35382023da39fa82f07a8711f97afd5bc0a1671e2","page":26,"pdf_sha256_prefix":"19054f532b8d407b","seen":"fcc-Ni group rows 1-3 (pure Ni)","verdict":"confirmed"}}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"disputed_normalization_only","specification_gaps":["table_defect_correction_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"id":"ORC-IAXRV6DN7K.189ffc","locator":{"ref":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3","row":3},"merged_ids":["ORC-IAXRV6DN7K.2e430b"],"method":"FP PBE","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.calphad.2017.09.004","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"YB":0.0},"paper":"doi:10.1016/j.calphad.2017.09.004","paper_id":"doi:10.1016/j.calphad.2017.09.004","phases":[{"label":"fcc-Ni","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3/r03#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"NI":{"phase":"FCC_A1"},"YB":{"phase":"FCC_A1"}},"source_system":"NI-YB","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.17655},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.03531,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.03531},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.531,"value_printed":3.531,"value_stored":3.531},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"NI-YB","evidence":{"basis":"phase_formula","overall_composition":{"YB":0.0},"phases":["fcc-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["ambient_value_stored_at_0K"],"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"gate_failures":[{"code":"ambient_value_stored_at_0K","detail":"FP PBE 3.540 has no '*': per caption it is the ambient-conditions prediction, but stored T=0.0 (printed). Page gives 'ambient conditions', no number (siblings use 298.15 caption_ambient). Composition also empty (should be {NI: 1.0})","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1 (temperature, t060)","image_sha256":"bbffca4f9b09a7132f84cdb35382023da39fa82f07a8711f97afd5bc0a1671e2","page":26,"pdf_sha256_prefix":"19054f532b8d407b","seen":"fcc-Ni FP PBE 3.531* / 3.540 This work","verdict":"confirmed"}}],"id":"ORC-ZJ37KVI7VQ.224856","locator":{"ref":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3","row":4},"merged_ids":["ORC-ZJ37KVI7VQ.b14e01"],"method":"FP PBE","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.calphad.2017.09.004","own_work_of_paper":true},"overall_composition":{},"overall_composition_basis":"from_formula","overall_composition_stored":{"YB":0.0},"paper":"doi:10.1016/j.calphad.2017.09.004","paper_id":"doi:10.1016/j.calphad.2017.09.004","phases":[{"label":"fcc-Ni","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.calphad.2017.09.004/p26/tab-3/r04#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"NI":{"phase":"FCC_A1"},"YB":{"phase":"FCC_A1"}},"source_system":"NI-YB","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.177},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.0354,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.0354},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.54,"value_printed":3.54,"value_stored":3.54},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"FE-NI","evidence":{"basis":"printed_overall_composition","overall_composition":{"FE":0.0,"NI":1.0},"phases":["Ni A1"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["phase_label_not_the_value_phase"],"review_state":"extracted","system_is_state_subsystem":true,"system_mismatch":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"phase_label_not_the_value_phase","detail":"Ni rows print Structure A1 with Lattice bcc (a0 0.2800, ΔH 9.2) and A2 with fcc (a0 0.3518, ΔH 0): structure and lattice columns contradict; labels 'Ni A1'/'Ni A2' likely swapped but the page does not decide.","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1 (phase2, t140)","image_sha256":"2675cc935949178e094e475ece20102190ff4498d56c02dc83c4e61950ecd313","page":7,"pdf_sha256_prefix":"fe6d9732a0155b00","seen":"row 13: Ni | A1 cF4-Cu | bcc | 100 | 9.2 | 0.2800; row 14: Ni | A2 cI2-W | fcc | 100 | 0 | 0.3518","verdict":"confirmed"}}],"id":"ORC-RATDL7RTN4","locator":{"ref":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3","row":13},"method":"first-principles (atomistic) calculations","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.intermet.2010.02.026","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_stored":{"FE":0.0,"NI":1.0},"paper":"doi:10.1016/j.intermet.2010.02.026","paper_id":"doi:10.1016/j.intermet.2010.02.026","phases":[{"label":"Ni A1"}],"pid":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3/r13#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"phase":"BCC_A2"},"NI":{"phase":"FCC_A1"}},"source_system":"FE-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.46},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"column_header","unit_printed":"kJ/mol at","unit_stored":"J/mol-atom","value":9.2,"value_printed":9.2,"value_stored":9200.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"FE-NI","evidence":{"basis":"printed_overall_composition","overall_composition":{"FE":0.0,"NI":1.0},"phases":["Ni A1"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["phase_label_not_the_value_phase"],"review_state":"extracted","system_is_state_subsystem":true,"system_mismatch":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"phase_label_not_the_value_phase","detail":"Ni rows print Structure A1 with Lattice bcc (a0 0.2800, ΔH 9.2) and A2 with fcc (a0 0.3518, ΔH 0): structure and lattice columns contradict; labels 'Ni A1'/'Ni A2' likely swapped but the page does not decide.","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1 (phase2, t140)","image_sha256":"2675cc935949178e094e475ece20102190ff4498d56c02dc83c4e61950ecd313","page":7,"pdf_sha256_prefix":"fe6d9732a0155b00","seen":"row 13: Ni | A1 cF4-Cu | bcc | 100 | 9.2 | 0.2800; row 14: Ni | A2 cI2-W | fcc | 100 | 0 | 0.3518","verdict":"confirmed"}}],"id":"ORC-SV2DYP2GC2","locator":{"ref":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3","row":13},"method":"first-principles (atomistic) calculations","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.intermet.2010.02.026","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_stored":{"FE":0.0,"NI":1.0},"paper":"doi:10.1016/j.intermet.2010.02.026","paper_id":"doi:10.1016/j.intermet.2010.02.026","phases":[{"label":"Ni A1"}],"pid":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3/r13#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_UNSPECIFIED_AXIS","property_group":"crystal structure","property_printed":"a0","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"phase":"BCC_A2"},"NI":{"phase":"FCC_A1"}},"source_system":"FE-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.14},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.05,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.028},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_basis":"column_header","unit_printed":"nm","unit_stored":"nm","value":2.8,"value_printed":0.28,"value_stored":0.28},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"FE-NI","evidence":{"basis":"printed_overall_composition","overall_composition":{"FE":0.0,"NI":1.0},"phases":["Ni A2"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["phase_label_not_the_value_phase"],"review_state":"extracted","system_is_state_subsystem":true,"system_mismatch":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"phase_label_not_the_value_phase","detail":"Ni rows print Structure A1 with Lattice bcc (a0 0.2800, ΔH 9.2) and A2 with fcc (a0 0.3518, ΔH 0): structure and lattice columns contradict; labels 'Ni A1'/'Ni A2' likely swapped but the page does not decide.","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1 (phase2, t140)","image_sha256":"2675cc935949178e094e475ece20102190ff4498d56c02dc83c4e61950ecd313","page":7,"pdf_sha256_prefix":"fe6d9732a0155b00","seen":"row 13: Ni | A1 cF4-Cu | bcc | 100 | 9.2 | 0.2800; row 14: Ni | A2 cI2-W | fcc | 100 | 0 | 0.3518","verdict":"confirmed"}}],"id":"ORC-M6ZH5C4SG6","locator":{"ref":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3","row":14},"method":"first-principles (atomistic) calculations","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.intermet.2010.02.026","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_stored":{"FE":0.0,"NI":1.0},"paper":"doi:10.1016/j.intermet.2010.02.026","paper_id":"doi:10.1016/j.intermet.2010.02.026","phases":[{"label":"Ni A2"}],"pid":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3/r14#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"phase":"BCC_A2"},"NI":{"phase":"FCC_A1"}},"source_system":"FE-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"column_header","unit_printed":"kJ/mol at","unit_stored":"J/mol-atom","value":0.0,"value_printed":0.0,"value_stored":0.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"FE-NI","evidence":{"basis":"printed_overall_composition","overall_composition":{"FE":0.0,"NI":1.0},"phases":["Ni A2"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["phase_label_not_the_value_phase"],"review_state":"extracted","system_is_state_subsystem":true,"system_mismatch":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"phase_label_not_the_value_phase","detail":"Ni rows print Structure A1 with Lattice bcc (a0 0.2800, ΔH 9.2) and A2 with fcc (a0 0.3518, ΔH 0): structure and lattice columns contradict; labels 'Ni A1'/'Ni A2' likely swapped but the page does not decide.","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-28; Claude (Studio sub-agent readers) rendered-page check, AI-assisted, not human re-review; ORCHID-TD-20261028-v1 (phase2, t140)","image_sha256":"2675cc935949178e094e475ece20102190ff4498d56c02dc83c4e61950ecd313","page":7,"pdf_sha256_prefix":"fe6d9732a0155b00","seen":"row 13: Ni | A1 cF4-Cu | bcc | 100 | 9.2 | 0.2800; row 14: Ni | A2 cI2-W | fcc | 100 | 0 | 0.3518","verdict":"confirmed"}}],"id":"ORC-32TJT4ZUEC","locator":{"ref":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3","row":14},"method":"first-principles (atomistic) calculations","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.intermet.2010.02.026","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_stored":{"FE":0.0,"NI":1.0},"paper":"doi:10.1016/j.intermet.2010.02.026","paper_id":"doi:10.1016/j.intermet.2010.02.026","phases":[{"label":"Ni A2"}],"pid":"doi:10.1016/j.intermet.2010.02.026/p7/tab-3/r14#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_UNSPECIFIED_AXIS","property_group":"crystal structure","property_printed":"a0","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"FE":{"phase":"BCC_A2"},"NI":{"phase":"FCC_A1"}},"source_system":"FE-NI","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.1759},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.03518,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.03518},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_basis":"column_header","unit_printed":"nm","unit_stored":"nm","value":3.518,"value_printed":0.3518,"value_stored":0.3518},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"BA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Bcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-UTNDABMEJB.28c421","locator":{"ref":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1","row":5},"method":"first-principles (SQS)","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2006.03.096","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.jallcom.2006.03.096","paper_id":"doi:10.1016/j.jallcom.2006.03.096","phases":[{"label":"Bcc","model_phase":"BCC_A2"}],"pid":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1/r05#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a (M)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","source_system":"BA-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (static calculation)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.13995},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02799,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.02799},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":2.799,"value_printed":2.799,"value_stored":2.799},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"BA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Bcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-UTNDABMEJB.569cdf","locator":{"ref":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1","row":5},"method":"first-principles (SQS)","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2006.03.096","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.jallcom.2006.03.096","paper_id":"doi:10.1016/j.jallcom.2006.03.096","phases":[{"label":"Bcc","model_phase":"BCC_A2"}],"pid":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1/r05#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","source_system":"BA-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (static calculation)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.1396},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02792,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.02792},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":2.792,"value_printed":2.792,"value_stored":2.792},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"BA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Fcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-FH67ZBF6LL.0b0dd5","locator":{"ref":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1","row":10},"method":"first-principles (SQS)","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2006.03.096","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.jallcom.2006.03.096","paper_id":"doi:10.1016/j.jallcom.2006.03.096","phases":[{"label":"Fcc","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1/r10#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a (M)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","source_system":"BA-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (static calculation)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.1759},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.03518,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.03518},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.518,"value_printed":3.518,"value_stored":3.518},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"BA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Fcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-FH67ZBF6LL.3fa2fc","locator":{"ref":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1","row":10},"method":"first-principles (SQS)","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2006.03.096","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.jallcom.2006.03.096","paper_id":"doi:10.1016/j.jallcom.2006.03.096","phases":[{"label":"Fcc","model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.jallcom.2006.03.096/p2/tab-1/r10#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"confirmed_pro","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","source_system":"BA-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (static calculation)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.17565},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.03513,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.03513},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.513,"value_printed":3.513,"value_stored":3.513},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"END_MEMBER_FORMATION_ENERGY","before":"HM_FORM","evidence":{"printed":null},"field":"property","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}},{"after":"NI","before":"NI-TI","evidence":{"printed":null},"field":"system","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}},{"after":["NI"],"before":["NI","TI"],"evidence":{"printed":null},"field":"elements","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}},{"after":{"NI":1},"before":{"TI":0.25},"evidence":{"printed":null},"field":"overall_composition","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}},{"after":"page_checked_end_member_site_fractions","before":null,"evidence":{"printed":null},"field":"overall_composition_basis","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}},{"after":[{"label":"(Ni)3(Ni)1","parent_phase":"Ni3Ti","pearson_symbol":"hP16","structure_basis":"printed_source_page"}],"before":[{"label":"Ni3Ti"}],"evidence":{"printed":null},"field":"phases","gate":"page","rule":"end_member_not_nominal_compound","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"corrected"}}],"elements_stored":["NI","TI"],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"espei_ready_before_gates":true,"extraction_accepted":true,"gate_failures":["end_member_requires_sublattice_mapping"],"review_state":"extracted"},"fold_lpo":3,"fold_lso":1,"gate_failures":[{"code":"end_member_requires_sublattice_mapping","detail":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","effect":"not_espei_ready","gate":"page","visual_check":{"checked":"2026-10-25","image_sha256":"d2aa7d6d2e859b261d052a1684888fd7ecd317132549e4ef9d457856ce3f0fe1","page":4,"pdf_sha256_prefix":"ee2f0144eb04347f","seen":"Table 5 prints end-member sublattice occupancies; vacancies are excluded when computing atomic fractions. Parent phase label is not the end-member composition.","verdict":"confirmed"}}],"id":"ORC-LXX4NRREAG","locator":{"ref":"doi:10.1016/j.jallcom.2014.08.200/p4/tab-5","row":10},"method":"first-principle","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2014.08.200","own_work_of_paper":true},"overall_composition":{"NI":1},"overall_composition_basis":"page_checked_end_member_site_fractions","overall_composition_basis_stored":null,"overall_composition_stored":{"TI":0.25},"paper":"doi:10.1016/j.jallcom.2014.08.200","paper_id":"doi:10.1016/j.jallcom.2014.08.200","phases":[{"label":"(Ni)3(Ni)1","parent_phase":"Ni3Ti","pearson_symbol":"hP16","structure_basis":"printed_source_page"}],"phases_stored":[{"label":"Ni3Ti"}],"pid":"doi:10.1016/j.jallcom.2014.08.200/p4/tab-5/r10#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"END_MEMBER_FORMATION_ENERGY","property_code_before_gates":"HM_FORM","property_group":"formation","property_printed":"ΔEf","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"FCC_A1"}},"reference_state_stored":{"NI":{"phase":"FCC_A1"},"TI":{"phase":"HCP_A3"}},"source_system":"NI","system":"NI","system_stored":"NI-TI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (the quantity is defined at 0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.354},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property END_MEMBER_FORMATION_ENERGY","sigma_method":{"reason":"no method floor defined for property END_MEMBER_FORMATION_ENERGY","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"caption","unit_printed":"kJ/mol-atom","unit_stored":"J/mol-atom","value":7.08,"value_printed":7.08,"value_stored":7080.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"CR-NI-V","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0,"V":0.0},"phases":["sigma"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["reference-dependent quantity without a resolved reference state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"id":"ORC-D4Y3NAPN56","locator":{"ref":"doi:10.1016/j.jallcom.2024.174011/p5/tab-4","row":14},"method":"DFT","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.jallcom.2024.174011","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NI":1.0,"V":0.0},"paper":"doi:10.1016/j.jallcom.2024.174011","paper_id":"doi:10.1016/j.jallcom.2024.174011","phases":[{"label":"sigma","model_phase":"SIGMA"}],"pid":"doi:10.1016/j.jallcom.2024.174011/p5/tab-4/r14#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔHf","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"printed:pure elements bcc Cr, fcc Ni and bcc V (ferromagnetic spin-polarization for Cr and Ni)"}},"reference_state_stored":{"CR":{"phase":"printed:pure elements bcc Cr, fcc Ni and bcc V (ferromagnetic spin-polarization for Cr and Ni)"},"NI":{"phase":"printed:pure elements bcc Cr, fcc Ni and bcc V (ferromagnetic spin-polarization for Cr and Ni)"},"V":{"phase":"printed:pure elements bcc Cr, fcc Ni and bcc V (ferromagnetic spin-polarization for Cr and Ni)"}},"source_system":"CR-NI-V","system":"NI","temperature_K":0.0,"temperature_basis":"printed","temperature_printed":"0 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.49215},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"column_header","unit_printed":"kJ/mol-atom","unit_stored":"J/mol-atom","value":9.843,"value_printed":9.843,"value_stored":9843.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/j.scriptamat.2004.09.007","first_author":"Wang","kind":"unknown","label":"13","paper":"doi:10.1016/j.scriptamat.2004.09.007","reference":"Y. Wang, C. Woodward, S.H. Zhou, Z.K. Liu, L.Q. Chen, Scripta Mater. 52 (2005) 17–20.","status":"resolved","year":"2005"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"corrections":[{"after":"NI","before":"MO-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:computation_context"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-5EBBIE7IWM.335297","locator":{"ref":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","row":24},"method":"first-principles","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"computed","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.msea.2005.02.037","paper_id":"doi:10.1016/j.msea.2005.02.037","phases":[{"label":"Ni"}],"pid":"doi:10.1016/j.msea.2005.02.037/p4/tab-2/r24#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"MO":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"MO-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (the quantity is defined at 0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"column_header","unit_printed":"kJ/mol","unit_stored":"J/mol (basis unstated)","value":0.0,"value_printed":0.0,"value_stored":0.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/j.scriptamat.2004.09.007","first_author":"Wang","kind":"unknown","label":"13","paper":"doi:10.1016/j.scriptamat.2004.09.007","reference":"Y. Wang, C. Woodward, S.H. Zhou, Z.K. Liu, L.Q. Chen, Scripta Mater. 52 (2005) 17–20.","status":"resolved","year":"2005"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"corrections":[{"after":"NI","before":"MO-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["UNKNOWN"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":[{"label":"Ni","label_source":"printed_source_page"}],"before":[{"label":"UNKNOWN"}],"evidence":{"doi":"10.1016/j.msea.2005.02.037","locator":{"artifact":"table","asset":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","caption":"First-principles calculation results","label":"2","page":4,"row":24},"pdf_page":4,"pdf_sha256":"846e8e90422f237b93fdb32fb9dd1ccc44ec7593f6c489793994099a21b4a2a4","printed_phase_text":"Ni","rationale":"Table 2 phase column read independently of formula/site-occupancy column. Ni3Mo endmember configurations retained under the printed phase group, without treating endmember formula as phase name. Structure distinctions require downstream revalidation.","rendered_page_sha256":"058cb921f3a445904f9f9fb6b3652727291374dbf0623c5664d96e149ec1a3c8","report_id":"ORCHID-PR-20261027-v1","review_group":39,"table":"2"},"field":"phases","gate":"PR20261027","rule":"source_adjudicated_placeholder_recovery","visual_check":{"checked":"2026-10-27; Codex rendered-page inspection","image_sha256":"058cb921f3a445904f9f9fb6b3652727291374dbf0623c5664d96e149ec1a3c8","method":"Explicit printed row or bounded table group; no composition or diagram inference","page":4,"pdf_sha256_prefix":"846e8e90422f237b","seen":"Ni","verdict":"confirmed"}},{"after":null,"before":"state_phases_missing","evidence":{"basis":"phases recovered on the printed page","evidence_id":"ORCHID-PR-20261027-v1"},"field":"gate_failures","gate":"PR20261027","rule":"placeholder_recovery_lifts_state_phases_missing"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["human_review_residual_concern"],"review_state":"extracted","specification_gaps":["state:T_K","state:computation_context","temperature not stated","placeholder_recovery_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"human_review_residual_concern","detail":"Phase labels only. Preserve all original scientific and state qualifications; downstream gates and ESPEI revalidation required. Table 2 phase column read independently of formula/site-occupancy column. Ni3Mo endmember configurations retained under the printed phase group, without treating endmember formula as phase name. Structure distinctions require downstream revalidation.","effect":"not_espei_ready","gate":"PR20261027"}],"id":"ORC-5EBBIE7IWM.d0ecfd","locator":{"ref":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","row":24},"method":"first-principles","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"computed","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.msea.2005.02.037","paper_id":"doi:10.1016/j.msea.2005.02.037","phases":[{"label":"Ni","label_source":"printed_source_page"}],"pid":"doi:10.1016/j.msea.2005.02.037/p4/tab-2/r24#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"MO":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"MO-NI","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.5},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"column_header","unit_printed":"kJ/mol","unit_stored":"J/mol (basis unstated)","value":0.0,"value_printed":0,"value_stored":0.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"MO-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["UNKNOWN"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":[{"label":"Ni","label_source":"printed_source_page"}],"before":[{"label":"UNKNOWN"}],"evidence":{"doi":"10.1016/j.msea.2005.02.037","locator":{"artifact":"table","asset":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","caption":"First-principles calculation results","label":"2","page":4,"row":25},"pdf_page":4,"pdf_sha256":"846e8e90422f237b93fdb32fb9dd1ccc44ec7593f6c489793994099a21b4a2a4","printed_phase_text":"Ni","rationale":"Table 2 phase column read independently of formula/site-occupancy column. Ni3Mo endmember configurations retained under the printed phase group, without treating endmember formula as phase name. Structure distinctions require downstream revalidation.","rendered_page_sha256":"058cb921f3a445904f9f9fb6b3652727291374dbf0623c5664d96e149ec1a3c8","report_id":"ORCHID-PR-20261027-v1","review_group":39,"table":"2"},"field":"phases","gate":"PR20261027","rule":"source_adjudicated_placeholder_recovery","visual_check":{"checked":"2026-10-27; Codex rendered-page inspection","image_sha256":"058cb921f3a445904f9f9fb6b3652727291374dbf0623c5664d96e149ec1a3c8","method":"Explicit printed row or bounded table group; no composition or diagram inference","page":4,"pdf_sha256_prefix":"846e8e90422f237b","seen":"Ni","verdict":"confirmed"}},{"after":null,"before":"state_phases_missing","evidence":{"basis":"phases recovered on the printed page","evidence_id":"ORCHID-PR-20261027-v1"},"field":"gate_failures","gate":"PR20261027","rule":"placeholder_recovery_lifts_state_phases_missing"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["human_review_residual_concern"],"review_state":"extracted","specification_gaps":["state:T_K","state:computation_context","temperature not stated","placeholder_recovery_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"gate_failures":[{"code":"human_review_residual_concern","detail":"Phase labels only. Preserve all original scientific and state qualifications; downstream gates and ESPEI revalidation required. Table 2 phase column read independently of formula/site-occupancy column. Ni3Mo endmember configurations retained under the printed phase group, without treating endmember formula as phase name. Structure distinctions require downstream revalidation.","effect":"not_espei_ready","gate":"PR20261027"}],"id":"ORC-IL45GRAGXF.753057","locator":{"ref":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","row":25},"method":"first-principles","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.msea.2005.02.037","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.msea.2005.02.037","paper_id":"doi:10.1016/j.msea.2005.02.037","phases":[{"label":"Ni","label_source":"printed_source_page"}],"pid":"doi:10.1016/j.msea.2005.02.037/p4/tab-2/r25#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"MO":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"MO-NI","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.4665},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"column_header","unit_printed":"kJ/mol","unit_stored":"J/mol (basis unstated)","value":9.33,"value_printed":9.33,"value_stored":9330.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"MO-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:computation_context"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-IL45GRAGXF.f4a144","locator":{"ref":"doi:10.1016/j.msea.2005.02.037/p4/tab-2","row":25},"method":"first-principles","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.msea.2005.02.037","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.msea.2005.02.037","paper_id":"doi:10.1016/j.msea.2005.02.037","phases":[{"label":"Ni"}],"pid":"doi:10.1016/j.msea.2005.02.037/p4/tab-2/r25#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"MO":{"fixed_state_variables":{"T":298.15},"phase":"BCC_A2"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"MO-NI","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"0 K (the quantity is defined at 0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.4665},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"column_header","unit_printed":"kJ/mol","unit_stored":"J/mol (basis unstated)","value":9.33,"value_printed":9.33,"value_stored":9330.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"HF-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0},"phases":["Ni(fcc-A1)"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-NXB4QUUXWI.faa632","locator":{"ref":"doi:10.1016/j.tca.2018.08.011/p4/tab-1","row":1},"merged_ids":["ORC-NXB4QUUXWI.c457f5"],"model":"Mbcd30acd","observation_type":"equilibrium_property","origin":{"basis":"this_work+paper_text_states_calculated","class":"model_value","measured_in":"doi:10.1016/j.tca.2018.08.011","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.tca.2018.08.011","paper_id":"doi:10.1016/j.tca.2018.08.011","phases":[{"label":"Ni(fcc-A1)","label_variants":["Ni (fcc-A1)"],"model_phase":"FCC_A1"}],"pid":"doi:10.1016/j.tca.2018.08.011/p4/tab-1/r01#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"reference_state_stored":{"HF":{"fixed_state_variables":{"T":298.15},"phase":"HCP_A3"},"NI":{"fixed_state_variables":{"T":298.15},"phase":"FCC_A1"}},"source_system":"HF-NI","system":"NI","temperature_K":298.15,"temperature_basis":"printed","temperature_printed":"298.15 K","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.9,"sigma_method":{"basis":"calibrated","ci95":[3.11346,4.54664],"class":"model_calculated","entry":"model/HM_FORM","floor":3.9,"floor_unit":"kJ/mol-atom","n_pairs":2045,"value":3.9},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.5},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"printed_unit","unit_printed":"kJ/mole-atom","unit_stored":"J/mol-atom","value":0.0,"value_printed":0,"value_stored":0.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"CO-FE-NI-PT","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"FE":0.0,"NI":1.0,"PT":0.0},"phases":["fcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:T_K_explicit","temperature not stated"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-RTF7TN4GBQ","locator":{"ref":"sha256:01e2c117c65fb968/p2/tab-1","row":7},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"structural_property","origin":{"basis":"caption_names_calculation_only","class":"model_value","measured_in":"doi:10.1016/j.calphad.2011.04.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"FE":0.0,"NI":1.0,"PT":0.0},"paper":"doi:10.1016/j.calphad.2011.04.005","paper_id":"doi:10.1016/j.calphad.2011.04.005","phases":[{"label":"fcc"}],"pid":"sha256:01e2c117c65fb968/p2/tab-1/r07#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-FE-NI-PT","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02693,"sigma_method":{"basis":"calibrated","ci95":[0.005826,0.012707],"class":"model_calculated","entry":"model/LATTICE_LENGTH","floor":0.0077,"floor_unit":"relative (fraction of the value)","n_pairs":175,"value":0.02693},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"Å","value":3.498,"value_stored":3.498},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"CO-FE-NI-PT","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"FE":0.0,"NI":1.0,"PT":0.0},"phases":["fcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:T_K_explicit","temperature not stated"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-GS6IVXN2DL","locator":{"ref":"sha256:01e2c117c65fb968/p2/tab-1","row":8},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"structural_property","origin":{"basis":"caption_names_calculation_only","class":"model_value","measured_in":"doi:10.1016/j.calphad.2011.04.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"FE":0.0,"NI":1.0,"PT":0.0},"paper":"doi:10.1016/j.calphad.2011.04.005","paper_id":"doi:10.1016/j.calphad.2011.04.005","phases":[{"label":"fcc"}],"pid":"sha256:01e2c117c65fb968/p2/tab-1/r08#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-FE-NI-PT","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02708,"sigma_method":{"basis":"calibrated","ci95":[0.005826,0.012707],"class":"model_calculated","entry":"model/LATTICE_LENGTH","floor":0.0077,"floor_unit":"relative (fraction of the value)","n_pairs":175,"value":0.02708},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"Å","value":3.517,"value_stored":3.517},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"CO-FE-NI-PT","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"FE":0.0,"NI":1.0,"PT":0.0},"phases":["fcc"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:T_K_explicit","temperature not stated"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-F5WYALFFST","locator":{"ref":"sha256:01e2c117c65fb968/p2/tab-1","row":9},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"structural_property","origin":{"basis":"caption_names_calculation_only","class":"model_value","measured_in":"doi:10.1016/j.calphad.2011.04.005","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"FE":0.0,"NI":1.0,"PT":0.0},"paper":"doi:10.1016/j.calphad.2011.04.005","paper_id":"doi:10.1016/j.calphad.2011.04.005","phases":[{"label":"fcc"}],"pid":"sha256:01e2c117c65fb968/p2/tab-1/r09#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-FE-NI-PT","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02713,"sigma_method":{"basis":"calibrated","ci95":[0.005826,0.012707],"class":"model_calculated","entry":"model/LATTICE_LENGTH","floor":0.0077,"floor_unit":"relative (fraction of the value)","n_pairs":175,"value":0.02713},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"Å","value":3.523,"value_stored":3.523},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"component":"NI","conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["FCC_A1"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-5JLEG4GE3A.063f06","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":41},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"FCC_A1"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r41#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-06},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":0.0,"value_printed":0.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["FCC_A1"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-5JLEG4GE3A.1f45bb","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":41},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"FCC_A1"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r41#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-06},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.5},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":0.0,"value_printed":0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["BCC_A2"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-5VECLZ5PXN.cc693a","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":47},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"BCC_A2"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r47#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":38.332},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":-766.64,"value_printed":-766.64},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"component":"NI","conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["BCC_A2"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-5VECLZ5PXN.cfd90c","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":47},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"BCC_A2"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r47#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":38.332},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":-766.64,"value_printed":-766.64},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"component":"NI","conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["HCP_A3"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-BP4LLE3UCY.874543","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":53},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"HCP_A3"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r53#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-06},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":0.0,"value_printed":0.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["HCP_A3"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-BP4LLE3UCY.e2d33d","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":53},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"HCP_A3"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r53#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-06},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.5},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":0.0,"value_printed":0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["σ"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-WCTOB43OG6.0086b7","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":58},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"σ"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r58#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":4.022},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":-80.44,"value_printed":-80.44},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0364-5916(91)90030-n","first_author":"Dinsdale","kind":"assessment","label":"56","paper":"doi:10.1016/0364-5916(91)90030-n","reference":"A.T. Dinsdale, SGTE data for pure elements, Calphad, 1991, 15(4), p 317–425. https://doi.org/10.1016/0364-5916(91)90030-N 123 356","status":"resolved","year":"1991"}],"component":"NI","conditions":{"kind":"cited_source","note":"conditions in the cited source"},"contribution":"magnetic","corrections":[{"after":"GIBBS_ENERGY_CONTRIBUTION","before":"GIBBS_ENERGY","evidence":{"contribution":"magnetic","printed":"magΔG_i^φ/SER(0 K)"},"field":"property","gate":"R3","rule":"contribution_stored_as_total","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}},{"after":"NI","before":"CO-CR-NI-RE","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"CR":0.0,"NI":1.0,"RE":0.0},"phases":["σ"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["contribution_not_a_total"],"review_state":"extracted","specification_gaps":["state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"contribution_not_a_total","detail":"magnetic contribution to GIBBS_ENERGY","effect":"not_espei_ready","gate":"R3","visual_check":{"checked":"2026-10-24","image_sha256":"d01a371b8676dfdf1107378005b484f0e72817f4ad1f99bd518ed1a361edf968","page":3,"pdf_sha256_prefix":"94d8dcd509c0dfc5","seen":"S°298 (el.) is the electronic part of S298 (phonon part listed separately); Cp mag at 298.15 K is the magnetic contribution.","verdict":"rule_confirmed"}}],"id":"ORC-WCTOB43OG6.3a92fc","locator":{"ref":"sha256:1d912ff9ab64cea0/p8/tab-2","row":58},"model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"equilibrium_property","origin":{"basis":"printed_source_other_calculation","class":"model_value","measured_in":"doi:10.1016/0364-5916(91)90030-n","own_work_of_paper":false},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"CR":0.0,"NI":1.0,"RE":0.0},"paper":"doi:10.1007/s11669-023-01079-3","paper_id":"doi:10.1007/s11669-023-01079-3","phases":[{"label":"σ"}],"pid":"sha256:1d912ff9ab64cea0/p8/tab-2/r58#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"GIBBS_ENERGY_CONTRIBUTION","property_code_before_gates":"GIBBS_ENERGY","property_group":"activity / EMF / Gibbs energy","property_printed":"magΔG_i^φ/SER(0 K)","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CO-CR-NI-RE","system":"NI","temperature_K":0.0,"temperature_basis":"quantity_label","temperature_printed":"(0 K)","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":4.022},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":null,"sigma_effective_reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","sigma_method":{"reason":"no method floor defined for property GIBBS_ENERGY_CONTRIBUTION","value":null},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"J/mol","value_type":null}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"J/mol","unit_basis":"column_header","unit_printed":"J/mol","value":-80.44,"value_printed":-80.44},{"chemical_system":"NI","conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"H-LA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"LA":0.0,"NI":1.0},"phases":["Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-PBEQT7JZZK.484054","locator":{"ref":"sha256:66d905f81bb74d58/p5/tab-3","row":4},"merged_ids":["ORC-PBEQT7JZZK.4e772d"],"observation_type":"structural_property","origin":{"basis":"no_printed_or_resolvable_source_kind","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2012.12.002","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"LA":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2012.12.002","paper_id":"doi:10.1016/j.calphad.2012.12.002","phases":[{"label":"Ni"}],"pid":"sha256:66d905f81bb74d58/p5/tab-3/r04#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"H-LA-NI","structure":{"pearson_symbol":"cF4","prototype":"Cu"},"system":"NI","temperature_K":298.15,"temperature_basis":"assumed_room_temperature","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.007751,"sigma_method":{"basis":"calibrated","ci95":[0.001793,0.002549],"class":"unknown","entry":"value_types/LATTICE_LENGTH/classes/unknown","floor":0.0022,"floor_unit":"relative (fraction of the value)","n_pairs":586,"value":0.007751},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"nm","value":3.523,"value_stored":0.3523},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":{"NI":1.0},"before":null,"evidence":{"paper":"doi:10.1016/j.calphad.2008.10.003","pdf_page":3,"pdf_sha256":"7a34c631d852730b68b8fcf6f84ba41e6e4aa31379df5a1b500289337eaf4bfd","rationale":"The page-decided temperature fix requires filing the record under the elements present in its state; move to NI and apply the preserved proposed fields.","report_id":"ORCHID-Y10-20261027-v1","table_key":"t196"},"field":"overall_composition","gate":"CX20261028","rule":"source_adjudicated_independent_check","visual_check":{"checked":"2026-10-27; Codex rendered-page recheck at 200 dpi with OCR assistance; AI-assisted, not human re-review; ORCHID-Y10-20261027-v1","image_sha256":"a04aba19979645415f1bdee76d829b763b0e3b172db36eec966ef4abc1893f50","page":3,"pdf_sha256_prefix":"7a34c631d852730b","seen":"Table 1 Fe-Ni-Ti solid phases: Phase | Pearson/prototype/SG/Strukturbericht | Lattice parameters (nm) each prefixed by formula (Pure Fe, Fe50Ni50, ...) | Temperature range (°C) of stability ('<882', '<517', '<1380', '<984', ranges) | Composition range | Database model. Measurement T printed only for two γ rows: 'at room T' and 'at 900 °C'.","verdict":"confirmed"}},{"after":"from_formula","before":null,"evidence":{"paper":"doi:10.1016/j.calphad.2008.10.003","pdf_page":3,"pdf_sha256":"7a34c631d852730b68b8fcf6f84ba41e6e4aa31379df5a1b500289337eaf4bfd","rationale":"The page-decided temperature fix requires filing the record under the elements present in its state; move to NI and apply the preserved proposed fields.","report_id":"ORCHID-Y10-20261027-v1","table_key":"t196"},"field":"overall_composition_basis","gate":"CX20261028","rule":"source_adjudicated_independent_check","visual_check":{"checked":"2026-10-27; Codex rendered-page recheck at 200 dpi with OCR assistance; AI-assisted, not human re-review; ORCHID-Y10-20261027-v1","image_sha256":"a04aba19979645415f1bdee76d829b763b0e3b172db36eec966ef4abc1893f50","page":3,"pdf_sha256_prefix":"7a34c631d852730b","seen":"Table 1 Fe-Ni-Ti solid phases: Phase | Pearson/prototype/SG/Strukturbericht | Lattice parameters (nm) each prefixed by formula (Pure Fe, Fe50Ni50, ...) | Temperature range (°C) of stability ('<882', '<517', '<1380', '<984', ranges) | Composition range | Database model. Measurement T printed only for two γ rows: 'at room T' and 'at 900 °C'.","verdict":"confirmed"}},{"after":"NI","before":"FE-NI-TI","evidence":{"paper":"doi:10.1016/j.calphad.2008.10.003","pdf_page":3,"pdf_sha256":"7a34c631d852730b68b8fcf6f84ba41e6e4aa31379df5a1b500289337eaf4bfd","rationale":"The page-decided temperature fix requires filing the record under the elements present in its state; move to NI and apply the preserved proposed fields.","report_id":"ORCHID-Y10-20261027-v1","table_key":"t196"},"field":"system","gate":"CX20261028","rule":"source_adjudicated_independent_check","visual_check":{"checked":"2026-10-27; Codex rendered-page recheck at 200 dpi with OCR assistance; AI-assisted, not human re-review; ORCHID-Y10-20261027-v1","image_sha256":"a04aba19979645415f1bdee76d829b763b0e3b172db36eec966ef4abc1893f50","page":3,"pdf_sha256_prefix":"7a34c631d852730b","seen":"Table 1 Fe-Ni-Ti solid phases: Phase | Pearson/prototype/SG/Strukturbericht | Lattice parameters (nm) each prefixed by formula (Pure Fe, Fe50Ni50, ...) | Temperature range (°C) of stability ('<882', '<517', '<1380', '<984', ranges) | Composition range | Database model. Measurement T printed only for two γ rows: 'at room T' and 'at 900 °C'.","verdict":"confirmed"}},{"after":"NI","before":null,"evidence":{"paper":"doi:10.1016/j.calphad.2008.10.003","pdf_page":3,"pdf_sha256":"7a34c631d852730b68b8fcf6f84ba41e6e4aa31379df5a1b500289337eaf4bfd","rationale":"The page-decided temperature fix requires filing the record under the elements present in its state; move to NI and apply the preserved proposed fields.","report_id":"ORCHID-Y10-20261027-v1","table_key":"t196"},"field":"chemical_system","gate":"CX20261028","rule":"source_adjudicated_independent_check","visual_check":{"checked":"2026-10-27; Codex rendered-page recheck at 200 dpi with OCR assistance; AI-assisted, not human re-review; ORCHID-Y10-20261027-v1","image_sha256":"a04aba19979645415f1bdee76d829b763b0e3b172db36eec966ef4abc1893f50","page":3,"pdf_sha256_prefix":"7a34c631d852730b","seen":"Table 1 Fe-Ni-Ti solid phases: Phase | Pearson/prototype/SG/Strukturbericht | Lattice parameters (nm) each prefixed by formula (Pure Fe, Fe50Ni50, ...) | Temperature range (°C) of stability ('<882', '<517', '<1380', '<984', ranges) | Composition range | Database model. Measurement T printed only for two γ rows: 'at room T' and 'at 900 °C'.","verdict":"confirmed"}},{"after":["NI"],"before":["FE","NI","TI"],"evidence":{"paper":"doi:10.1016/j.calphad.2008.10.003","pdf_page":3,"pdf_sha256":"7a34c631d852730b68b8fcf6f84ba41e6e4aa31379df5a1b500289337eaf4bfd","rationale":"The page-decided temperature fix requires filing the record under the elements present in its state; move to NI and apply the preserved proposed fields.","report_id":"ORCHID-Y10-20261027-v1","table_key":"t196"},"field":"elements","gate":"CX20261028","rule":"source_adjudicated_independent_check","visual_check":{"checked":"2026-10-27; Codex rendered-page recheck at 200 dpi with OCR assistance; AI-assisted, not human re-review; ORCHID-Y10-20261027-v1","image_sha256":"a04aba19979645415f1bdee76d829b763b0e3b172db36eec966ef4abc1893f50","page":3,"pdf_sha256_prefix":"7a34c631d852730b","seen":"Table 1 Fe-Ni-Ti solid phases: Phase | Pearson/prototype/SG/Strukturbericht | Lattice parameters (nm) each prefixed by formula (Pure Fe, Fe50Ni50, ...) | Temperature range (°C) of stability ('<882', '<517', '<1380', '<984', ranges) | Composition range | Database model. Measurement T printed only for two γ rows: 'at room T' and 'at 900 °C'.","verdict":"confirmed"}}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["human_review_residual_concern"],"review_state":"extracted","specification_gaps":["state:composition","independent_check_correction_requires_downstream_revalidation"],"state_fully_specified":false},"fold_lpo":1,"fold_lso":1,"gate_failures":[{"code":"human_review_residual_concern","detail":"Prepared for 2026.10.1; requires exporter re-filing and full invariant tests.","effect":"not_espei_ready","gate":"CX20261028"}],"id":"ORC-L4SLJ36CHK.2d4c95","locator":{"ref":"sha256:7a34c631d852730b/p3/tab-1","row":1},"model_unlinked_reason":"linked TDB not the reporting paper's own model (link basis: None)","observation_type":"structural_property","origin":{"basis":"caption_names_calculation_only","class":"model_value","measured_in":"doi:10.1016/j.calphad.2008.10.003","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","paper":"doi:10.1016/j.calphad.2008.10.003","paper_id":"doi:10.1016/j.calphad.2008.10.003","phases":[{"label":"γ-(Fe, Ni)"}],"pid":"sha256:7a34c631d852730b/p3/tab-1/r01#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"FE-NI-TI","structure":{"pearson_symbol":"cF4","prototype":"Cu","strukturbericht":"A1"},"system":"NI","temperature_K":298.15,"temperature_basis":"assumed_room_temperature","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":5e-05},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.02713,"sigma_method":{"basis":"calibrated","ci95":[0.005826,0.012707],"class":"model_calculated","entry":"model/LATTICE_LENGTH","floor":0.0077,"floor_unit":"relative (fraction of the value)","n_pairs":175,"value":0.02713},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":5e-05},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"nm","value":3.5232,"value_stored":0.35232},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"HF-NI-SN","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0,"SN":0.0},"phases":["A1-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["reference-dependent quantity without a resolved reference state","state:reference_state"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-AHKQDN4OVJ.4a984b","locator":{"ref":"sha256:864a974ee9a34cd4/p4/tab-2","row":1},"merged_ids":["ORC-AHKQDN4OVJ.024caa"],"method":"DFT","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.commatsci.2016.08.042","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NI":1.0,"SN":0.0},"paper":"doi:10.1016/j.commatsci.2016.08.042","paper_id":"doi:10.1016/j.commatsci.2016.08.042","phases":[{"label":"A1-Ni"}],"pid":"sha256:864a974ee9a34cd4/p4/tab-2/r01#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔfH0K","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"printed:none"}},"reference_state_stored":{"HF":{"phase":"printed:none"},"NI":{"phase":"printed:none"},"SN":{"phase":"printed:none"}},"source_system":"HF-NI-SN","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"kJ/mol (basis unstated)","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol (basis unstated)","unit_basis":"unstated","unit_printed":"kJ/mol","unit_stored":"J/mol (basis unstated)","value":0.0,"value_printed":0.0,"value_stored":0.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"HF-NI-SN","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0,"SN":0.0},"phases":["A1-Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-MNXIWEI33D.0cda5d","locator":{"ref":"sha256:864a974ee9a34cd4/p4/tab-2","row":1},"merged_ids":["ORC-MNXIWEI33D.9a1152"],"method":"DFT","method_basis":"printed in the table row/column","observation_type":"structural_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.commatsci.2016.08.042","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NI":1.0,"SN":0.0},"paper":"doi:10.1016/j.commatsci.2016.08.042","paper_id":"doi:10.1016/j.commatsci.2016.08.042","phases":[{"label":"A1-Ni"}],"pid":"sha256:864a974ee9a34cd4/p4/tab-2/r01#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","property_printed":"a","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"HF-NI-SN","system":"NI","temperature_K":0.0,"temperature_basis":"printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.1758},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.03516,"sigma_method":{"basis":"prior","class":"dft","entry":"dft/priors/LATTICE_LENGTH","floor":0.01,"floor_unit":"relative (fraction of the value)","value":0.03516},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_printed":"Å","unit_stored":"Å","value":3.516,"value_printed":3.516,"value_stored":3.516},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"MO-NI-TA","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0,"TA":0.0},"phases":["UNKNOWN"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":[{"label":"Ni","label_source":"printed_source_page"}],"before":[{"label":"UNKNOWN"}],"evidence":{"doi":"10.1016/j.calphad.2009.06.006","locator":{"artifact":"table","asset":"sha256:bcd69fa868b68ab2/p7/tab-6","caption":"A summary of results from the first-principles calculations.","label":"6","page":7,"row":1},"pdf_page":7,"pdf_sha256":"bcd69fa868b68ab22bd990197ed0fb69ae0d0f46e9ebfaf301a954d2d11e745a","printed_phase_text":"Ni","rationale":"Table 6 elemental phase groups explicit; bcc/fcc lattice-stability distinctions remain to be revalidated, with no assumed stable structure.","rendered_page_sha256":"8689691bd7c2127b63e7f9e80e9a1a10b74135f5cd2ff9905dcc34ab487796c3","report_id":"ORCHID-PR-20261027-v1","review_group":87,"table":"6"},"field":"phases","gate":"PR20261027","rule":"source_adjudicated_placeholder_recovery","visual_check":{"checked":"2026-10-27; Codex rendered-page inspection","image_sha256":"8689691bd7c2127b63e7f9e80e9a1a10b74135f5cd2ff9905dcc34ab487796c3","method":"Explicit printed row or bounded table group; no composition or diagram inference","page":7,"pdf_sha256_prefix":"bcd69fa868b68ab2","seen":"Ni","verdict":"confirmed"}},{"after":null,"before":"state_phases_missing","evidence":{"basis":"phases recovered on the printed page","evidence_id":"ORCHID-PR-20261027-v1"},"field":"gate_failures","gate":"PR20261027","rule":"placeholder_recovery_lifts_state_phases_missing"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["human_review_residual_concern"],"review_state":"extracted","specification_gaps":["reference-dependent quantity without a resolved reference state","state:T_K","state:computation_context","state:reference_state","temperature not stated","placeholder_recovery_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"gate_failures":[{"code":"human_review_residual_concern","detail":"Phase labels only. Preserve all original scientific and state qualifications; downstream gates and ESPEI revalidation required. Table 6 elemental phase groups explicit; bcc/fcc lattice-stability distinctions remain to be revalidated, with no assumed stable structure.","effect":"not_espei_ready","gate":"PR20261027"}],"id":"ORC-Z5BP2ECH5W","locator":{"ref":"sha256:bcd69fa868b68ab2/p7/tab-6","row":1},"method":"first-principles calculations","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.calphad.2009.06.006","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NI":1.0,"TA":0.0},"paper":"doi:10.1016/j.calphad.2009.06.006","paper_id":"doi:10.1016/j.calphad.2009.06.006","phases":[{"label":"Ni","label_source":"printed_source_page"}],"pid":"sha256:bcd69fa868b68ab2/p7/tab-6/r01#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"printed:none"}},"reference_state_stored":{"MO":{"phase":"printed:none"},"NI":{"phase":"printed:none"},"TA":{"phase":"printed:none"}},"source_system":"MO-NI-TA","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":1e-09},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.5},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"reviewer","unit_printed":"kJ/mol","unit_stored":"J/mol-atom","value":0.0,"value_printed":0,"value_stored":0.0},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"MO-NI-TA","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"NI":1.0,"TA":0.0},"phases":["UNKNOWN"]},"field":"system","gate":"A1","rule":"system_of_the_state"},{"after":[{"label":"Ni","label_source":"printed_source_page"}],"before":[{"label":"UNKNOWN"}],"evidence":{"doi":"10.1016/j.calphad.2009.06.006","locator":{"artifact":"table","asset":"sha256:bcd69fa868b68ab2/p7/tab-6","caption":"A summary of results from the first-principles calculations.","label":"6","page":7,"row":2},"pdf_page":7,"pdf_sha256":"bcd69fa868b68ab22bd990197ed0fb69ae0d0f46e9ebfaf301a954d2d11e745a","printed_phase_text":"Ni","rationale":"Table 6 elemental phase groups explicit; bcc/fcc lattice-stability distinctions remain to be revalidated, with no assumed stable structure.","rendered_page_sha256":"8689691bd7c2127b63e7f9e80e9a1a10b74135f5cd2ff9905dcc34ab487796c3","report_id":"ORCHID-PR-20261027-v1","review_group":87,"table":"6"},"field":"phases","gate":"PR20261027","rule":"source_adjudicated_placeholder_recovery","visual_check":{"checked":"2026-10-27; Codex rendered-page inspection","image_sha256":"8689691bd7c2127b63e7f9e80e9a1a10b74135f5cd2ff9905dcc34ab487796c3","method":"Explicit printed row or bounded table group; no composition or diagram inference","page":7,"pdf_sha256_prefix":"bcd69fa868b68ab2","seen":"Ni","verdict":"confirmed"}},{"after":null,"before":"state_phases_missing","evidence":{"basis":"phases recovered on the printed page","evidence_id":"ORCHID-PR-20261027-v1"},"field":"gate_failures","gate":"PR20261027","rule":"placeholder_recovery_lifts_state_phases_missing"}],"evidence_class":"dft","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"gate_failures":["human_review_residual_concern"],"review_state":"extracted","specification_gaps":["reference-dependent quantity without a resolved reference state","state:T_K","state:computation_context","state:reference_state","temperature not stated","placeholder_recovery_requires_downstream_revalidation"],"state_fully_specified":false,"system_is_state_subsystem":true},"fold_lpo":3,"fold_lso":1,"gate_failures":[{"code":"human_review_residual_concern","detail":"Phase labels only. Preserve all original scientific and state qualifications; downstream gates and ESPEI revalidation required. Table 6 elemental phase groups explicit; bcc/fcc lattice-stability distinctions remain to be revalidated, with no assumed stable structure.","effect":"not_espei_ready","gate":"PR20261027"}],"id":"ORC-TW47OPDAEX","locator":{"ref":"sha256:bcd69fa868b68ab2/p7/tab-6","row":2},"method":"first-principles calculations","method_basis":"printed in the table row/column","observation_type":"equilibrium_property","origin":{"basis":"this_work+label_first_principles","class":"computed","measured_in":"doi:10.1016/j.calphad.2009.06.006","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"NI":1.0,"TA":0.0},"paper":"doi:10.1016/j.calphad.2009.06.006","paper_id":"doi:10.1016/j.calphad.2009.06.006","phases":[{"label":"Ni","label_source":"printed_source_page"}],"pid":"sha256:bcd69fa868b68ab2/p7/tab-6/r02#equilibrium_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"HM_FORM","property_group":"formation","property_printed":"ΔH","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","reference_state":{"NI":{"phase":"printed:none"}},"reference_state_stored":{"MO":{"phase":"printed:none"},"NI":{"phase":"printed:none"},"TA":{"phase":"printed:none"}},"source_system":"MO-NI-TA","system":"NI","temperature_basis":"not_printed","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"stated_default","note":"5% default","value":0.4665},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":3.929,"sigma_method":{"basis":"calibrated","ci95":[2.742,4.87],"class":"dft","entry":"dft/literature/strata/magnetic_3d","floor":3.929,"floor_unit":"kJ/mol-atom","n_pairs":105,"stratum":"literature/magnetic_3d","value":3.929},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"kJ/mol-atom","value_type":"HM_FORM"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"kJ/mol-atom","unit_basis":"reviewer","unit_printed":"kJ/mol","unit_stored":"J/mol-atom","value":9.33,"value_printed":9.33,"value_stored":9330.0},{"chemical_system":"NI","conditions":{"kind":"own_work_origin_unspecified"},"corrections":[{"after":"NI","before":"CU-LA-NI","evidence":{"basis":"overall_composition_all_elements","overall_composition":{"LA":0.0,"NI":1.0},"phases":["Ni"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"unspecified","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","system_is_state_subsystem":true},"fold_lpo":4,"fold_lso":1,"id":"ORC-OZI6YJRPV3","locator":{"ref":"sha256:d74c2ece3dfbcad3/p5/tab-2","row":4},"observation_type":"structural_property","origin":{"basis":"no_printed_or_resolvable_source_kind","class":"unspecified","measured_in":"doi:10.1016/j.calphad.2011.10.004","own_work_of_paper":true},"overall_composition":{"NI":1.0},"overall_composition_basis":"from_formula","overall_composition_stored":{"LA":0.0,"NI":1.0},"paper":"doi:10.1016/j.calphad.2011.10.004","paper_id":"doi:10.1016/j.calphad.2011.10.004","phases":[{"label":"Ni"}],"pid":"sha256:d74c2ece3dfbcad3/p5/tab-2/r04#structural_property","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"LATTICE_A","property_group":"crystal structure","reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.1-pro-preview","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"CU-LA-NI","structure":{"pearson_symbol":"cF4","prototype":"Cu"},"system":"NI","temperature_K":298.15,"temperature_basis":"assumed_room_temperature","tool_release":"tools-release-v2.1.18","uncertainty":{"basis":"reading_resolution","value":0.0005},"uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.007751,"sigma_method":{"basis":"calibrated","ci95":[0.001793,0.002549],"class":"unknown","entry":"value_types/LATTICE_LENGTH/classes/unknown","floor":0.0022,"floor_unit":"relative (fraction of the value)","n_pairs":586,"value":0.007751},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.0005},"sigma_scatter":null,"unit":"Å","value_type":"LATTICE_LENGTH"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"Å","unit_stored":"nm","value":3.523,"value_stored":0.3523},{"chemical_system":"NI","cited_sources":[{"doi":"10.1016/0022-3697(81)90174-8","first_author":"Meschter","kind":"unknown","label":"112","paper":"doi:10.1016/0022-3697(81)90174-8","reference":"P.J. Meschter, J.W. Wright, C.R. Brooks, T.G. Kollie, Physical contributions to the heat capacity of nickel, J. Phys. Chem. Solids. 42 (1981) 861–871. https://doi.org/10.1016/0022-3697(81)90174-8.","status":"resolved","year":"1981"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-57DYGTGRGN","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":1},"method":"Heat capacity measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r01#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":633.0,"temperature_basis":"printed","temperature_printed":"633","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":633.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1098/rspa.1963.0045","first_author":"Crangle","kind":"unknown","label":"114","paper":"doi:10.1098/rspa.1963.0045","reference":"J. Crangle, G.C. Hallam, The magnetization of face-centred cubic and body-centred cubic iron + nickel alloys, Proc. R. Soc. Lond. A. 272 (1963) 119–132. https://doi.org/10.1098/rspa.1963.0045.","status":"resolved","year":"1963"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-2R4A5ZQIO2","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":2},"method":"Magnetization measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r02#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":633.0,"temperature_basis":"printed","temperature_printed":"633","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":633.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1103/physrev.136.a1626","first_author":"Kouvel","kind":"unknown","label":"115","paper":"doi:10.1103/physrev.136.a1626","reference":"J.S. Kouvel, M.E. Fisher, Detailed magnetic behavior of nickel near its curie point, Phys. Rev. 136 (1964). https://doi.org/10.1103/PhysRev.136.A1626.","status":"resolved","year":"1964"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-MVFAEERPRS","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":3},"method":"Susceptibility measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r03#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":627.2,"temperature_basis":"printed","temperature_printed":"627.2","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":16.0,"sigma_method":{"basis":"calibrated","ci95":[10.483565,26.208913],"class":"dilatometry_resistivity","entry":"value_types/T_TRANSITION/classes/unknown","floor":16.0,"floor_unit":"K","n_pairs":274,"value":16.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":627.2},{"chemical_system":"NI","cited_sources":[{"doi":"10.1143/jpsj.50.454","first_author":"Tange","kind":"unknown","label":"116","paper":"doi:10.1143/jpsj.50.454","reference":"H. Tange, T. Yonei, M. Goto, Forced volume magnetostriction of Ni-Cr alloys, J. Phys. Soc. Japan. 50 (1981) 454–460. https://doi.org/10.1143/JPSJ.50.454.","status":"resolved","year":"1981"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-XWI6IEROMF","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":4},"method":"Magnetization measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r04#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":631.0,"temperature_basis":"printed","temperature_printed":"631","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":631.0},{"chemical_system":"NI","cited_sources":[{"first_author":"Schmidt","kind":"unknown","label":"117","reference":"E.O. Schmidt, W. Leidenfrost, Adiabatic calorimeter for measurements of specific heats of powders and granular materials at 0 C to 500 C, in: Prog. Int. Res. Thermodyn. Transp. Prop., 1962: pp. 178–184. https://doi.org/10.1016/B978-1-4832-0083-5.50022-1.","status":"resolved","year":"1962"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-W6GSGJ4LKW","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":5},"method":"Heat capacity measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r05#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":628.5,"temperature_basis":"printed","temperature_printed":"628.5","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":628.5},{"chemical_system":"NI","cited_sources":[{"doi":"10.1002/pssa.2210470160","first_author":"Maszkiewicz","kind":"unknown","label":"118","paper":"doi:10.1002/pssa.2210470160","reference":"M. Maszkiewicz, Specific heat of high purity nickel single crystal near the critical temperature, Phys. Status Solidi. 47 (1978) 77–80. https://doi.org/10.1002/pssa.2210470160.","status":"resolved","year":"1978"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-TJVP3VVYDX","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":6},"method":"Heat capacity measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r06#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":625.25,"temperature_basis":"printed","temperature_printed":"625.25","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":625.25},{"chemical_system":"NI","cited_sources":[{"doi":"10.1080/14786443409462519","first_author":"Foster","kind":"unknown","label":"119","paper":"doi:10.1080/14786443409462519","reference":"A.W. Foster, XLIV. The temperature variation of the thermoelectric properties and the specific heat of nickel-chromium alloys, Philos. Mag. 18 (1934) 470–488. https://doi.org/10.1080/14786443409462519.","status":"resolved","year":"1934"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-5IKQDMMZNK","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":7},"method":"Thermoelectric measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r07#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":626.0,"temperature_basis":"printed","temperature_printed":"626","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"experimental_unspecified","entry":"value_types/T_TRANSITION/classes/experimental_unspecified","floor":10.0,"floor_unit":"K","n_pairs":0,"prior_source":"orchid_assumed","value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":626.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1103/physrevb.16.4872","first_author":"Kollie","kind":"unknown","label":"120","paper":"doi:10.1103/physrevb.16.4872","reference":"T.G. Kollie, Measurement of the thermal-expansion coefficient of nickel from 300 to 1000 K and determination of the power-law constants near the Curie temperature, Phys. Rev. B. 16 (1977) 4872–4881. https://doi.org/10.1103/PhysRevB.16.4872. 29","status":"resolved","year":"1977"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-3FN54UUSRZ","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":8},"method":"Thermal expansion measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r08#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":628.5,"temperature_basis":"printed","temperature_printed":"628.5","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":16.0,"sigma_method":{"basis":"calibrated","ci95":[10.483565,26.208913],"class":"dilatometry_resistivity","entry":"value_types/T_TRANSITION/classes/unknown","floor":16.0,"floor_unit":"K","n_pairs":274,"value":16.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":628.5},{"chemical_system":"NI","cited_sources":[{"first_author":"Shiga","kind":"assessment","label":"199","reference":"M. Shiga, G.P. Pells, The optical properties of nickel above and below the Curie temperature, J. Phys. C Solid State Phys. 2 (1969) 1847–1856. https://doi.org/10.1088/0022-3719/2/10/319. 36 Figure captions Figure 1. Comparison of the calculated heat capacities of bcc and liquid Cr in this work with experimental datapoints [48,54,55,67,70,90–98] and evaluation by handbooks [37,39]. Figure 2. Compar","status":"resolved","year":1969,"year_basis":"printed_parenthesised_year","year_read":"1856"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-LHHDTIDNQH","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":9},"method":"Optical absorption spectrum measurement","method_basis":"printed in the table row/column","observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r09#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":632.0,"temperature_basis":"printed","temperature_printed":"632","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":16.0,"sigma_method":{"basis":"calibrated","ci95":[10.483565,26.208913],"class":"metallography_microscopy","entry":"value_types/T_TRANSITION/classes/unknown","floor":16.0,"floor_unit":"K","n_pairs":274,"value":16.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":632.0},{"chemical_system":"NI","cited_sources":[{"doi":"10.1103/physrevb.77.054431","first_author":"Yu","kind":"unknown","label":"140","paper":"doi:10.1103/physrevb.77.054431","reference":"P. Yu, X.F. Jin, J. Kudrnovský, D.S. Wang, P. Bruno, Curie temperatures of fcc and bcc nickel and permalloy: Supercell and Green’s function methods, Phys. Rev. B. 77 (2008) 1–8. https://doi.org/10.1103/PhysRevB.77.054431.","status":"resolved","year":"2008"}],"conditions":{"kind":"cited_source","note":"conditions in the cited source"},"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","specification_gaps":["state:composition"],"state_fully_specified":false},"fold_lpo":2,"fold_lso":1,"id":"ORC-VRS6KWRF73","locator":{"ref":"sha256:fa1f9d709d911f4a/p42/tab-4","row":10},"method":"Renormalized random-phase approximation","method_basis":"printed in the table row/column","model_unlinked_reason":"reporting paper's own calculation, but no TDB linked to the table","observation_type":"phase_transition","origin":{"basis":"printed_source_other_calculation","class":"model_value","own_work_of_paper":false},"paper":"doi:10.1016/j.calphad.2021.102268","paper_id":"doi:10.1016/j.calphad.2021.102268","phases":[{"label":"magnetic"}],"pid":"sha256:fa1f9d709d911f4a/p42/tab-4/r10#phase_transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"unstated_assumed","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"TC, K","type":"magnetic"},"reader_agreement":"multi_reader","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash","text_layer"],"record_kind":"general_table","source_system":"NI","system":"NI","temperature_K":686.0,"temperature_basis":"printed","temperature_printed":"686","tool_release":"tools-release-v2.1.18","transition_kind":"magnetic","transition_kind_printed":"magnetic","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"model_calculated","entry":"model/T_TRANSITION","floor":10.0,"floor_unit":"K","n_pairs":129,"value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.05},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":686.0},{"chemical_system":"NI","conditions":{"kind":"paper_context_not_extracted","paper":"doi:10.1007/s10973-014-4189-1"},"corrections":[{"after":"NI","before":"HO-NI","evidence":{"basis":"every_phase_determined","overall_composition":null,"phases":["L","(fcc_A1)"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"experimental","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"settled","state_fully_specified":true,"system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-H2BOKWP7XA","locator":{"ref":"doi:10.1007/s10973-014-4189-1/p7/tab-6","row":29},"observation_type":"phase_transition","origin":{"basis":"printed_source_experimental","class":"experimental","measured_in":"doi:10.1007/s10973-014-4189-1","measured_in_basis":"no_citation_printed","own_work_of_paper":true},"paper":"doi:10.1007/s10973-014-4189-1","paper_id":"doi:10.1007/s10973-014-4189-1","phase_compositions":[{"basis":"mole_fraction","composition":{"NI":1.0},"composition_source":"printed","phase":"L"},{"basis":"mole_fraction","composition":{"NI":1.0},"composition_source":"printed","phase":"(fcc_A1)"}],"phases":[{"label":"L","mapping_confidence":"confirmed","model_phase":"LIQUID"},{"label":"(fcc_A1)","mapping_confidence":"confirmed","model_phase":"FCC_A1","pearson_symbol":"cF4","prototype":"Cu","structure_basis":"mapped_model_phase"}],"pid":"doi:10.1007/s10973-014-4189-1/p7/tab-6/r-unplaced-722a82fe#transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"stated_default_1_atm","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"L -> (fcc_A1)"},"reader_agreement":"multi_reader","reader_agreement_basis":"derived_from_readers","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"invariant_table","source_system":"HO-NI","system":"NI","temperature_K":1728.15,"temperature_printed":"1,455","temperature_uncertainty":{"basis":"stated_default","value":2.0},"tool_release":"v2.1.19n","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"composition":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.05,"sigma_method":{"basis":"calibrated","ci95":[0.010484,0.011532],"class":"unknown","entry":"value_types/X_PHASE/classes/unknown","floor":0.011,"floor_unit":"mole fraction","n_pairs":3014,"value":0.011},"sigma_printed":null,"sigma_reading":{"basis":"last_stored_digit","value":0.05},"sigma_scatter":null,"unit":"mole fraction","value_type":"X_PHASE"},"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":16.0,"sigma_method":{"basis":"calibrated","ci95":[10.483565,26.208913],"class":"unknown","entry":"value_types/T_TRANSITION/classes/unknown","floor":16.0,"floor_unit":"K","n_pairs":274,"value":16.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":1728.15},{"chemical_system":"NI","conditions":{"kind":"not_applicable_own_calculation"},"corrections":[{"after":"NI","before":"HO-NI","evidence":{"basis":"every_phase_determined","overall_composition":null,"phases":["L","(fcc_A1)"]},"field":"system","gate":"A1","rule":"system_of_the_state"}],"evidence_class":"model","flags":{"calphad_check":"not_available","espei_certified":false,"espei_ready":false,"extraction_accepted":true,"review_state":"extracted","row_state":"settled","state_fully_specified":true,"system_is_state_subsystem":true},"fold_lpo":2,"fold_lso":1,"id":"ORC-QGVIKVSSCY","locator":{"ref":"doi:10.1007/s10973-014-4189-1/p7/tab-6","row":30},"model":"M5e03aef9","observation_type":"phase_transition","origin":{"basis":"this_work+paper_text_states_calculated","class":"model_value","measured_in":"doi:10.1007/s10973-014-4189-1","measured_in_basis":"reporting_paper_own_value","own_work_of_paper":true},"paper":"doi:10.1007/s10973-014-4189-1","paper_id":"doi:10.1007/s10973-014-4189-1","phase_compositions":[{"basis":"mole_fraction","composition":{"NI":1.0},"composition_source":"printed","phase":"L"},{"basis":"mole_fraction","composition":{"NI":1.0},"composition_source":"printed","phase":"(fcc_A1)"}],"phases":[{"label":"L","mapping_confidence":"confirmed","model_phase":"LIQUID"},{"label":"(fcc_A1)","mapping_confidence":"confirmed","model_phase":"FCC_A1","pearson_symbol":"cF4","prototype":"Cu","structure_basis":"mapped_model_phase"}],"pid":"doi:10.1007/s10973-014-4189-1/p7/tab-6/r-unplaced-756737d1#transition","pressure_Pa":101325,"pressure_basis":"assumed_default_1_atm_not_printed","pressure_basis_stored":"stated_default_1_atm","property":"TRANSITION_TEMPERATURE","property_group":"phase transition","reaction":{"printed":"L -> (fcc_A1)"},"reader_agreement":"multi_reader","reader_agreement_basis":"derived_from_readers","reader_agreement_label":"confirmed (two or more readers)","reader_tier":"preliminary_flash+claude","readers":["claude-opus-5.5","gemini-3.8-flash"],"record_kind":"invariant_table","source_system":"HO-NI","system":"NI","temperature_K":1728.15,"temperature_printed":"1,455","temperature_uncertainty":{"basis":"stated_default","value":2.0},"tool_release":"v2.1.19n","uncertainty_budget":{"calibration":"orchid-uncertainty-calibration 2026-10-24 (audit round 2) sha256 6a2b5a92b0ec","quantities":{"composition":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":0.05,"sigma_method":{"basis":"calibrated","ci95":[0.004448,0.004448],"class":"model_calculated","entry":"model/X_PHASE","floor":0.005,"floor_unit":"mole fraction","n_pairs":16730,"value":0.005},"sigma_printed":null,"sigma_reading":{"basis":"last_stored_digit","value":0.05},"sigma_scatter":null,"unit":"mole fraction","value_type":"X_PHASE"},"value":{"sigma_composition":null,"sigma_conversion":null,"sigma_effective":10.0,"sigma_method":{"basis":"prior","ci95":null,"class":"model_calculated","entry":"model/T_TRANSITION","floor":10.0,"floor_unit":"K","n_pairs":129,"value":10.0},"sigma_printed":null,"sigma_reading":{"basis":"last_printed_digit","value":0.005},"sigma_scatter":null,"unit":"K","value_type":"T_TRANSITION"}},"sigma_rule":"max(sqrt(max(printed, reading, method)^2 + composition^2 + conversion^2), scatter)"},"unit":"K","value":1728.15}],"release":"orchid-literature 2026-10-23 (record store db-v2.1: invariant/general v2.1.19r, text+context fixup-20261022)","system":"NI"}