{"assessments":[{"data_papers_used":[],"doi":"10.1007/bf02868957","id":"doi:10.1007/bf02868957","key":"pd3082b78f138d0ef","n_data_papers_used":0,"n_values_from_cited_papers":0,"reassesses":[],"tdb_files":[],"title":"The Ge−Si (Germanium-Silicon) system","values_reported":72,"year":1984},{"data_papers_used":[],"doi":"10.1007/bf02667471","id":"doi:10.1007/bf02667471","key":"pb9f4935a946b161c","n_data_papers_used":0,"n_values_from_cited_papers":0,"reassesses":[],"tdb_files":[],"title":"Thermodynamic investigation on the si-ge binary system by calorimetry and knudsen cell mass spectrometry","values_reported":54,"year":1992},{"data_papers_used":[],"doi":"10.1016/j.intermet.2008.01.002","id":"doi:10.1016/j.intermet.2008.01.002","key":"p3083d83d912d8ec3","n_data_papers_used":0,"n_values_from_cited_papers":0,"reassesses":[],"tdb_files":[],"title":"Thermodynamic assessments of the V–Ge and V–Pt systems","values_reported":40,"year":2008},{"data_papers_used":[],"doi":"10.1007/s10973-012-2271-0","id":"doi:10.1007/s10973-012-2271-0","key":"p36adbca864f09830","n_data_papers_used":0,"n_values_from_cited_papers":0,"reassesses":[],"tdb_files":[],"title":"Thermodynamic optimization of the germanium–yttrium system","values_reported":62,"year":2012},{"data_papers_used":[{"doi":"10.1007/bf02868307","evidence_class":{"model":1,"unspecified":2},"id":"doi:10.1007/bf02868307","key":"p35aa9aa9229e7182","n_values":3,"n_values_accepted":3,"title":"Crystal structures of the elements at 25°C","year":1981}],"doi":"10.1016/j.calphad.2011.12.010","id":"doi:10.1016/j.calphad.2011.12.010","key":"pd8649a39e612f533","n_data_papers_used":1,"n_values_from_cited_papers":3,"reassesses":[],"tdb_files":[],"title":"Thermodynamic modeling of the Ge–Sc system supported by key experiments and first-principles calculation","values_reported":88,"year":2012},{"data_papers_used":[{"doi":"10.1007/s10973-012-2271-0","evidence_class":{"experimental":14},"id":"doi:10.1007/s10973-012-2271-0","key":"p36adbca864f09830","n_values":14,"n_values_accepted":14,"title":"Thermodynamic optimization of the germanium–yttrium system","year":2012}],"doi":"10.1007/s10973-017-6820-4","id":"doi:10.1007/s10973-017-6820-4","key":"p85226870c144825f","n_data_papers_used":1,"n_values_from_cited_papers":14,"reassesses":[],"tdb_files":[],"title":"Thermodynamic modeling of the thulium–germanium binary system","values_reported":62,"year":2017},{"data_papers_used":[{"doi":"10.1016/j.calphad.2004.08.005","evidence_class":{"model":17},"id":"doi:10.1016/j.calphad.2004.08.005","key":"p8b47537aa736ad97","n_values":17,"n_values_accepted":15,"title":"A new equation for the temperature dependence of the excess Gibbs energy of solution phases","year":2004},{"doi":"10.1016/j.calphad.2007.10.002","evidence_class":{"model":17},"id":"doi:10.1016/j.calphad.2007.10.002","key":"p59e1696c79aa9057","n_values":17,"n_values_accepted":15,"title":"A Calphad-compatible method to calculate liquid/liquid interfacial energies in immiscible metallic systems","year":2008},{"doi":"10.1021/ie50458a036","evidence_class":{"model":15},"id":"doi:10.1021/ie50458a036","key":"p09fe487bb06f56bd","n_values":15,"n_values_accepted":15,"title":"Algebraic Representation of Thermodynamic Properties and the Classification of Solutions","year":1948}],"doi":"10.1016/j.jallcom.2017.07.129","id":"doi:10.1016/j.jallcom.2017.07.129","key":"p193682682a921c72","n_data_papers_used":3,"n_values_from_cited_papers":49,"reassesses":[],"tdb_files":[],"title":"Thermodynamic optimization of the Erbium-Germanium binary system","values_reported":156,"year":2017},{"data_papers_used":[{"doi":"10.1021/j150537a011","evidence_class":{"experimental":5},"id":"doi:10.1021/j150537a011","key":"p0ec19079832f6338","n_values":5,"n_values_accepted":5,"title":"The Barium–Strontium Equilibrium System","year":1956},{"doi":"10.1063/1.1702202","evidence_class":{"experimental":3},"id":"doi:10.1063/1.1702202","key":"p388f692893ad3900","n_values":3,"n_values_accepted":3,"title":"Lattice Parameters, Coefficients of Thermal Expansion, and Atomic Weights of Purest Silicon and Germanium","year":1952}],"doi":"10.1007/s11669-019-00714-2","id":"doi:10.1007/s11669-019-00714-2","key":"pa9f27299150c5ffe","n_data_papers_used":2,"n_values_from_cited_papers":8,"reassesses":[],"tdb_files":[],"title":"Thermodynamic Modeling of the Al-Ba and Ba-Ge Systems Supported by First-Principles Calculations","values_reported":238,"year":2019},{"data_papers_used":[],"doi":"10.1007/s11664-022-09474-1","id":"doi:10.1007/s11664-022-09474-1","key":"p262984546e5d2a0d","n_data_papers_used":0,"n_values_from_cited_papers":0,"reassesses":[],"tdb_files":[],"title":"Thermodynamic Modeling of the Ge-X (X = As, Se, S, P) Systems","values_reported":132,"year":2022}],"cite_as":{"also_cite":["the papers themselves when you use their data (doi / citation of each bibliography record)"],"bibtex":"@misc{orchid_bibliography_2026,\n  author    = {Arr{\\'o}yave, Raymundo and Saal, James and Shin, Dongwon},\n  title     = {{ORCHID-Bibliography: papers and typed citation relations}},\n  version   = {2026.10},\n  publisher = {Zenodo},\n  year      = {2026},\n  doi       = {10.5281/zenodo.23736021},\n  url       = {https://doi.org/10.5281/zenodo.23736021},\n  note      = {Version 1, machine-extracted}\n}","dataset":"bibliography","doi":"10.5281/zenodo.23736021","licence_note":"Crossref bibliographic metadata: CC0; ORCHID-derived fields (roles, evidence counts, relations): CC BY 4.0","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: roles and evidence counts derive from machine-extracted literature values and link tables; bibliographic fields are Crossref metadata as deposited (DOIs matched from printed references checked against Crossref: doi_match; mismatches dropped).","text":"R. Arróyave, J. Saal, D. Shin, ORCHID-Bibliography: papers and typed citation relations (version 2026.10; Version 1, machine-extracted), Zenodo (2026). https://doi.org/10.5281/zenodo.23736021","title":"ORCHID-Bibliography: papers and typed citation relations","url":"https://doi.org/10.5281/zenodo.23736021","version":"2026.10"},"elements":["GE"],"papers":[{"doi":"10.1007/bf02667471","id":"doi:10.1007/bf02667471","key":"pb9f4935a946b161c","title":"Thermodynamic investigation on the si-ge binary system by calorimetry and knudsen cell mass spectrometry","year":1992},{"doi":"10.1007/bf02868307","id":"doi:10.1007/bf02868307","key":"p35aa9aa9229e7182","title":"Crystal structures of the elements at 25°C","year":1981},{"doi":"10.1007/bf02868957","id":"doi:10.1007/bf02868957","key":"pd3082b78f138d0ef","title":"The Ge−Si (Germanium-Silicon) system","year":1984},{"doi":"10.1007/s10973-012-2271-0","id":"doi:10.1007/s10973-012-2271-0","key":"p36adbca864f09830","title":"Thermodynamic optimization of the germanium–yttrium system","year":2012},{"doi":"10.1007/s10973-017-6820-4","id":"doi:10.1007/s10973-017-6820-4","key":"p85226870c144825f","title":"Thermodynamic modeling of the thulium–germanium binary system","year":2017},{"doi":"10.1007/s11664-022-09474-1","id":"doi:10.1007/s11664-022-09474-1","key":"p262984546e5d2a0d","title":"Thermodynamic Modeling of the Ge-X (X = As, Se, S, P) Systems","year":2022},{"doi":"10.1007/s11669-019-00714-2","id":"doi:10.1007/s11669-019-00714-2","key":"pa9f27299150c5ffe","title":"Thermodynamic Modeling of the Al-Ba and Ba-Ge Systems Supported by First-Principles Calculations","year":2019},{"doi":"10.1016/j.calphad.2004.08.005","id":"doi:10.1016/j.calphad.2004.08.005","key":"p8b47537aa736ad97","title":"A new equation for the temperature dependence of the excess Gibbs energy of solution phases","year":2004},{"doi":"10.1016/j.calphad.2007.10.002","id":"doi:10.1016/j.calphad.2007.10.002","key":"p59e1696c79aa9057","title":"A Calphad-compatible method to calculate liquid/liquid interfacial energies in immiscible metallic systems","year":2008},{"doi":"10.1016/j.calphad.2011.12.010","id":"doi:10.1016/j.calphad.2011.12.010","key":"pd8649a39e612f533","title":"Thermodynamic modeling of the Ge–Sc system supported by key experiments and first-principles calculation","year":2012},{"doi":"10.1016/j.intermet.2008.01.002","id":"doi:10.1016/j.intermet.2008.01.002","key":"p3083d83d912d8ec3","title":"Thermodynamic assessments of the V–Ge and V–Pt systems","year":2008},{"doi":"10.1016/j.jallcom.2017.07.129","id":"doi:10.1016/j.jallcom.2017.07.129","key":"p193682682a921c72","title":"Thermodynamic optimization of the Erbium-Germanium binary system","year":2017},{"doi":"10.1021/ie50458a036","id":"doi:10.1021/ie50458a036","key":"p09fe487bb06f56bd","title":"Algebraic Representation of Thermodynamic Properties and the Classification of Solutions","year":1948},{"doi":"10.1021/j150537a011","id":"doi:10.1021/j150537a011","key":"p0ec19079832f6338","title":"The Barium–Strontium Equilibrium System","year":1956},{"doi":"10.1063/1.1702202","id":"doi:10.1063/1.1702202","key":"p388f692893ad3900","title":"Lattice Parameters, Coefficients of Thermal Expansion, and Atomic Weights of Purest Silicon and Germanium","year":1952}],"papers_by_role":{"cited_original_source":["doi:10.1007/bf02868307","doi:10.1007/s10973-012-2271-0","doi:10.1016/j.calphad.2004.08.005","doi:10.1016/j.calphad.2007.10.002","doi:10.1016/j.intermet.2008.01.002","doi:10.1021/ie50458a036","doi:10.1021/j150537a011","doi:10.1063/1.1702202"],"corpus_assessment_read":["doi:10.1007/bf02667471","doi:10.1007/bf02868957","doi:10.1007/s10973-012-2271-0","doi:10.1007/s10973-017-6820-4","doi:10.1007/s11664-022-09474-1","doi:10.1007/s11669-019-00714-2","doi:10.1016/j.calphad.2011.12.010","doi:10.1016/j.intermet.2008.01.002","doi:10.1016/j.jallcom.2017.07.129"],"discovery_lead":["doi:10.1007/s11664-022-09474-1"],"handbook_diagram_source":["doi:10.1007/bf02667471","doi:10.1007/bf02868957","doi:10.1016/j.intermet.2008.01.002"],"tdb_source_assessment":["doi:10.1007/bf02667471","doi:10.1007/bf02868957","doi:10.1007/s10973-012-2271-0","doi:10.1007/s10973-017-6820-4","doi:10.1007/s11664-022-09474-1","doi:10.1007/s11669-019-00714-2","doi:10.1016/j.calphad.2011.12.010","doi:10.1016/j.intermet.2008.01.002","doi:10.1016/j.jallcom.2017.07.129"]},"system":"GE"}
