Co–Pt system

18 accepted literature values from 1 paper(s) (experimental 10, model 2, DFT 6); 3 calculated phase diagram(s). 1 further extracted value(s) not accepted by the reader-agreement checks are only in the JSON/CSV.

Data: JSON · CSV · interactive explorer · interactive phase diagram · phases (7) · papers (bibliography) · Markdown

Accepted values by evidence class
Evidence classValues
experimental10
model2
DFT6
Accepted values by property group
Property groupValues
phase transition3
formation3
mixing / partial1
crystal structure10
other property1

Calculated phase diagrams

Binary phase diagrams calculated with pycalphad 0.11.2 from the SGTE binary collection (Hallstedt 2025, CC BY 4.0). Evidence class: model.

Assessments with a calculated phase diagram
TDB fileAssessmentSHA-256Links
CoPt-01Oik.tdbK. Oikawa, G.W. Qin, T. Ikeshoji, O. Kitakami, Y. Shimada, K. Ishida, K. Fukamichi, J. Magn. Magn. Mater., 236, 220-33(2001). doi:10.1016/S0304-8853(00)00520-5adf708dbafc5b2c33e1c38c29470eecad45f99bc0f546e31c1dc5b079e13b2bdviewer · TDB · JSON
CoPt-11Kim.tdbD. Kim, J.E. Saal, L. Zhou, S. Shang, Y. Du, Z.-K. Liu, Calphad, 35, 323-30(2011). doi:10.1016/j.calphad.2011.04.005335cf2628217f37fe82d25ddcd19a8fc5d7d507ef2e61b63faf15962523eced6viewer · TDB · JSON
CoPt-90Spe-LB.tdbP.J. Spencer, unpublished, 1990.8a9bf4d4f4636b8994e37943ba8aff05c80e6d02794f1c610e7343ae0dee89c6viewer · TDB · JSON
Calculated three-phase invariants (model, mole fraction of the second component)
TDB fileT (K)Phases at the invariant
CoPt-11Kim.tdb962.79FCC_4SL (x(Pt) 0.57621) + FCC_4SL#2 (x(Pt) 0.61122) + FCC_4SL#3 (x(Pt) 0.6201)
CoPt-11Kim.tdb962.79FCC_4SL (x(Pt) 0.57621) + FCC_A1 (x(Pt) 0.61122) + FCC_4SL#2 (x(Pt) 0.6201)
CoPt-11Kim.tdb652.1HCP_A3 (x(Pt) 0.15243) + FCC_A1 (x(Pt) 0.16793) + FCC_4SL (x(Pt) 0.22638)
CoPt-11Kim.tdb652.1HCP_A3 (x(Pt) 0.15243) + FCC_4SL#2 (x(Pt) 0.16793) + FCC_4SL (x(Pt) 0.22638)
CoPt-90Spe-LB.tdb673.57HCP_A3 (x(Pt) 0.36339) + FCC_A1 (x(Pt) 0.37848) + COPT_L10 (x(Pt) 0.39722)
CoPt-90Spe-LB.tdb446.9COPT_L10 (x(Pt) 0.63247) + FCC_A1 (x(Pt) 0.65973) + COPT3_L12 (x(Pt) 0.69701)

Convex hulls: Materials Project DFT hull · OQMD DFT hull · CALPHAD hull CoPt-01Oik · CALPHAD hull CoPt-90Spe-LB

Formation enthalpies

Literature values in kJ/mol-atom where the per-atom basis is known. DFT columns: the lowest-energy entry at the same composition (Materials Project 2026.04.13, OQMD v1.8; different energy references, never averaged), from dft_parity.json.

Enthalpies of formation, Co–Pt system (3)
PhaseCompoundValueT (K)ClassMP DFT (kJ/mol-atom)OQMD DFT (kJ/mol-atom)SourceLocationQuote
CoPt-13.6 per mol-atom ± 0.7914experimental[1] Kim 2011
cites Oriani 1962 doi
Table 2, p. 3, row 16
report
CoPt-12.265 kJ/mol-atom914DFT[1] Kim 2011Table 2, p. 3, row 15
report
CoPt3-12.8 per mol-atom ± 1.63914experimental[1] Kim 2011
cites Oriani 1962 doi
Table 2, p. 3, row 16
report

Other properties

Phase transition (3)

Phase transition, Co–Pt system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Phase transition822 K822Co3Ptmodel[1] Kim 2011p. 5
report
Co3 Pt is predicted to be stable up to about 822 K.
Phase transition840 K840congruent transformationexperimental[1] Kim 2011
cites Inden 1983
p. 5
report
This behavior is similar to that measured by Inden [25] with a congruent temperature of approximately 840 K.
Phase transition1104 K1104otherexperimental[1] Kim 2011p. 6
report
The calculated LRO parameter for L10 according to Eq. (12) is plotted in Fig. 9 along with the experimental data [24] with the temperature normalized by the order/disorder transition temperature of the L10 CoPt phase of 1104 K, showing a good agreement.

Mixing / partial (1)

Mixing / partial, Co–Pt system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Enthalpy of mixing
printed: ΔHmix
-8.651 kJ/mol-atom300Co3Pt
alloy: Pt 0.25
DFT[1] Kim 2011Table 2, p. 3, row 17
report

Crystal structure (10)

Crystal structure, Co–Pt system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Lattice a
printed: a
3.654 ÅCo3Pt
alloy: Pt 0.25
DFT[1] Kim 2011Table 2, p. 3, row 1
report
Lattice a
printed: a
3.664 ÅCo3Pt
alloy: Pt 0.25
experimental[1] Kim 2011
cites Capitan 1999 doi
Table 2, p. 3, row 2
report
Lattice a
printed: a
3.806 ÅCoPt
alloy: Pt 0.5
experimental[1] Kim 2011
cites Galanakis 2000 doi
Table 2, p. 3, row 3
report
Lattice a
printed: a
3.809 ÅCoPt
alloy: Pt 0.5
DFT[1] Kim 2011Table 2, p. 3, row 1
report
Lattice a
printed: a
3.811 ÅCoPt
alloy: Pt 0.5
experimental[1] Kim 2011
cites Capitan 1999 doi
Table 2, p. 3, row 2
report
Lattice a
printed: a
3.885 ÅCoPt3
alloy: Pt 0.75
DFT[1] Kim 2011Table 2, p. 3, row 1
report
Lattice a
printed: a
3.857 ÅCoPt3
alloy: Pt 0.75
experimental[1] Kim 2011
cites Capitan 1999 doi
Table 2, p. 3, row 2
report
Lattice c
printed: c
3.708 ÅCoPt
alloy: Pt 0.5
DFT[1] Kim 2011Table 2, p. 3, row 4
report
Lattice c
printed: c
3.684 ÅCoPt
alloy: Pt 0.5
experimental[1] Kim 2011
cites Galanakis 2000 doi
Table 2, p. 3, row 6
report
Lattice c
printed: c
3.694 ÅCoPt
alloy: Pt 0.5
experimental[1] Kim 2011
cites Leroux 1988
Table 2, p. 3, row 5
report

Other property (1)

Other property, Co–Pt system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Other
printed: enthalpy of transformation
-3.303 kJ/mol-atom783L10 + fccmodel[1] Kim 2011p. 5
report
The calculated enthalpy for the disordered fcc phase to L10 transformation in CoPt compound at 783 K from the current modeling is -3.303 kJ/mol-atom which is also in a good agreement with the experimental data (-3.1 ± 0.2 kJ/mol-atom) in the literature [16].

Sources

Reporting papers the values were read from (a value cited from another work names that work in its row).

  1. 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). doi:10.1016/j.calphad.2011.04.005