P–Si system

69 accepted literature values from 3 paper(s) (experimental 33, model 27, unspecified 9); 0 calculated phase diagram(s). 12 further extracted value(s) not accepted by the reader-agreement checks are only in the JSON/CSV.

Data: JSON · CSV · interactive explorer · phases (10) · papers (bibliography) · Markdown

Accepted values by evidence class
Evidence classValues
experimental33
model27
unspecified9
Accepted values by property group
Property groupValues
invariant reaction20
phase transition4
phase equilibrium7
formation14
heat capacity / entropy / enthalpy12
activity / EMF / Gibbs energy5
crystal structure6
model expression1

Convex hulls: Materials Project DFT hull · OQMD DFT hull · CALPHAD hull SiP-04Din-LB · CALPHAD hull SiP-14Lia · CALPHAD hull SiP-21Don

Invariant reactions (literature)

Invariant reactions reported in the literature for the P–Si system (20)
T (K)Reaction / phasesCompositions (mole fraction)ClassSourceLocationQuote
1451.15other: Congruent melting L = SiP2L: P 0.666667, Si 0.333333; SiP2: P 0.666667, Si 0.333333experimental[1] Liang 2014
cites Ugai 1987
Table 4, p. 7, row 11
report
1443.15other: Congruent melting L = SiPL: P 0.5, Si 0.5; SiP: P 0.5, Si 0.5experimental[1] Liang 2014
cites Ugai 1987
Table 4, p. 7, row 7
report
1442.15other: Congruent melting L = SiP2L: P 0.666667, Si 0.333333; SiP2: P 0.666667, Si 0.333333model[1] Liang 2014Table 4, p. 7, row 13
report
1434.15other: Congruent melting L = SiPL: P 0.5, Si 0.5; SiP: P 0.5, Si 0.5model[1] Liang 2014Table 4, p. 7, row 10
report
1430.15eutectic: Eutectic L = SiP + SiP2SiP: P 0.5, Si 0.5 (basis unresolved); SiP2: P 0.666667, Si 0.333333 (basis unresolved)model[1] Liang 2014Table 4, p. 7, row 16
report
1429.15other: Congruent melting L = SiP2L: P 0.666667, Si 0.333333; SiP2: P 0.666667, Si 0.333333model[1] Liang 2014
cites Jung 2012 doi
Table 4, p. 7, row 12
report
1412.15other: Congruent melting L = SiPL: P 0.5, Si 0.5; SiP: P 0.5, Si 0.5experimental[1] Liang 2014
cites Safarian 2011 doi
Table 4, p. 7, row 8
report
1410.15other: Congruent melting L = SiPL: P 0.5, Si 0.5; SiP: P 0.5, Si 0.5model[1] Liang 2014
cites Jung 2012 doi
Table 4, p. 7, row 9
report
1407.15eutectic: Eutectic L = (Si) + SiPSiP: P 0.5, Si 0.5 (basis unresolved)model[1] Liang 2014Table 4, p. 7, row 6
report
1407.15eutectic: Eutectic L = SiP + SiP2SiP: P 0.5, Si 0.5; SiP2: P 0.666667, Si 0.333333model[1] Liang 2014
cites Jung 2012 doi
Table 4, p. 7, row 15
report
1404.15eutectic: Eutectic L = (Si) + SiPSiP: P 0.5, Si 0.5 (basis unresolved)model[1] Liang 2014Table 4, p. 7, row 5
report
1404.15eutectic: Eutectic L = (Si) + SiPL: P 0.32807, Si 0.67193; SiP: P 0.5, Si 0.5experimental[1] Liang 2014
cites Giessen 1959
Table 4, p. 7, row 1
report
1404.15eutectic: Eutectic L = (Si) + SiPSiP: P 0.5, Si 0.5experimental[1] Liang 2014
cites Ugai 1987
Table 4, p. 7, row 2
report
1404eutectic: Si-SiP-liq. eutecticSiP: P 0.5unspecified[2] Favre 2024
cites ref. 12
Table 9, p. 50, row 2
report
1404eutectic: Si-SiP-liq. eutecticSiP: P 0.5unspecified[2] Favre 2024
cites as well as Safarian and Tangstad[6] namely for liquidus retained data
Table 9, p. 50, row 1
report
1402.15eutectic: Eutectic L = (Si) + SiPSiP: P 0.5, Si 0.5 (basis unresolved)experimental[1] Liang 2014
cites Safarian 2011 doi
Table 4, p. 7, row 3
report
1402eutectic: Si-SiP-liq. eutecticSiP: P 0.5unspecified[2] Favre 2024
cites ref. 6
Table 9, p. 50, row 4
report
1400.15eutectic: Eutectic L = (Si) + SiPSiP: P 0.5, Si 0.5 (basis unresolved)model[1] Liang 2014
cites Jung 2012 doi
Table 4, p. 7, row 4
report
1400eutectic: Si-SiP-liq. eutecticSiP: P 0.5experimental[2] Favre 2024
cites values for SiP and – (ii) Philipp and Schmidt [59] for SiP2
Table 9, p. 50, row 3
report
1398.15eutectic: Eutectic L = SiP + SiP2SiP: P 0.5, Si 0.5; SiP2: P 0.666667, Si 0.333333experimental[1] Liang 2014
cites Ugai 1987
Table 4, p. 7, row 14
report

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, P–Si system (14)
PhaseCompoundValueT (K)ClassMP DFT (kJ/mol-atom)OQMD DFT (kJ/mol-atom)SourceLocationQuote
SiPSiP-39.52 kJ/mol-atom298.15unspecified-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014
cites ref. 1938Bil
Table 5, p. 8, row 3
report
SiPSiP-37.6 kJ/mol-atom298.15unspecified-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014
cites ref. 1976Kor
Table 5, p. 8, row 4
report
SiPSiP-31.65 kJ/mol-atom298.15model-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014Table 5, p. 8, row 7
report
SiPSiP-31.65 kJ/mol-atom298.15model-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014
cites ref. 2012Jun
Table 5, p. 8, row 6
report
SiPSiP-31.61 kJ/mol-atom298.15model-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014
cites ref. 2011Aru
Table 5, p. 8, row 5
report
SiPSiP-30.95 kJ/mol-atom298.15unspecified-13.047 (mp-aaaaaedq)-26.653 (oqmd-1784005)[1] Liang 2014
cites ref. 1977Bar
Table 5, p. 8, row 2
report
SiP(liq)-63.746 kJ/mol (basis unstated)1443model[2] Favre 2024
cites ref. 11
Table 3, p. 35, row 1
report
SiP(liq)-46.893 kJ/mol (basis unstated)1443model[2] Favre 2024
cites ref. 11
Table 3, p. 35, row 2
report
SiP(liq)36.202 kJ/mol (basis unstated)1418model[2] Favre 2024Table 3, p. 35, row 3
report
SiP(s)-246.525 kJ/mol (basis unstated)1443model[2] Favre 2024
cites ref. 11
Table 3, p. 35, row 1
report
SiP(s)-147.253 kJ/mol (basis unstated)1443model[2] Favre 2024
cites ref. 11
Table 3, p. 35, row 2
report
SiP(s)-66.425 kJ/mol (basis unstated)1418model[2] Favre 2024Table 3, p. 35, row 3
report
SiP2SiP2-26.69 kJ/mol-atom298.15model-12.072 (mp-aaaaaoum)-27.964 (oqmd-7989)[1] Liang 2014Table 5, p. 8, row 9
report
SiP2SiP2-26.43 kJ/mol-atom298.15model-12.072 (mp-aaaaaoum)-27.964 (oqmd-7989)[1] Liang 2014
cites ref. 2012Jun
Table 5, p. 8, row 8
report

Other properties

Phase transition (4)

Phase transition, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Phase transition1237.15 K1237.15otherexperimental[1] Liang 2014p. 2
report
Differential thermal analysis in static air from room temperature to 1015 C shows heating signals in the range 964-990 C but no thermal activity was seen upon cooling.
Phase transition1375 K1375othermodel[2] Favre 2024p. 48
report
We observed that applying a 1 bar pressure, the SiP compound decomposes at 1375K before melting - equilibrium with 1 bar pressure of P2(g) + P4(g).
Phase transition1410.15 K1410.15congruent meltingmodel[1] Liang 2014
cites Jung 2012 doi
p. 9
report
They chose 1137 C as congruent melting temperature of SiP, but it is noted that the pressure-discrepancy increases in their Gas + SiP + liquid range.[5]
Phase transition1443.15 K1443.15congruent meltingexperimental[1] Liang 2014
cites Ugai 1987
p. 9
report
It was found impossible to reconcile in a consistent thermodynamic assessment the experimentally determined[34] high congruent melting temperature of SiP (1170 C, Fig. 2) with the low experimental pressure value at that point from the same group of authors[26] (2.7 bar, Fig. 4); the calculated values are 1161 C and 13 bar.

Phase equilibrium (7)

Phase equilibrium, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Phase composition823Si + (Si)
Si: P 0.0011, Si 0.9989; (Si): P 0.0011, Si 0.9989
experimental[2] Favre 2024
cites ref. 22
Table 2, p. 20, row 6
report
Phase composition923Si + (Si)
Si: P 0.0013, Si 0.9987; (Si): P 0.0013, Si 0.9987
experimental[2] Favre 2024
cites ref. 22
Table 2, p. 20, row 7
report
Phase composition973Si + (Si)
Si: P 0.0014, Si 0.9986; (Si): P 0.0014, Si 0.9986
experimental[2] Favre 2024
cites ref. 16
Table 2, p. 20, row 1
report
Phase composition1073Si + (Si)
Si: P 0.0032, Si 0.9968; (Si): P 0.0032, Si 0.9968
experimental[2] Favre 2024
cites ref. 16
Table 2, p. 20, row 2
report
Phase composition1173Si + (Si)
Si: P 0.0045, Si 0.9955; (Si): P 0.0045, Si 0.9955
experimental[2] Favre 2024
cites ref. 16
Table 2, p. 20, row 3
report
Phase composition1273Si + (Si)
Si: P 0.005, Si 0.995; (Si): P 0.005, Si 0.995
experimental[2] Favre 2024
cites ref. 16
Table 2, p. 20, row 4
report
Phase composition1473Si + (Si)
Si: P 0.0043, Si 0.9957; (Si): P 0.0043, Si 0.9957
experimental[2] Favre 2024
cites ref. 16
Table 2, p. 20, row 5
report

Heat capacity / entropy / enthalpy (12)

Heat capacity / entropy / enthalpy, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Entropy
printed: S°298(SiP, est.)
65 J/mol (basis unstated)/K298 (>)SiP
alloy: Si 0.5
experimental[2] Favre 2024
cites ref. 59
Table 6, p. 44, row 3
report
Entropy
printed: S°298(SiP)
34.78 J/mol (basis unstated)/K298.15SiP
alloy: Si 0.5
experimental[2] Favre 2024
cites ref. 55
Table 6, p. 44, row 2
report
Entropy
printed: S°298
6.3 J/mol-atom/K298.15SiP
alloy: Si 0.5
unspecified[1] Liang 2014
cites ref. 1938Bil
Table 5, p. 8, row 3
report
Entropy
printed: S°298
14.7 J/mol-atom/K298.15SiP
alloy: Si 0.5
model[1] Liang 2014
cites ref. 2011Aru
Table 5, p. 8, row 5
report
Entropy
printed: S°298
17.37 J/mol-atom/K298.15SiP
alloy: Si 0.5
model[1] Liang 2014Table 5, p. 8, row 7
report
Entropy
printed: S°298
16.3 J/mol-atom/K298.15SiP
alloy: Si 0.5
unspecified[1] Liang 2014
cites ref. 1977Bar
Table 5, p. 8, row 2
report
Entropy
printed: S°298
7.95 J/mol-atom/K298.15SiP
alloy: Si 0.5
unspecified[1] Liang 2014
cites ref. 1976Kor
Table 5, p. 8, row 4
report
Entropy
printed: S°298
17.37 J/mol-atom/K298.15SiP
alloy: Si 0.5
experimental[1] Liang 2014
cites ref. 1979Uga
Table 5, p. 8, row 1
report
Entropy
printed: S°298
17.37 J/mol-atom/K298.15SiP
alloy: Si 0.5
model[1] Liang 2014
cites ref. 2012Jun
Table 5, p. 8, row 6
report
Entropy
printed: S°298
22.33 J/mol-atom/K298.15SiP2
alloy: Si 0.333333
model[1] Liang 2014
cites ref. 2012Jun
Table 5, p. 8, row 8
report
Entropy
printed: S°298
21.35 J/mol-atom/K298.15SiP2
alloy: Si 0.333333
model[1] Liang 2014Table 5, p. 8, row 9
report
Heat capacity
printed: C°p(SiP, 298 K)
35.23 J/mol (basis unstated)/K298.15SiP
alloy: Si 0.5
experimental[2] Favre 2024
cites ref. 55
Table 6, p. 44, row 2
report

Activity / EMF / Gibbs energy (5)

Activity / EMF / Gibbs energy, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Vapour pressure
printed: p
3.37 bar1398experimental[2] Favre 2024p. 29
report
Eutectic temperature between the two compounds is 1398K and 3.37 bar obtained by extrapolation.
Vapour pressure
printed: p
0.944 bar1400experimental[2] Favre 2024p. 29
report
A minimum temperature as extrapolated corresponds to the eutectic between Si and SiP is at about 1400 K for 0.944 bar according to their original graph.
Vapour pressure
printed: p
2.5 bar1439experimental[2] Favre 2024
cites ref. 45
p. 29
report
The maximum temperature would correspond to the congruent melting point of SiP that is observed at 1439 ± 5 K for 2.5 bar a pressure composed mainly by P2(g) + P4(g).
Vapour pressure
printed: total pressure
2.7 bar1443experimental[2] Favre 2024p. 29
report
Full results allow the authors to propose the melting temperature of the two compounds as well as their total pressure in equilibrium: for SiP 1443K and 2.7 bar and for SiP2 1451K and 3.7 bar.
Vapour pressure
printed: total pressure
3.7 bar1451experimental[2] Favre 2024p. 29
report
Full results allow the authors to propose the melting temperature of the two compounds as well as their total pressure in equilibrium: for SiP 1443K and 2.7 bar and for SiP2 1451K and 3.7 bar.

Crystal structure (6)

Crystal structure, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Lattice a20.49 Å298.15SiP
alloy: Si 0.5
experimental[3] Liu 2016
cites Wadsten 1975
Table 1, p. 3, row 1
report
Lattice a13.97 Å298.15SiP2
alloy: Si 0.333333
experimental[3] Liu 2016
cites Wadsten 1967 doi
Table 1, p. 3, row 2
report
Lattice b13.61 Å298.15SiP
alloy: Si 0.5
experimental[3] Liu 2016
cites Wadsten 1975
Table 1, p. 3, row 1
report
Lattice b10.08 Å298.15SiP2
alloy: Si 0.333333
experimental[3] Liu 2016
cites Wadsten 1967 doi
Table 1, p. 3, row 2
report
Lattice c3.51 Å298.15SiP
alloy: Si 0.5
experimental[3] Liu 2016
cites Wadsten 1975
Table 1, p. 3, row 1
report
Lattice c3.43 Å298.15SiP2
alloy: Si 0.333333
experimental[3] Liu 2016
cites Wadsten 1967 doi
Table 1, p. 3, row 2
report

Model expression (1)

Model expression, P–Si system
PropertyValueT (K)Phases / compositionClassSourceLocationQuote
Heat capacity
printed: C°p(SiP2)
expression: 67.02 + 17.14·10^-3 T298 (>)SiP2experimental[2] Favre 2024
cites ref. 59
Table 6, p. 44, row 3
report

Sources

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

  1. Song-Mao Liang, Rainer Schmid-Fetzer, Modeling of Thermodynamic Properties and Phase Equilibria of the Si-P System, J. Phase Equilib. Diffus. 35, 24-35 (2014). doi:10.1007/s11669-013-0269-3
  2. Simon Favre, Ioana Nuta, Guy Chichignoud, Evelyne Fischer, Christian Chatillon, Critical assessment of the Si-P system: P solubility in the Si-rich region and refining by phosphorus distillation, Calphad 87, 102758 (2024). doi:10.1016/j.calphad.2024.102758
  3. Ya Liu, Bin Zhou, Wei Lv, Changjun Wu, Xuping Su, Jianhua Wang, Experimental investigation and thermodynamic assessment of the Zn–Si–P system, Surface and Coatings Technology 306, 370-377 (2016). doi:10.1016/j.surfcoat.2016.01.016