Final Magnetic Moment0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom-2.381 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.087 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density2.81 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToFeP4 + P2O5 + Fe(PO3)3 |
Band Gap4.329 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinP1 [2] |
Hall-P 1 |
Point Group1 |
Crystal Systemtriclinic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
BN (mp-984) | <1 0 0> | <1 -1 0> | 252.8 |
LiNbO3 (mp-3731) | <1 1 0> | <0 0 1> | 261.7 |
LiNbO3 (mp-3731) | <1 1 1> | <0 0 1> | 261.7 |
LaAlO3 (mp-2920) | <1 0 0> | <1 1 0> | 143.9 |
LiGaO2 (mp-5854) | <0 1 0> | <1 1 1> | 199.4 |
LiGaO2 (mp-5854) | <1 0 0> | <1 1 0> | 143.9 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 261.7 |
CdTe (mp-406) | <1 0 0> | <0 0 1> | 87.2 |
SiC (mp-7631) | <0 0 1> | <1 1 1> | 199.4 |
GaN (mp-804) | <1 0 1> | <1 0 -1> | 211.4 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 174.5 |
Fe3O4 (mp-19306) | <1 0 0> | <1 0 -1> | 211.4 |
TiO2 (mp-2657) | <0 0 1> | <0 0 1> | 87.2 |
TiO2 (mp-2657) | <1 0 1> | <0 0 1> | 261.7 |
LiF (mp-1138) | <1 1 0> | <1 1 -1> | 259.9 |
Mg (mp-153) | <1 0 0> | <1 0 1> | 149.7 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 261.7 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 87.2 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 87.2 |
PbS (mp-21276) | <1 0 0> | <0 0 1> | 174.5 |
GaP (mp-2490) | <1 1 1> | <0 0 1> | 261.7 |
BaTiO3 (mp-5986) | <1 0 1> | <1 1 -1> | 259.9 |
NdGaO3 (mp-3196) | <1 0 1> | <0 0 1> | 261.7 |
Ga2O3 (mp-886) | <0 1 0> | <1 0 -1> | 211.4 |
Si (mp-149) | <1 1 1> | <0 0 1> | 261.7 |
WSe2 (mp-1821) | <0 0 1> | <1 1 -1> | 259.9 |
WSe2 (mp-1821) | <1 0 0> | <1 1 1> | 199.4 |
SiC (mp-8062) | <1 0 0> | <0 0 1> | 174.5 |
CdWO4 (mp-19387) | <0 0 1> | <1 -1 1> | 152.9 |
CdWO4 (mp-19387) | <1 1 0> | <1 0 0> | 287.4 |
TiO2 (mp-390) | <1 0 1> | <1 0 0> | 191.6 |
MgF2 (mp-1249) | <0 0 1> | <0 0 1> | 87.2 |
MgF2 (mp-1249) | <1 0 1> | <0 0 1> | 261.7 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 174.5 |
InSb (mp-20012) | <1 0 0> | <0 0 1> | 87.2 |
BaTiO3 (mp-5986) | <1 0 0> | <1 -1 0> | 252.8 |
BaTiO3 (mp-5986) | <1 1 0> | <1 0 -1> | 211.4 |
BaTiO3 (mp-5986) | <1 1 1> | <1 0 0> | 287.4 |
NdGaO3 (mp-3196) | <0 1 1> | <0 0 1> | 261.7 |
SiC (mp-11714) | <0 0 1> | <1 1 1> | 199.4 |
MoSe2 (mp-1634) | <0 0 1> | <1 1 -1> | 259.9 |
Ga2O3 (mp-886) | <1 1 -1> | <1 -1 0> | 252.8 |
Au (mp-81) | <1 0 0> | <0 0 1> | 87.2 |
ZrO2 (mp-2858) | <0 0 1> | <1 0 0> | 191.6 |
ZrO2 (mp-2858) | <1 0 -1> | <1 1 0> | 143.9 |
CdWO4 (mp-19387) | <0 1 0> | <1 0 0> | 287.4 |
CsI (mp-614603) | <1 1 0> | <1 1 -1> | 259.9 |
MgF2 (mp-1249) | <1 0 0> | <0 0 1> | 87.2 |
MgAl2O4 (mp-3536) | <1 0 0> | <1 0 -1> | 211.4 |
LiAlO2 (mp-3427) | <0 0 1> | <1 0 0> | 191.6 |
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
NiP4O11 (mp-764190) | 0.1261 | 0.009 | 3 |
ZnP4O11 (mp-774868) | 0.0560 | 0.006 | 3 |
MnP4O11 (mp-557493) | 0.1165 | 0.000 | 3 |
CoP4O11 (mp-763297) | 0.0966 | 0.126 | 3 |
MnP4O11 (mp-649781) | 0.1175 | 0.000 | 3 |
LiP4WO13 (mp-763403) | 0.2445 | 0.002 | 4 |
LiP4WO12 (mp-763455) | 0.3493 | 0.017 | 4 |
LiSb(PO3)4 (mp-504340) | 0.1950 | 0.042 | 4 |
LiNb(PO3)4 (mp-757816) | 0.3188 | 0.118 | 4 |
LiSn(PO3)4 (mp-757616) | 0.2891 | 0.078 | 4 |
V5O12 (mp-776915) | 0.6161 | 0.032 | 2 |
MgCr3Se2(SO6)4 (mp-769544) | 0.5712 | 0.126 | 5 |
MnVP2(O4F)2 (mp-777435) | 0.6498 | 0.002 | 5 |
MgCr3Se3(SO8)3 (mp-773999) | 0.5664 | 0.180 | 5 |
LiBS4(ClO3)4 (mp-555090) | 0.6728 | 0.005 | 5 |
Cs3Mg3In(PO3)12 (mp-720658) | 0.6304 | 0.006 | 5 |
RbScBP2HO9 (mp-23809) | 0.7474 | 0.000 | 6 |
CsAlBP2HO9 (mp-542129) | 0.5982 | 0.000 | 6 |
RbAlBP2HO9 (mp-542130) | 0.6788 | 0.000 | 6 |
CsFeBP2HO9 (mp-761395) | 0.7053 | 0.118 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eV |
PseudopotentialsVASP PAW: Fe_pv P O |
Final Energy/Atom-7.0116 eV |
Corrected Energy-487.9931 eV
Uncorrected energy = -448.7411 eV
Composition-based energy adjustment (-0.687 eV/atom x 44.0 atoms) = -30.2280 eV
Composition-based energy adjustment (-2.256 eV/atom x 4.0 atoms) = -9.0240 eV
Corrected energy = -487.9931 eV
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Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)