Final Magnetic Moment10.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-1.945 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.058 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. |
Density3.42 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToNi2P2O7 + Ni3(PO4)2 + O2 |
Band Gap0.000 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 MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
Crystal Systemmonoclinic |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 1 0> | 270.6 |
GaAs (mp-2534) | <1 0 0> | <1 1 0> | 228.3 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 275.8 |
SiO2 (mp-6930) | <1 1 1> | <0 1 0> | 270.6 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 0> | 270.6 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 0> | 275.8 |
ZnSe (mp-1190) | <1 0 0> | <1 1 0> | 228.3 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 202.9 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 228.3 |
YVO4 (mp-19133) | <1 0 0> | <1 0 0> | 91.9 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 275.8 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 183.8 |
Te2Mo (mp-602) | <0 0 1> | <0 1 1> | 164.9 |
Te2Mo (mp-602) | <1 0 1> | <0 1 1> | 164.9 |
Ag (mp-124) | <1 1 0> | <1 0 0> | 275.8 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 275.8 |
BN (mp-984) | <0 0 1> | <0 1 0> | 202.9 |
LiNbO3 (mp-3731) | <1 0 0> | <0 0 1> | 150.4 |
MoS2 (mp-1434) | <0 0 1> | <0 1 0> | 270.6 |
MoS2 (mp-1434) | <1 0 0> | <1 0 0> | 275.8 |
MoS2 (mp-1434) | <1 0 1> | <1 0 0> | 275.8 |
CdTe (mp-406) | <1 1 0> | <1 0 0> | 183.8 |
BaF2 (mp-1029) | <1 0 0> | <1 0 1> | 194.7 |
LiTaO3 (mp-3666) | <1 0 0> | <0 0 1> | 150.4 |
TiO2 (mp-2657) | <0 0 1> | <1 0 1> | 194.7 |
TiO2 (mp-2657) | <1 0 1> | <1 0 -1> | 155.7 |
TiO2 (mp-2657) | <1 1 0> | <1 0 0> | 275.8 |
Mg (mp-153) | <0 0 1> | <0 1 0> | 270.6 |
MgO (mp-1265) | <1 1 0> | <1 0 0> | 275.8 |
KP(HO2)2 (mp-23959) | <0 0 1> | <0 0 1> | 150.4 |
KP(HO2)2 (mp-23959) | <0 1 0> | <0 0 1> | 150.4 |
LaF3 (mp-905) | <1 0 1> | <1 0 0> | 275.8 |
C (mp-66) | <1 0 0> | <0 1 0> | 270.6 |
GdScO3 (mp-5690) | <0 1 1> | <0 1 0> | 270.6 |
TbScO3 (mp-31119) | <0 1 1> | <0 1 0> | 270.6 |
Ni (mp-23) | <1 1 0> | <1 0 0> | 275.8 |
TbScO3 (mp-31119) | <1 1 1> | <1 0 0> | 275.8 |
InSb (mp-20012) | <1 1 0> | <1 0 0> | 183.8 |
Ga2O3 (mp-886) | <1 0 0> | <0 1 0> | 202.9 |
CdSe (mp-2691) | <1 0 0> | <1 0 1> | 194.7 |
WS2 (mp-224) | <0 0 1> | <0 1 0> | 270.6 |
PbSe (mp-2201) | <1 0 0> | <1 0 1> | 194.7 |
Ga2O3 (mp-886) | <1 0 -1> | <0 1 0> | 270.6 |
Ga2O3 (mp-886) | <1 1 0> | <1 1 0> | 228.3 |
Au (mp-81) | <1 1 0> | <1 0 0> | 275.8 |
WS2 (mp-224) | <1 0 0> | <1 0 0> | 91.9 |
WS2 (mp-224) | <1 1 0> | <1 0 -1> | 155.7 |
NaCl (mp-22862) | <1 0 0> | <1 1 0> | 228.3 |
ZrO2 (mp-2858) | <0 1 1> | <0 1 0> | 270.6 |
TiO2 (mp-390) | <0 0 1> | <1 0 0> | 275.8 |
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 |
---|---|---|---|
Li2Cr2O7 (mp-770678) | 0.3822 | 0.020 | 3 |
CrPO4 (mp-764345) | 0.4099 | 0.022 | 3 |
PRhO4 (mp-28870) | 0.3276 | 0.000 | 3 |
CrPO4 (mp-19401) | 0.4116 | 0.000 | 3 |
PWO4 (mp-25654) | 0.4014 | 0.109 | 3 |
Li3Fe2(PO4)3 (mp-853256) | 0.4157 | 0.015 | 4 |
LiP2WO7 (mp-763478) | 0.4106 | 0.053 | 4 |
Li2Mo(PO4)2 (mp-697748) | 0.4220 | 0.037 | 4 |
Li3Ni3(PO4)4 (mp-540306) | 0.3534 | 0.078 | 4 |
LiCr2(PO4)3 (mp-697765) | 0.4145 | 0.074 | 4 |
CrO2 (mvc-11581) | 0.5601 | 0.166 | 2 |
VO2 (mp-777469) | 0.5479 | 0.038 | 2 |
Cr5O12 (mp-19575) | 0.6420 | 0.025 | 2 |
VO2 (mvc-6918) | 0.4909 | 0.094 | 2 |
MoO2 (mvc-6944) | 0.4811 | 0.281 | 2 |
Li6MnV3(PO4)6 (mp-775325) | 0.4865 | 0.023 | 5 |
Fe2Ni3P6WO24 (mp-771051) | 0.4570 | 0.094 | 5 |
Li3MnV(PO4)3 (mp-772102) | 0.4317 | 0.058 | 5 |
Li3MnV(PO4)3 (mp-775267) | 0.4937 | 0.039 | 5 |
ZnCuNiP2O9 (mvc-8436) | 0.4585 | 0.113 | 5 |
LiMgCr3Se2(SO6)4 (mp-769552) | 0.5841 | 0.255 | 6 |
NaLi3Ti2Fe2(PO4)6 (mp-850140) | 0.5837 | 0.011 | 6 |
NaLi3Ti2Cr2(PO4)6 (mp-777190) | 0.5804 | 0.020 | 6 |
Li2MgCr3Se3(SO8)3 (mp-773983) | 0.6142 | 0.330 | 6 |
Mn4Si4SnB2(HO9)2 (mp-743890) | 0.5959 | 0.000 | 6 |
Ca2Al2FeSi4BHO16 (mp-540713) | 0.6929 | 0.002 | 7 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesNi: 6.2 eV |
PseudopotentialsVASP PAW: Ni_pv P O |
Final Energy/Atom-6.2613 eV |
Corrected Energy-263.6698 eV
-263.6698 eV = -231.6669 eV (uncorrected energy) - 16.8550 eV (MP Anion Correction) - 15.1480 eV (MP Advanced Correction)
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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)