Final Magnetic Moment6.004 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-2.149 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.064 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. |
Density5.04 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCo2SiO4 |
Band Gap0.772 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 MauguinFd3m [227] |
HallF 4d 2 3 1d |
Point Groupm3m |
Crystal Systemcubic |
Topological ClassificationTI*
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SubclassificationSEBR†
|
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] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 269.7 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 67.4 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 116.8 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 286.0 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 286.0 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 95.3 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 0> | 190.7 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 67.4 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 269.7 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 134.8 |
DyScO3 (mp-31120) | <1 0 0> | <1 1 0> | 95.3 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 95.3 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 95.3 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 116.8 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 269.7 |
TePb (mp-19717) | <1 1 0> | <1 1 0> | 190.7 |
CdS (mp-672) | <1 0 0> | <1 1 0> | 286.0 |
CdS (mp-672) | <1 1 1> | <1 0 0> | 269.7 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 67.4 |
TeO2 (mp-2125) | <1 0 0> | <1 1 0> | 286.0 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 0> | 134.8 |
CdTe (mp-406) | <1 1 0> | <1 1 0> | 190.7 |
TeO2 (mp-2125) | <1 1 0> | <1 0 0> | 202.3 |
GdScO3 (mp-5690) | <0 1 0> | <1 0 0> | 134.8 |
GdScO3 (mp-5690) | <1 1 0> | <1 0 0> | 67.4 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 286.0 |
Mg (mp-153) | <1 0 0> | <1 1 0> | 286.0 |
C (mp-66) | <1 1 0> | <1 1 0> | 286.0 |
GdScO3 (mp-5690) | <1 0 0> | <1 1 0> | 95.3 |
Mg (mp-153) | <1 1 1> | <1 0 0> | 269.7 |
BaTiO3 (mp-5986) | <0 0 1> | <1 0 0> | 269.7 |
BaTiO3 (mp-5986) | <1 0 0> | <1 0 0> | 67.4 |
BaTiO3 (mp-5986) | <1 1 0> | <1 1 0> | 95.3 |
GaP (mp-2490) | <1 0 0> | <1 0 0> | 269.7 |
TbScO3 (mp-31119) | <0 1 0> | <1 0 0> | 134.8 |
TbScO3 (mp-31119) | <1 0 0> | <1 1 0> | 95.3 |
TbScO3 (mp-31119) | <1 1 0> | <1 1 0> | 190.7 |
NdGaO3 (mp-3196) | <0 0 1> | <1 0 0> | 269.7 |
Ga2O3 (mp-886) | <1 0 0> | <1 1 0> | 286.0 |
Ni (mp-23) | <1 1 0> | <1 1 0> | 190.7 |
InSb (mp-20012) | <1 1 0> | <1 1 0> | 190.7 |
NaCl (mp-22862) | <1 0 0> | <1 0 0> | 67.4 |
Ga2O3 (mp-886) | <0 1 0> | <1 1 0> | 286.0 |
Ga2O3 (mp-886) | <1 1 0> | <1 1 0> | 286.0 |
Si (mp-149) | <1 0 0> | <1 0 0> | 269.7 |
CdWO4 (mp-19387) | <0 1 0> | <1 0 0> | 134.8 |
NaCl (mp-22862) | <1 1 0> | <1 1 0> | 95.3 |
ZrO2 (mp-2858) | <0 0 1> | <1 0 0> | 134.8 |
MgAl2O4 (mp-3536) | <1 0 0> | <1 0 0> | 67.4 |
MgAl2O4 (mp-3536) | <1 1 0> | <1 1 0> | 95.3 |
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 |
---|---|---|---|
Yb2MnS4 (mp-20213) | 0.1162 | 0.312 | 3 |
Zn2SiO4 (mp-558096) | 0.1012 | 0.145 | 3 |
Si(NiO2)2 (mp-18766) | 0.0925 | 0.027 | 3 |
Fe2SiO4 (mp-18816) | 0.1045 | 0.039 | 3 |
Co2SiO4 (mp-561534) | 0.0620 | 0.064 | 3 |
LiTiSiO4 (mp-753305) | 0.2046 | 0.076 | 4 |
LiMnVO4 (mp-861571) | 0.2287 | 0.024 | 4 |
LiNiPO4 (mp-767362) | 0.2279 | 0.079 | 4 |
LiVSiO4 (mp-767033) | 0.2549 | 0.041 | 4 |
LiVFeO4 (mp-773535) | 0.2450 | 0.016 | 4 |
Fe3S4 (mp-21515) | 0.4826 | 0.197 | 2 |
Fe3S4 (mp-850016) | 0.4805 | 0.144 | 2 |
Cr3N4 (mp-1014379) | 0.4599 | 0.105 | 2 |
Cr3N4 (mp-1014358) | 0.4643 | 0.226 | 2 |
Fe3O4 (mp-19306) | 0.4689 | 0.000 | 2 |
Li4FeNi3(PO4)4 (mp-767739) | 0.4111 | 0.158 | 5 |
Li4VNi3(PO4)4 (mp-761403) | 0.4091 | 0.029 | 5 |
Li2VNi(PO4)2 (mp-761302) | 0.4092 | 0.054 | 5 |
Li4CoNi3(PO4)4 (mp-853138) | 0.4104 | 0.013 | 5 |
Li2FeNi(PO4)2 (mp-769706) | 0.4079 | 0.002 | 5 |
Li3MnFeCo(PO4)3 (mp-764809) | 0.4712 | 0.014 | 6 |
Li3MnFeCo(PO4)3 (mp-764869) | 0.4695 | 0.032 | 6 |
Li3MnFeCo(PO4)3 (mp-764707) | 0.4724 | 0.035 | 6 |
Li3MnFeCo(PO4)3 (mp-764969) | 0.4668 | 0.057 | 6 |
Li3MnFeCo(PO4)3 (mp-764870) | 0.4704 | 0.466 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCo: 3.32 eV |
PseudopotentialsVASP PAW: Co Si O |
Final Energy/Atom-6.8455 eV |
Corrected Energy-107.8851 eV
Uncorrected energy = -95.8371 eV
Composition-based energy adjustment (-0.687 eV/atom x 8.0 atoms) = -5.4960 eV
Composition-based energy adjustment (-1.638 eV/atom x 4.0 atoms) = -6.5520 eV
Corrected energy = -107.8851 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)