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-3.188 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density3.35 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap6.022 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 MauguinPnma [62] |
Hall-P 2ac 2n |
Point Groupmmm |
Crystal Systemorthorhombic |
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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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
DyScO3 (mp-31120) | <0 0 1> | <1 0 1> | 62.5 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 216.0 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 1> | 187.6 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 225.4 |
DyScO3 (mp-31120) | <1 1 1> | <0 1 0> | 218.1 |
InAs (mp-20305) | <1 0 0> | <0 1 0> | 261.7 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 200.4 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 100.2 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 144.0 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 225.4 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 114.6 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 57.3 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 216.0 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 144.0 |
CdS (mp-672) | <1 1 1> | <0 1 0> | 261.7 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 218.1 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 72.0 |
LiF (mp-1138) | <1 1 1> | <1 0 0> | 57.3 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 175.3 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 216.0 |
Te2W (mp-22693) | <1 1 0> | <1 1 0> | 216.0 |
YVO4 (mp-19133) | <0 0 1> | <0 1 0> | 305.4 |
YVO4 (mp-19133) | <1 0 0> | <0 0 1> | 275.5 |
YVO4 (mp-19133) | <1 0 1> | <0 0 1> | 275.5 |
YVO4 (mp-19133) | <1 1 0> | <0 1 0> | 130.9 |
YVO4 (mp-19133) | <1 1 1> | <0 0 1> | 250.5 |
TePb (mp-19717) | <1 1 0> | <1 1 1> | 305.0 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 325.6 |
Te2Mo (mp-602) | <1 0 0> | <1 1 0> | 216.0 |
LaAlO3 (mp-2920) | <0 0 1> | <1 0 1> | 312.6 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 1> | 312.6 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 171.9 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 72.0 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 57.3 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 250.5 |
AlN (mp-661) | <1 0 0> | <1 1 0> | 216.0 |
AlN (mp-661) | <1 0 1> | <1 0 1> | 125.0 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 216.0 |
AlN (mp-661) | <1 1 1> | <1 1 1> | 228.7 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 275.5 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 100.2 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 144.0 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 114.6 |
GaSe (mp-1943) | <1 0 0> | <0 0 1> | 200.4 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 200.4 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 200.4 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 275.5 |
GaN (mp-804) | <1 0 0> | <1 1 1> | 152.5 |
GaN (mp-804) | <1 0 1> | <1 0 1> | 187.6 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 150.3 |
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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Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
2.98 | 0.00 | 0.00 |
0.00 | 2.87 | 0.00 |
0.00 | 0.00 | 3.01 |
Dielectric Tensor εij (total) |
||
---|---|---|
8.85 | 0.00 | 0.00 |
0.00 | 8.04 | 0.00 |
0.00 | 0.00 | 8.52 |
Polycrystalline dielectric constant
εpoly∞
2.95
|
Polycrystalline dielectric constant
εpoly
8.47
|
Refractive Index n1.72 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Zn2SiO4 (mp-1020609) | 0.2722 | 0.083 | 3 |
Mg2SiO4 (mp-554396) | 0.2887 | 0.223 | 3 |
Co2SiO4 (mp-555558) | 0.3005 | 0.617 | 3 |
Mg2SiO4 (mp-560321) | 0.3035 | 0.169 | 3 |
Ca2GeO4 (mp-560647) | 0.2839 | 0.000 | 3 |
LiFeBO4 (mp-777222) | 0.1764 | 0.239 | 4 |
CaMgSiO4 (mp-6493) | 0.1734 | 0.000 | 4 |
LiSiBiO4 (mp-753327) | 0.2497 | 0.021 | 4 |
LiVBO4 (mp-770028) | 0.2288 | 0.091 | 4 |
CaMgGeO4 (mp-558362) | 0.2413 | 0.000 | 4 |
Fe3S4 (mp-21515) | 0.6193 | 0.197 | 2 |
Cr3N4 (mp-1014379) | 0.6103 | 0.105 | 2 |
Mn3N4 (mp-1080204) | 0.5796 | 0.172 | 2 |
Cr3N4 (mp-1014358) | 0.5020 | 0.227 | 2 |
Fe3O4 (mp-19306) | 0.6219 | 0.000 | 2 |
Li4CuNi3(PO4)4 (mp-767664) | 0.3735 | 0.014 | 5 |
Li4MnCo3(PO4)4 (mp-767249) | 0.3736 | 0.502 | 5 |
Li2CrFe(PO4)2 (mp-861527) | 0.3608 | 1.608 | 5 |
Li4CrNi3(PO4)4 (mp-767198) | 0.3654 | 0.027 | 5 |
Li2CrCo(PO4)2 (mp-761707) | 0.3734 | 0.035 | 5 |
Li3MnFeCo(PO4)3 (mp-764912) | 0.4022 | 0.282 | 6 |
Li3MnFeCo(PO4)3 (mp-764869) | 0.3996 | 0.032 | 6 |
Li3MnFeCo(PO4)3 (mp-764707) | 0.3996 | 0.035 | 6 |
Li3MnFeCo(PO4)3 (mp-764969) | 0.4025 | 0.057 | 6 |
Li3MnFeCo(PO4)3 (mp-764870) | 0.4031 | 0.466 | 6 |
Run TypeGGA |
Energy Cutoff700 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Al B O |
Final Energy/Atom-7.3322 eV |
Corrected Energy-216.5377 eV
-216.5377 eV = -205.3010 eV (uncorrected energy) - 11.2366 eV (MP Anion Correction)
|
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)