Final Magnetic Moment3.999 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-1.767 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.050 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. |
Density2.40 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCrCl3 + LiCl + Cr |
Band Gap0.354 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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <1 1 -1> | 172.9 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 230.5 |
CeO2 (mp-20194) | <1 1 1> | <1 0 0> | 153.7 |
BaF2 (mp-1029) | <1 1 1> | <1 0 1> | 264.4 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 168.7 |
GaN (mp-804) | <1 0 1> | <0 1 0> | 309.3 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 337.4 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 281.1 |
DyScO3 (mp-31120) | <0 1 0> | <0 1 0> | 309.3 |
InAs (mp-20305) | <1 1 1> | <1 0 1> | 264.4 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 253.0 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 84.3 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 190.4 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 281.1 |
CeO2 (mp-20194) | <1 0 0> | <0 1 0> | 365.5 |
CeO2 (mp-20194) | <1 1 0> | <0 1 0> | 281.1 |
YVO4 (mp-19133) | <1 0 0> | <0 1 0> | 337.4 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 192.1 |
TePb (mp-19717) | <1 0 0> | <1 1 0> | 333.3 |
TePb (mp-19717) | <1 1 0> | <0 1 1> | 242.6 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 268.9 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 192.1 |
SiO2 (mp-6930) | <0 0 1> | <1 0 1> | 88.1 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 115.3 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 253.0 |
KCl (mp-23193) | <1 0 0> | <1 1 0> | 333.3 |
Ag (mp-124) | <1 0 0> | <0 1 0> | 224.9 |
Ag (mp-124) | <1 1 1> | <1 0 -1> | 245.2 |
InAs (mp-20305) | <1 1 0> | <1 0 1> | 264.4 |
GaSe (mp-1943) | <1 0 0> | <1 0 0> | 268.9 |
GaSe (mp-1943) | <1 1 0> | <0 1 1> | 242.6 |
BN (mp-984) | <1 0 1> | <0 1 0> | 224.9 |
BN (mp-984) | <1 1 1> | <1 0 1> | 264.4 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 0> | 253.0 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 115.3 |
CdS (mp-672) | <1 0 0> | <1 1 -1> | 86.4 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 196.8 |
CdS (mp-672) | <1 1 0> | <0 0 1> | 151.6 |
LiNbO3 (mp-3731) | <0 0 1> | <1 0 0> | 268.9 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 0> | 238.0 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 224.9 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 365.5 |
LiF (mp-1138) | <1 1 1> | <1 0 0> | 115.3 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 345.8 |
MoS2 (mp-1434) | <0 0 1> | <0 1 0> | 168.7 |
MoS2 (mp-1434) | <1 0 0> | <1 0 0> | 268.9 |
Al (mp-134) | <1 0 0> | <0 1 0> | 253.0 |
Al (mp-134) | <1 1 0> | <0 1 0> | 253.0 |
YVO4 (mp-19133) | <0 0 1> | <0 1 0> | 309.3 |
Te2Mo (mp-602) | <0 0 1> | <1 1 0> | 238.0 |
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 |
---|---|---|---|
LiV2O4 (mp-771663) | 0.3963 | 0.089 | 3 |
Li2Cr3O6 (mp-762482) | 0.4494 | 0.085 | 3 |
LiMn2O4 (mvc-16811) | 0.4179 | 0.074 | 3 |
MgMn2O4 (mp-1097894) | 0.4452 | 0.072 | 3 |
MgMn2O4 (mp-1002568) | 0.4562 | 0.072 | 3 |
Li2MnCr3O8 (mp-780543) | 0.4176 | 0.094 | 4 |
Li2Cr3FeO8 (mp-780014) | 0.4406 | 0.671 | 4 |
LiCoCuO4 (mp-764366) | 0.4217 | 0.062 | 4 |
LiCoNiO4 (mp-763751) | 0.4390 | 0.057 | 4 |
Li2MnCo3O8 (mp-777604) | 0.3847 | 0.037 | 4 |
Ni3O4 (mp-714961) | 0.6311 | 0.000 | 2 |
Ni3O4 (mp-656887) | 0.6018 | 0.000 | 2 |
Zr3S4 (mp-684749) | 0.5540 | 0.000 | 2 |
Ni5Cl6 (mp-1094110) | 0.6054 | 0.120 | 2 |
Ni3Cl4 (mp-1096770) | 0.6151 | 0.076 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv Cr_pv Cl |
Final Energy/Atom-4.4081 eV |
Corrected Energy-30.8567 eV
-30.8567 eV = -30.8567 eV (uncorrected energy)
|
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)