Final Magnetic Moment0.262 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 / Atom0.072 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.617 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. |
Density10.68 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToThBr4 + Th |
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 MauguinI4/mmm [139] |
Hall-I 4 2 |
Point Group4/mmm |
Crystal Systemtetragonal |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 362.0 |
AlN (mp-661) | <1 0 0> | <1 0 1> | 109.5 |
AlN (mp-661) | <1 1 1> | <1 1 1> | 220.7 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 313.7 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 193.1 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 193.1 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 289.6 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 120.7 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 168.9 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 193.1 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 120.7 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 193.1 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 313.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 217.2 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 69.5 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 144.8 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 144.8 |
CdS (mp-672) | <1 0 1> | <0 0 1> | 362.0 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 208.5 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 217.2 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 69.5 |
Te2W (mp-22693) | <0 1 1> | <0 0 1> | 289.6 |
YVO4 (mp-19133) | <0 0 1> | <1 1 0> | 208.5 |
YVO4 (mp-19133) | <1 0 1> | <1 0 1> | 219.0 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 196.5 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 193.1 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 245.7 |
AlN (mp-661) | <1 1 0> | <1 0 1> | 54.7 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 120.7 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 139.0 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 278.0 |
SiO2 (mp-6930) | <1 0 0> | <1 0 1> | 54.7 |
SiO2 (mp-6930) | <1 0 1> | <1 0 1> | 273.7 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 273.7 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 278.0 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 289.6 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 139.0 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 278.0 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 265.5 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 217.2 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 144.8 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 217.2 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 208.5 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 217.2 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 168.9 |
Te2Mo (mp-602) | <1 0 0> | <1 1 0> | 208.5 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 217.2 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 217.2 |
Ag (mp-124) | <1 1 0> | <1 0 1> | 219.0 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 343.9 |
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 |
---|---|---|---|
ZnCu2Ni (mp-30593) | 0.0470 | 0.005 | 3 |
CrCoPt2 (mp-570863) | 0.0573 | 0.000 | 3 |
LiCa6Ge (mp-12609) | 0.0655 | 0.180 | 3 |
GaFeNi2 (mp-1065359) | 0.0556 | 0.066 | 3 |
GaCo2Ni (mp-1018060) | 0.0588 | 0.075 | 3 |
Cr8Ni50Mo15W2 (mp-767372) | 0.1861 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.3338 | 0.118 | 4 |
CrFeCoNi (mp-1096923) | 0.3784 | 0.193 | 4 |
Li3Co (mp-976017) | 0.0053 | 0.329 | 2 |
RbPr3 (mp-975253) | 0.0001 | 0.502 | 2 |
Nd3Mg (mp-976421) | 0.0070 | 0.053 | 2 |
Ni3Au (mp-976818) | 0.0018 | 0.097 | 2 |
NaBi (mp-22924) | 0.0018 | 0.000 | 2 |
Pr (mp-97) | 0.0549 | 0.008 | 1 |
Sm (mp-21377) | 0.0546 | 0.010 | 1 |
Th (mp-37) | 0.0591 | 0.000 | 1 |
Rb (mp-12628) | 0.0545 | 0.015 | 1 |
La (mp-156) | 0.0428 | 0.001 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Th Br |
Final Energy/Atom-5.8979 eV |
Corrected Energy-23.5916 eV
-23.5916 eV = -23.5916 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)