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-3.333 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.005 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. |
Density5.84 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToK2U2O7 |
Band Gap1.624 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 MauguinP1 [2] |
Hall-P 1 |
Point Group1 |
Crystal Systemtriclinic |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 1> | <0 1 0> | 222.6 |
LaAlO3 (mp-2920) | <1 1 0> | <1 -1 1> | 237.6 |
AlN (mp-661) | <0 0 1> | <0 1 -1> | 126.3 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 246.5 |
AlN (mp-661) | <1 1 0> | <1 0 -1> | 217.5 |
LaAlO3 (mp-2920) | <0 0 1> | <0 1 0> | 222.6 |
AlN (mp-661) | <1 0 0> | <1 0 -1> | 217.5 |
AlN (mp-661) | <1 1 1> | <1 0 -1> | 145.0 |
CeO2 (mp-20194) | <1 1 0> | <1 -1 0> | 215.2 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 169.4 |
BaF2 (mp-1029) | <1 1 0> | <1 -1 1> | 158.4 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 278.3 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 222.6 |
GaN (mp-804) | <1 0 1> | <0 1 -1> | 252.6 |
GaN (mp-804) | <1 1 0> | <1 -1 1> | 237.6 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 254.1 |
GaN (mp-804) | <1 0 0> | <1 -1 1> | 237.6 |
InAs (mp-20305) | <1 1 0> | <1 -1 1> | 158.4 |
SiO2 (mp-6930) | <1 1 0> | <1 0 1> | 151.4 |
KCl (mp-23193) | <1 1 0> | <1 -1 1> | 237.6 |
KCl (mp-23193) | <1 1 1> | <0 1 0> | 222.6 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 167.0 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 254.1 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 221.3 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 278.3 |
Te2W (mp-22693) | <0 1 0> | <1 0 1> | 227.1 |
Te2W (mp-22693) | <1 1 1> | <1 0 1> | 227.1 |
TePb (mp-19717) | <1 1 0> | <1 -1 1> | 237.6 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 278.3 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 169.4 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 -1> | 252.6 |
Te2Mo (mp-602) | <1 0 0> | <1 -1 1> | 158.4 |
Te2Mo (mp-602) | <1 0 1> | <1 0 1> | 227.1 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 227.1 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 221.3 |
LiF (mp-1138) | <1 1 0> | <0 1 1> | 168.1 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 1 0> | 222.6 |
Te2W (mp-22693) | <0 0 1> | <1 0 -1> | 217.5 |
BN (mp-984) | <1 1 1> | <1 0 0> | 166.0 |
TePb (mp-19717) | <1 1 1> | <0 1 0> | 222.6 |
Te2Mo (mp-602) | <0 0 1> | <1 -1 1> | 316.8 |
Ag (mp-124) | <1 0 0> | <1 -1 -1> | 188.4 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 168.1 |
LiNbO3 (mp-3731) | <1 0 0> | <0 1 0> | 222.6 |
GaSe (mp-1943) | <0 0 1> | <1 -1 0> | 286.9 |
MoS2 (mp-1434) | <0 0 1> | <0 1 0> | 222.6 |
BN (mp-984) | <0 0 1> | <0 1 -1> | 126.3 |
BN (mp-984) | <1 0 0> | <1 1 0> | 254.1 |
BN (mp-984) | <1 0 1> | <0 1 0> | 222.6 |
BN (mp-984) | <1 1 0> | <1 0 1> | 302.8 |
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 |
---|---|---|---|
Na5Mn3F14 (mp-615626) | 0.5226 | 0.000 | 3 |
Rb2U2O7 (mp-674373) | 0.2870 | 0.008 | 3 |
Rb8U9O31 (mp-683981) | 0.3935 | 0.010 | 3 |
Na5Mn3F14 (mp-558166) | 0.5222 | 0.000 | 3 |
Rb4U5O17 (mp-558239) | 0.5950 | 0.004 | 3 |
Na2Te4MoO12 (mp-559249) | 0.7143 | 0.000 | 4 |
NaCaAlF6 (mp-558169) | 0.6873 | 0.007 | 4 |
Na2Te4WO12 (mp-562125) | 0.6255 | 0.000 | 4 |
UAg2(WO5)2 (mp-705061) | 0.7221 | 0.012 | 4 |
Na2U(WO5)2 (mp-566655) | 0.6995 | 0.000 | 4 |
UO3 (mp-616580) | 0.6653 | 0.134 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: K_sv U O |
Final Energy/Atom-8.2899 eV |
Corrected Energy-191.9954 eV
Uncorrected energy = -182.3774 eV
Composition-based energy adjustment (-0.687 eV/atom x 14.0 atoms) = -9.6180 eV
Corrected energy = -191.9954 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)