Final Magnetic Moment0.597 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-0.221 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.014 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. |
Density11.33 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToUNi5 + InNi + U11Ni16 |
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 MauguinF43m [216] |
HallF 4 2 3 |
Point Group43m |
Crystal Systemcubic |
Topological ClassificationSM*
|
SubclassificationESFD†
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Crossing TypePoint
|
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] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 337.5 |
AlN (mp-661) | <1 0 0> | <1 1 1> | 250.5 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 241.1 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 136.4 |
GaAs (mp-2534) | <1 1 1> | <1 0 0> | 289.3 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 192.9 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 241.1 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 272.8 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 337.5 |
SiO2 (mp-6930) | <1 1 1> | <1 1 0> | 204.6 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 192.9 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 272.8 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 272.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 167.0 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 241.1 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 192.9 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 204.6 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 250.5 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 136.4 |
ZnSe (mp-1190) | <1 1 1> | <1 0 0> | 289.3 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 68.2 |
KTaO3 (mp-3614) | <1 1 1> | <1 1 1> | 83.5 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 144.7 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 204.6 |
LiF (mp-1138) | <1 1 1> | <1 0 0> | 144.7 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 272.8 |
NaCl (mp-22862) | <1 1 0> | <1 1 0> | 136.4 |
NaCl (mp-22862) | <1 1 1> | <1 1 0> | 272.8 |
ZrO2 (mp-2858) | <0 0 1> | <1 0 0> | 241.1 |
ZrO2 (mp-2858) | <1 0 -1> | <1 0 0> | 144.7 |
SiC (mp-8062) | <1 0 0> | <1 0 0> | 96.4 |
CdWO4 (mp-19387) | <0 0 1> | <1 1 0> | 272.8 |
TiO2 (mp-390) | <0 0 1> | <1 0 0> | 192.9 |
CsI (mp-614603) | <1 0 0> | <1 0 0> | 241.1 |
CsI (mp-614603) | <1 1 0> | <1 1 0> | 272.8 |
MgF2 (mp-1249) | <0 0 1> | <1 0 0> | 192.9 |
MgF2 (mp-1249) | <1 0 0> | <1 0 0> | 144.7 |
ZnO (mp-2133) | <0 0 1> | <1 1 1> | 83.5 |
ZnO (mp-2133) | <1 1 0> | <1 1 0> | 272.8 |
MgAl2O4 (mp-3536) | <1 1 0> | <1 1 0> | 272.8 |
GaSb (mp-1156) | <1 0 0> | <1 0 0> | 192.9 |
SrTiO3 (mp-4651) | <0 0 1> | <1 0 0> | 241.1 |
SrTiO3 (mp-4651) | <1 0 0> | <1 1 0> | 136.4 |
SrTiO3 (mp-4651) | <1 0 1> | <1 1 1> | 167.0 |
SrTiO3 (mp-4651) | <1 1 0> | <1 0 0> | 241.1 |
Cu (mp-30) | <1 0 0> | <1 0 0> | 241.1 |
Cu (mp-30) | <1 1 0> | <1 1 0> | 204.6 |
Ge (mp-32) | <1 1 0> | <1 1 0> | 136.4 |
Ge (mp-32) | <1 1 1> | <1 0 0> | 289.3 |
LiAlO2 (mp-3427) | <0 0 1> | <1 0 0> | 241.1 |
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 |
---|---|---|---|
MgCu4Sn (mp-3676) | 0.0005 | 0.000 | 3 |
MnCu4Sn (mp-1072398) | 0.0000 | 0.058 | 3 |
DyNi4Au (mp-1077279) | 0.0005 | 0.000 | 3 |
SmInPt4 (mp-1077380) | 0.0005 | 0.000 | 3 |
YbCu4Ag (mp-1077741) | 0.0000 | 0.000 | 3 |
Be5Co (mp-1071690) | 0.0026 | 0.000 | 2 |
ZrCu5 (mp-30603) | 0.0005 | 0.010 | 2 |
Be5Pt (mp-1072399) | 0.0022 | 0.000 | 2 |
PaPt5 (mp-1077534) | 0.0029 | 0.000 | 2 |
PuPt5 (mp-1080388) | 0.0029 | 0.000 | 2 |
Co (mp-1072089) | 0.0143 | 0.199 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: U In_d Ni_pv |
Final Energy/Atom-6.4146 eV |
Corrected Energy-38.4878 eV
Uncorrected energy = -38.4878 eV
Corrected energy = -38.4878 eV
|
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)