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-0.848 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. |
Density7.94 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinIbam [72] |
Hall-I 2 2c |
Point Groupmmm |
Crystal Systemorthorhombic |
Topological ClassificationTI*
|
SubclassificationNLC†
|
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) | <0 0 1> | <0 0 1> | 321.6 |
LaAlO3 (mp-2920) | <1 1 0> | <1 0 1> | 128.3 |
AlN (mp-661) | <1 0 0> | <0 1 0> | 271.1 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 214.4 |
CeO2 (mp-20194) | <1 1 0> | <0 1 1> | 86.4 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 160.8 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 135.6 |
BaF2 (mp-1029) | <1 1 0> | <0 1 1> | 172.8 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 53.6 |
GaN (mp-804) | <1 1 0> | <0 1 1> | 86.4 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 214.4 |
KCl (mp-23193) | <1 1 0> | <0 1 1> | 172.8 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 160.8 |
DyScO3 (mp-31120) | <0 1 0> | <0 1 0> | 135.6 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 53.6 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 135.6 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 53.6 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 321.6 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 160.8 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 135.6 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 160.8 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 67.8 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 107.2 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 268.0 |
CdS (mp-672) | <1 0 1> | <0 1 1> | 259.2 |
LiF (mp-1138) | <1 1 0> | <1 0 1> | 256.5 |
YVO4 (mp-19133) | <1 0 1> | <0 0 1> | 214.4 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 321.6 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 321.6 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 107.2 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 53.6 |
Al (mp-134) | <1 0 0> | <0 0 1> | 160.8 |
C (mp-48) | <0 0 1> | <0 0 1> | 321.6 |
C (mp-48) | <1 1 0> | <0 1 1> | 259.2 |
WSe2 (mp-1821) | <1 0 0> | <0 1 1> | 259.2 |
WSe2 (mp-1821) | <1 0 1> | <1 0 1> | 256.5 |
NaCl (mp-22862) | <1 0 0> | <0 0 1> | 160.8 |
NaCl (mp-22862) | <1 1 0> | <0 1 0> | 135.6 |
ZrO2 (mp-2858) | <0 1 0> | <0 0 1> | 321.6 |
ZrO2 (mp-2858) | <1 0 0> | <0 1 1> | 86.4 |
YAlO3 (mp-3792) | <0 0 1> | <1 0 1> | 256.5 |
TiO2 (mp-390) | <0 0 1> | <0 0 1> | 214.4 |
TiO2 (mp-390) | <1 0 0> | <0 0 1> | 107.2 |
TiO2 (mp-390) | <1 1 0> | <1 0 1> | 256.5 |
CsI (mp-614603) | <1 1 0> | <1 0 1> | 256.5 |
CsI (mp-614603) | <1 1 1> | <0 0 1> | 107.2 |
MgF2 (mp-1249) | <0 0 1> | <0 0 1> | 268.0 |
MgF2 (mp-1249) | <1 0 0> | <1 0 0> | 116.5 |
MgF2 (mp-1249) | <1 0 1> | <0 0 1> | 53.6 |
MgF2 (mp-1249) | <1 1 0> | <0 0 1> | 160.8 |
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 |
---|---|---|---|
Er2Ge5Rh3 (mp-984743) | 0.4410 | 0.000 | 3 |
La2Ge5Ru3 (mp-621852) | 0.2469 | 0.002 | 3 |
Y2Ge5Ru3 (mp-620812) | 0.2252 | 0.000 | 3 |
Sm2Ge5Ru3 (mp-754776) | 0.2207 | 0.000 | 3 |
Tb2Si5Ru3 (mp-16478) | 0.0607 | 0.000 | 3 |
Cs4Pb9 (mp-574070) | 0.7409 | 0.000 | 2 |
Mg2Si3 (mp-1073130) | 0.7417 | 0.333 | 2 |
K3Hg11 (mp-11028) | 0.7422 | 0.005 | 2 |
Ce2Si7 (mp-1079241) | 0.7288 | 0.074 | 2 |
Mg3Si4 (mp-1075031) | 0.7394 | 0.213 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Er_3 Si Ru_pv |
Final Energy/Atom-7.2564 eV |
Corrected Energy-145.1279 eV
-145.1279 eV = -145.1279 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)