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 / Atom0.083 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.186 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. |
Density6.69 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToInSb |
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 MauguinPmm2 [25] |
HallP 2 2 |
Point Groupmm2 |
Crystal Systemorthorhombic |
Topological Classificationtrivial*
|
SubclassificationLCEBR†
|
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> | 200.5 |
LaAlO3 (mp-2920) | <1 0 0> | <1 0 1> | 279.9 |
LaAlO3 (mp-2920) | <1 0 1> | <1 1 1> | 313.7 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 241.8 |
LaAlO3 (mp-2920) | <1 1 1> | <1 1 1> | 256.6 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 66.8 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 47.7 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 105.0 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 248.3 |
AlN (mp-661) | <1 1 1> | <0 1 1> | 209.9 |
CeO2 (mp-20194) | <1 0 0> | <0 1 0> | 149.6 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 80.6 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 162.3 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 295.6 |
GaAs (mp-2534) | <1 1 1> | <0 1 1> | 167.9 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 38.6 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 53.7 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 143.2 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 85.9 |
GaN (mp-804) | <1 0 0> | <1 0 1> | 64.6 |
GaN (mp-804) | <1 0 1> | <1 1 0> | 134.3 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 181.4 |
GaN (mp-804) | <1 1 1> | <0 1 0> | 149.6 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 181.4 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 181.4 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 1> | 167.9 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 317.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 270.2 |
DyScO3 (mp-31120) | <1 1 0> | <0 1 0> | 243.0 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 219.6 |
InAs (mp-20305) | <1 0 0> | <0 1 0> | 37.4 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 53.7 |
InAs (mp-20305) | <1 1 1> | <1 1 0> | 322.4 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 107.5 |
SiO2 (mp-6930) | <1 0 0> | <0 1 1> | 84.0 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 107.5 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 296.0 |
SiO2 (mp-6930) | <1 1 1> | <1 1 0> | 53.7 |
KCl (mp-23193) | <1 0 0> | <1 1 1> | 85.5 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 57.3 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 143.2 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 162.3 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 295.6 |
ZnSe (mp-1190) | <1 1 1> | <0 1 1> | 167.9 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 0> | 149.6 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 154.4 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 86.1 |
CdS (mp-672) | <1 1 0> | <0 1 1> | 146.9 |
CdS (mp-672) | <1 1 1> | <1 1 1> | 256.6 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 181.4 |
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 |
---|---|---|---|
AgCl (mp-570687) | 0.6267 | 0.011 | 2 |
VN (mvc-13303) | 0.6282 | 0.183 | 2 |
AgI (mp-568927) | 0.5134 | 0.103 | 2 |
KAs (mp-1078831) | 0.7071 | 0.964 | 2 |
Bi (mp-567379) | 0.4980 | 0.059 | 1 |
Bi (mp-1096851) | 0.4578 | 0.095 | 1 |
Explore more synthesis descriptions for materials of composition InSb.
Text computed by synthesisproject.org.
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: In_d Sb |
Final Energy/Atom-3.3571 eV |
Corrected Energy-6.7142 eV
-6.7142 eV = -6.7142 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)