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-1.766 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.124 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. |
Density6.04 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToSn5O6 + ZnO + SnO2 |
Band Gap1.233 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 MauguinImma [74] |
Hall-I 2b 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
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> | <1 1 0> | 255.2 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 255.2 |
LaAlO3 (mp-2920) | <1 1 1> | <1 1 0> | 255.2 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 72.8 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 318.0 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 227.2 |
BaF2 (mp-1029) | <1 1 0> | <0 1 0> | 56.9 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 136.3 |
GaN (mp-804) | <1 1 0> | <1 0 1> | 233.4 |
SiO2 (mp-6930) | <1 1 1> | <1 0 0> | 315.9 |
KCl (mp-23193) | <1 1 0> | <0 1 0> | 56.9 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 341.7 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 136.3 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 170.1 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 1> | 218.5 |
CdS (mp-672) | <1 0 0> | <1 1 1> | 289.3 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 189.5 |
CdS (mp-672) | <1 1 1> | <1 0 1> | 155.6 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 45.4 |
Te2W (mp-22693) | <0 1 1> | <1 0 1> | 233.4 |
Te2W (mp-22693) | <1 0 0> | <0 1 1> | 291.4 |
YVO4 (mp-19133) | <0 0 1> | <1 0 1> | 155.6 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 181.7 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 227.2 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 318.0 |
Ag (mp-124) | <1 1 0> | <0 1 0> | 227.8 |
LaAlO3 (mp-2920) | <1 0 0> | <1 1 1> | 289.3 |
BN (mp-984) | <0 0 1> | <0 0 1> | 227.2 |
BN (mp-984) | <1 0 1> | <0 1 0> | 341.7 |
BN (mp-984) | <1 1 0> | <0 1 1> | 291.4 |
LiNbO3 (mp-3731) | <0 0 1> | <1 0 0> | 189.5 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 1 0> | 227.8 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 136.3 |
AlN (mp-661) | <1 0 0> | <0 1 1> | 218.5 |
CeO2 (mp-20194) | <1 0 0> | <1 0 1> | 233.4 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 284.7 |
MoS2 (mp-1434) | <0 0 1> | <0 1 0> | 284.7 |
LiGaO2 (mp-5854) | <1 0 0> | <0 0 1> | 136.3 |
LiGaO2 (mp-5854) | <1 1 0> | <0 1 1> | 145.7 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 284.7 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 227.2 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 252.7 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 181.7 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 341.7 |
KCl (mp-23193) | <1 0 0> | <0 1 0> | 284.7 |
KCl (mp-23193) | <1 1 1> | <0 1 0> | 284.7 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 255.2 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 1> | 218.5 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 315.9 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 318.0 |
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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Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
6.44 | 0.00 | 0.00 |
0.00 | 6.64 | 0.00 |
0.00 | 0.00 | 7.07 |
Dielectric Tensor εij (total) |
||
---|---|---|
14.60 | 0.00 | -0.00 |
0.00 | 15.36 | 0.00 |
-0.00 | 0.00 | 23.22 |
Polycrystalline dielectric constant
εpoly∞
6.72
|
Polycrystalline dielectric constant
εpoly
17.73
|
Refractive Index n2.59 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Ca(SnO2)2 (mvc-6576) | 0.3681 | 0.069 | 3 |
CaMn2O4 (mvc-6953) | 0.3772 | 0.336 | 3 |
Mg(SnO2)2 (mvc-6497) | 0.1525 | 0.109 | 3 |
AlSiP3 (mp-5168) | 0.3758 | 0.014 | 3 |
Li2VSi3O8 (mp-767616) | 0.3319 | 0.092 | 4 |
LiMnSbO4 (mp-773720) | 0.3408 | 0.024 | 4 |
LiCrSiO4 (mp-765908) | 0.3351 | 0.054 | 4 |
LiVSiO4 (mp-761613) | 0.3585 | 0.066 | 4 |
Li2Si3NiO8 (mp-767953) | 0.3413 | 0.076 | 4 |
NiP4 (mp-770274) | 0.4085 | 0.087 | 2 |
P4Ru (mp-27173) | 0.3973 | 0.000 | 2 |
NiP4 (mp-769108) | 0.3794 | 0.078 | 2 |
P4Ru (mp-1080439) | 0.3608 | 0.016 | 2 |
P4Os (mp-1087509) | 0.3724 | 0.016 | 2 |
Li4V2Cr3Sb3O16 (mp-775451) | 0.4713 | 0.096 | 5 |
Li4Fe3Co2Ni3O16 (mp-766922) | 0.4786 | 0.284 | 5 |
Li4Ti3Mn3(NiO8)2 (mp-770507) | 0.4804 | 0.061 | 5 |
Li4Fe3Co2Cu3O16 (mp-763163) | 0.4603 | 0.088 | 5 |
Li4Mn3V3(WO8)2 (mp-763077) | 0.4534 | 0.273 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Zn Sn_d O |
Final Energy/Atom-5.5180 eV |
Corrected Energy-82.8701 eV
-82.8701 eV = -77.2518 eV (uncorrected energy) - 5.6183 eV (MP Anion Correction)
|
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)