Final Magnetic Moment0.006 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-0.523 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.334 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. |
Density4.20 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCs2Mn3Se4 + Cs2Se |
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 ClassificationSM*
|
SubclassificationESFD†
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Crossing TypePoint
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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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 0 1> | 209.0 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 156.8 |
CdS (mp-672) | <1 0 0> | <0 1 0> | 198.0 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 313.6 |
AlN (mp-661) | <1 1 0> | <1 0 1> | 244.5 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 209.0 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 198.0 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 313.6 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 261.3 |
Te2W (mp-22693) | <0 1 1> | <0 1 1> | 111.9 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 148.4 |
CdS (mp-672) | <1 1 0> | <0 1 0> | 99.0 |
BN (mp-984) | <1 0 0> | <0 0 1> | 156.8 |
LiNbO3 (mp-3731) | <1 0 1> | <1 0 0> | 221.1 |
LiGaO2 (mp-5854) | <1 1 0> | <1 0 1> | 244.5 |
BN (mp-984) | <0 0 1> | <0 0 1> | 261.3 |
BN (mp-984) | <1 0 1> | <1 0 1> | 122.3 |
BN (mp-984) | <1 1 0> | <0 0 1> | 261.3 |
LiNbO3 (mp-3731) | <1 0 0> | <1 1 0> | 148.4 |
Al (mp-134) | <1 1 0> | <0 0 1> | 209.0 |
TeO2 (mp-2125) | <0 1 1> | <0 1 1> | 223.9 |
SiC (mp-7631) | <1 1 0> | <1 0 1> | 244.5 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 221.1 |
TiO2 (mp-2657) | <0 0 1> | <0 0 1> | 261.3 |
TiO2 (mp-2657) | <1 0 0> | <0 0 1> | 209.0 |
LiTaO3 (mp-3666) | <1 0 0> | <0 0 1> | 209.0 |
LiTaO3 (mp-3666) | <1 0 1> | <1 0 0> | 221.1 |
PbS (mp-21276) | <1 1 0> | <1 1 0> | 148.4 |
Ni (mp-23) | <1 0 0> | <1 0 1> | 122.3 |
Ni (mp-23) | <1 1 0> | <0 1 0> | 297.0 |
BaTiO3 (mp-5986) | <1 0 1> | <0 0 1> | 313.6 |
BaTiO3 (mp-5986) | <1 1 0> | <0 0 1> | 209.0 |
NdGaO3 (mp-3196) | <0 1 0> | <0 0 1> | 209.0 |
NdGaO3 (mp-3196) | <1 0 0> | <0 0 1> | 209.0 |
NdGaO3 (mp-3196) | <1 1 1> | <0 0 1> | 261.3 |
Au (mp-81) | <1 1 0> | <1 1 0> | 148.4 |
C (mp-48) | <1 1 0> | <0 0 1> | 261.3 |
ZrO2 (mp-2858) | <1 1 -1> | <0 0 1> | 313.6 |
Ge(Bi3O5)4 (mp-23352) | <1 1 0> | <1 1 0> | 148.4 |
SiC (mp-8062) | <1 1 0> | <1 0 1> | 244.5 |
TiO2 (mp-390) | <0 0 1> | <1 0 1> | 244.5 |
TiO2 (mp-390) | <1 0 1> | <0 0 1> | 156.8 |
CsI (mp-614603) | <1 1 0> | <0 0 1> | 261.3 |
MgF2 (mp-1249) | <0 0 1> | <0 1 0> | 198.0 |
ZnO (mp-2133) | <1 1 1> | <0 0 1> | 156.8 |
Cu (mp-30) | <1 1 0> | <1 1 0> | 148.4 |
LiAlO2 (mp-3427) | <0 0 1> | <1 0 1> | 244.5 |
CaF2 (mp-2741) | <1 0 0> | <1 0 1> | 122.3 |
CaF2 (mp-2741) | <1 1 0> | <0 0 1> | 209.0 |
Fe2O3 (mp-24972) | <1 0 1> | <1 0 0> | 221.1 |
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 |
---|---|---|---|
Rb2CoS2 (mp-558919) | 0.1418 | 0.135 | 3 |
Cs2SnAs2 (mp-8934) | 0.1375 | 0.000 | 3 |
Cs2MnTe2 (mp-610744) | 0.1555 | 0.000 | 3 |
Rb2CoS2 (mp-8766) | 0.1296 | 0.135 | 3 |
Cs2MnS2 (mp-561813) | 0.1580 | 0.000 | 3 |
Rb2VAgS4 (mp-8901) | 0.6600 | 0.000 | 4 |
K2VAgS4 (mp-8900) | 0.6562 | 0.000 | 4 |
Rb2LiVS4 (mp-558815) | 0.6162 | 0.000 | 4 |
K2TaAgS4 (mp-15216) | 0.6657 | 0.000 | 4 |
Ag2IOF (mp-1079461) | 0.6405 | 0.604 | 4 |
Run TypeGGA |
Energy Cutoff700 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Cs_sv Mn_pv Se |
Final Energy/Atom-4.1118 eV |
Corrected Energy-43.0059 eV
Uncorrected energy = -41.1179 eV
Composition-based energy adjustment (-0.472 eV/atom x 4.0 atoms) = -1.8880 eV
Corrected energy = -43.0059 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)