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-0.722 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.011 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 ToWSe2 + WS2 |
Band Gap0.643 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 MauguinP3m1 [156] |
HallP 3 2" |
Point Group3m |
Crystal Systemtrigonal |
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] |
---|---|---|---|
C (mp-48) | <0 0 1> | <0 0 1> | 37.4 |
C (mp-48) | <1 0 0> | <0 0 1> | 308.6 |
C (mp-48) | <1 0 1> | <0 0 1> | 159.0 |
C (mp-48) | <1 1 0> | <0 0 1> | 224.4 |
C (mp-48) | <1 1 1> | <0 0 1> | 346.0 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 177.7 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 233.8 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 112.2 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 252.5 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 224.4 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 327.3 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 327.3 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 149.6 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 168.3 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 318.0 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 177.7 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 196.4 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 65.5 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 65.5 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 299.3 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 140.3 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 327.3 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 299.3 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 299.3 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 289.9 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 93.5 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 364.7 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 224.4 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 56.1 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 261.9 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 65.5 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 168.3 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 224.4 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 177.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 177.7 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 112.2 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 28.1 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 252.5 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 177.7 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 215.1 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 261.9 |
CdWO4 (mp-19387) | <0 1 0> | <0 0 1> | 215.1 |
CdWO4 (mp-19387) | <0 1 1> | <0 0 1> | 233.8 |
CdWO4 (mp-19387) | <1 0 0> | <0 0 1> | 121.6 |
CdWO4 (mp-19387) | <1 1 0> | <0 0 1> | 299.3 |
CdWO4 (mp-19387) | <1 1 1> | <0 0 1> | 261.9 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 299.3 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 187.0 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 233.8 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 149.6 |
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 |
---|---|---|---|
WSeS (mp-1028663) | 0.0508 | 0.014 | 3 |
Mo2Se3S (mp-1026980) | 0.0192 | 0.011 | 3 |
MoSeS (mp-1026916) | 0.0466 | 0.014 | 3 |
Mo3(Se2S)2 (mp-1025819) | 0.0486 | 0.012 | 3 |
W3(Se2S)2 (mp-1025588) | 0.0402 | 0.013 | 3 |
MoW3(Se3S)2 (mp-1030567) | 0.0079 | 0.073 | 4 |
MoWSe3S (mp-1030519) | 0.0097 | 0.096 | 4 |
MoWSe3S (mp-1030513) | 0.0110 | 0.096 | 4 |
MoW3(Se3S)2 (mp-1028952) | 0.0097 | 0.073 | 4 |
MoWSe3S (mp-1027672) | 0.0110 | 0.096 | 4 |
Te2Mo (mp-1030319) | 0.1581 | 0.000 | 2 |
WSe2 (mp-1028698) | 0.1621 | 0.000 | 2 |
WS2 (mp-1028441) | 0.1607 | 0.001 | 2 |
Te2Mo (mp-1025576) | 0.1561 | 0.000 | 2 |
WSe2 (mp-1025572) | 0.1630 | 0.000 | 2 |
Te4Mo3W(SeS)2 (mp-1030450) | 0.1800 | 0.082 | 5 |
Te4Mo3W(SeS)2 (mp-1030404) | 0.1891 | 0.116 | 5 |
Te4Mo3W(SeS)2 (mp-1030284) | 0.1823 | 0.098 | 5 |
Te2MoWSeS (mp-1030176) | 0.1886 | 0.083 | 5 |
Te2MoWSeS (mp-1029213) | 0.1809 | 0.083 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: W_pv Se S |
Final Energy/Atom-7.3683 eV |
Corrected Energy-92.2582 eV
Uncorrected energy = -88.4202 eV
Composition-based energy adjustment (-0.503 eV/atom x 2.0 atoms) = -1.0060 eV
Composition-based energy adjustment (-0.472 eV/atom x 6.0 atoms) = -2.8320 eV
Corrected energy = -92.2582 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)