Final Magnetic Moment0.008 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-0.810 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.004 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. |
Density7.62 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToTaSe2 |
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 MauguinP63/mmc [194] |
Hall-P 6c 2c |
Point Group6/mmm |
Crystal Systemhexagonal |
Topological ClassificationSM*
|
SubclassificationESFD†
|
Crossing TypePoint
|
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) | <1 0 0> | <1 0 1> | 250.8 |
C (mp-48) | <1 1 0> | <0 0 1> | 324.3 |
C (mp-48) | <1 1 1> | <0 0 1> | 303.4 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 73.2 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 282.5 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 240.6 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 282.5 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 198.8 |
C (mp-48) | <0 0 1> | <0 0 1> | 136.0 |
C (mp-48) | <1 0 1> | <0 0 1> | 292.9 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 73.2 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 261.5 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 125.5 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 177.8 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 167.4 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 196.2 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 282.5 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 198.8 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 198.8 |
SiO2 (mp-6930) | <1 0 0> | <1 0 1> | 301.0 |
SiO2 (mp-6930) | <1 0 1> | <1 0 1> | 250.8 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 196.2 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 292.9 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 73.2 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 292.9 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 261.5 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 245.3 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 188.3 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 198.8 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 198.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 1> | 200.7 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 198.8 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 104.6 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 251.1 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 167.4 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 196.2 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 272.0 |
Te2W (mp-22693) | <0 1 1> | <0 0 1> | 292.9 |
CdWO4 (mp-19387) | <0 0 1> | <0 0 1> | 209.2 |
CdWO4 (mp-19387) | <0 1 0> | <0 0 1> | 324.3 |
CdWO4 (mp-19387) | <0 1 1> | <1 0 0> | 245.3 |
CdWO4 (mp-19387) | <1 0 0> | <1 1 0> | 254.9 |
CdWO4 (mp-19387) | <1 0 1> | <0 0 1> | 313.8 |
CdWO4 (mp-19387) | <1 1 0> | <0 0 1> | 240.6 |
CdWO4 (mp-19387) | <1 1 1> | <0 0 1> | 324.3 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 219.7 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 73.2 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 10.5 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 272.0 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 282.5 |
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 |
---|---|---|---|
MoWS4 (mp-1030119) | 0.3381 | 0.002 | 3 |
MoW3S8 (mp-1029246) | 0.3389 | 0.002 | 3 |
MoWS4 (mp-1027335) | 0.3427 | 0.002 | 3 |
MoW3S8 (mp-1027273) | 0.3427 | 0.002 | 3 |
Mo3WS8 (mp-1027569) | 0.3417 | 0.002 | 3 |
MoWSe3S (mp-1030535) | 0.3532 | 0.113 | 4 |
Mo3W(SeS)4 (mp-1026927) | 0.3518 | 0.059 | 4 |
Mo3W(Se3S)2 (mp-1027729) | 0.3505 | 0.056 | 4 |
Mo3W(Se3S)2 (mp-1080150) | 0.3511 | 0.073 | 4 |
MoW(SeS)2 (mp-1080170) | 0.3469 | 0.060 | 4 |
NbSe2 (mp-7597) | 0.0640 | 0.001 | 2 |
TaSe2 (mp-7926) | 0.0578 | 0.004 | 2 |
NbSe2 (mp-571133) | 0.0299 | 0.000 | 2 |
TaSe2 (mp-7834) | 0.0224 | 0.000 | 2 |
MoS2 (mp-1434) | 0.0711 | 0.000 | 2 |
Te4Mo3W(SeS)2 (mp-1030450) | 0.4578 | 0.082 | 5 |
Te4Mo3W(SeS)2 (mp-1030404) | 0.4652 | 0.116 | 5 |
Te4Mo3W(SeS)2 (mp-1030284) | 0.4597 | 0.098 | 5 |
Te2MoWSeS (mp-1029213) | 0.4594 | 0.083 | 5 |
Te4MoW3(SeS)2 (mp-1028626) | 0.4648 | 0.111 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ta_pv Se |
Final Energy/Atom-7.0931 eV |
Corrected Energy-44.4468 eV
Uncorrected energy = -42.5588 eV
Composition-based energy adjustment (-0.472 eV/atom x 4.0 atoms) = -1.8880 eV
Corrected energy = -44.4468 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)