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-0.936 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.076 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. |
Density4.93 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToWS2 + MoWSe4 + MoS2 |
Band Gap0.596 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> | 36.7 |
C (mp-48) | <1 0 0> | <0 0 1> | 293.3 |
C (mp-48) | <1 0 1> | <0 0 1> | 183.3 |
C (mp-48) | <1 1 0> | <0 0 1> | 265.8 |
C (mp-48) | <1 1 1> | <0 0 1> | 320.8 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 174.2 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 229.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 110.0 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 247.5 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 256.7 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 256.7 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 366.7 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 91.7 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 128.3 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 146.7 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 165.0 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 311.7 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 174.2 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 320.8 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 284.2 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 64.2 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 201.7 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 137.5 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 146.7 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 320.8 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 293.3 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 293.3 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 284.2 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 91.7 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 357.5 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 220.0 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 55.0 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 192.5 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 64.2 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 165.0 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 311.7 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 174.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 82.5 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 201.7 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 27.5 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 320.8 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 247.5 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 64.2 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 256.7 |
Te2W (mp-22693) | <1 0 0> | <0 0 1> | 293.3 |
Te2W (mp-22693) | <1 1 1> | <0 0 1> | 229.2 |
CdWO4 (mp-19387) | <0 0 1> | <0 0 1> | 357.5 |
CdWO4 (mp-19387) | <0 1 0> | <0 0 1> | 210.8 |
CdWO4 (mp-19387) | <0 1 1> | <0 0 1> | 275.0 |
CdWO4 (mp-19387) | <1 0 0> | <0 0 1> | 119.2 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
W2Se3S (mp-1028686) | 0.0501 | 0.011 | 3 |
WSeS (mp-1028663) | 0.0079 | 0.014 | 3 |
MoSeS (mp-1026916) | 0.0172 | 0.014 | 3 |
Mo3(Se2S)2 (mp-1025819) | 0.0537 | 0.012 | 3 |
W3(Se2S)2 (mp-1025588) | 0.0368 | 0.013 | 3 |
MoW3(SeS)4 (mp-1030536) | 0.0142 | 0.076 | 4 |
MoW3(SeS)4 (mp-1028855) | 0.0079 | 0.093 | 4 |
Mo3W(SeS)4 (mp-1026927) | 0.0112 | 0.059 | 4 |
Mo3W(SeS)4 (mp-1026909) | 0.0095 | 0.076 | 4 |
MoW(SeS)2 (mp-1030742) | 0.0060 | 0.076 | 4 |
Te2Mo (mp-1030319) | 0.1561 | 0.000 | 2 |
WSe2 (mp-1028698) | 0.1516 | 0.000 | 2 |
Te2Mo (mp-1025576) | 0.1513 | 0.000 | 2 |
WSe2 (mp-1025572) | 0.1505 | 0.000 | 2 |
Te2Mo (mp-1023938) | 0.1540 | 0.001 | 2 |
Te4Mo3W(SeS)2 (mp-1030450) | 0.1785 | 0.082 | 5 |
Te4Mo3W(SeS)2 (mp-1030284) | 0.1823 | 0.098 | 5 |
Te2MoWSeS (mp-1029213) | 0.1794 | 0.083 | 5 |
Te2MoWSeS (mp-1029154) | 0.1871 | 0.104 | 5 |
Te4MoW3(SeS)2 (mp-1028626) | 0.1870 | 0.111 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mo_pv W_pv Se S |
Final Energy/Atom-7.2263 eV |
Corrected Energy-90.6156 eV
Uncorrected energy = -86.7156 eV
Composition-based energy adjustment (-0.503 eV/atom x 4.0 atoms) = -2.0120 eV
Composition-based energy adjustment (-0.472 eV/atom x 4.0 atoms) = -1.8880 eV
Corrected energy = -90.6156 eV
|
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)