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-1.783 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.180 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. |
Density2.42 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCS14 + CsCOF3 + CsSO3F + CO2 + CF4 + N2 |
Band Gap6.237 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 MauguinC2/c [15] |
Hall-C 2yc |
Point Group2/m |
Crystal Systemmonoclinic |
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] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <1 0 0> | 295.6 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 197.1 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 98.5 |
LiNbO3 (mp-3731) | <1 0 0> | <1 0 0> | 295.6 |
LiTaO3 (mp-3666) | <1 0 0> | <1 0 0> | 295.6 |
KP(HO2)2 (mp-23959) | <0 0 1> | <1 0 0> | 295.6 |
Ni (mp-23) | <1 0 0> | <1 0 0> | 98.5 |
PbSe (mp-2201) | <1 0 0> | <1 0 0> | 197.1 |
CdSe (mp-2691) | <1 0 0> | <1 0 0> | 197.1 |
ZrO2 (mp-2858) | <1 0 -1> | <1 0 0> | 295.6 |
GaSb (mp-1156) | <1 0 0> | <1 0 0> | 197.1 |
Cu (mp-30) | <1 1 0> | <1 0 0> | 295.6 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 295.6 |
Al2O3 (mp-1143) | <1 0 1> | <1 0 0> | 197.1 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 197.1 |
Ni (mp-23) | <1 1 0> | <1 0 0> | 295.6 |
MgF2 (mp-1249) | <0 0 1> | <1 0 0> | 197.1 |
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Rb2S2O7 (mp-752728) | 0.5574 | 0.004 | 3 |
Rb2S2O7 (mp-770773) | 0.5875 | 0.000 | 3 |
S2O5F2 (mp-28676) | 0.6049 | 0.000 | 3 |
Te(S2O7)2 (mp-752443) | 0.6101 | 0.000 | 3 |
K2S5O16 (mp-27792) | 0.6397 | 0.000 | 3 |
PBrNF (mp-559366) | 0.6751 | 0.014 | 4 |
PNClF (mp-554472) | 0.6703 | 0.008 | 4 |
K2P2O5F2 (mp-558480) | 0.6733 | 0.000 | 4 |
K2CrSO7 (mp-565687) | 0.6276 | 0.000 | 4 |
SNClO (mp-667281) | 0.6978 | 0.292 | 4 |
Cl2O7 (mp-31050) | 0.6738 | 0.000 | 2 |
Mn2O7 (mp-554850) | 0.6859 | 0.318 | 2 |
SeO3 (mp-27519) | 0.6861 | 0.018 | 2 |
Re2O7 (mvc-7040) | 0.6537 | 0.039 | 2 |
SO3 (mp-2414) | 0.6986 | 0.000 | 2 |
KS2N(O2F)2 (mp-652068) | 0.5882 | 0.059 | 5 |
RbSi2H18C6N (mp-567899) | 0.5724 | 0.022 | 5 |
PSN(Cl2O)2 (mp-557775) | 0.4662 | 0.125 | 5 |
C2SeS2O7F6 (mp-557877) | 0.5553 | 0.233 | 5 |
CSCl(OF)3 (mp-558648) | 0.5842 | 0.080 | 5 |
H10C5S2N2(O2F3)2 (mp-708184) | 0.4200 | 0.311 | 6 |
LiC2S2N(O2F3)2 (mp-557395) | 0.5890 | 0.216 | 6 |
RbC2S2N(OF)4 (mp-559029) | 0.6515 | 0.250 | 6 |
KC2S2N(O2F3)2 (mp-6902) | 0.4419 | 0.184 | 6 |
VP2C4N3(ClF6)2 (mp-693133) | 0.5718 | 0.479 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Cs_sv C S N O F |
Final Energy/Atom-5.5172 eV |
Corrected Energy-369.6439 eV
-369.6439 eV = -353.0996 eV (uncorrected energy) - 16.5443 eV (MP Anion Correction)
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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)