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-1.101 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.502 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. |
Density2.41 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCeSe2 |
Band Gap0.953 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 [5] |
HallC 2y |
Point Group2 |
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%)
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 |
---|---|---|---|
CoSiO4 (mp-633897) | 0.4540 | 0.356 | 3 |
BeCrO4 (mp-770887) | 0.3729 | 0.011 | 3 |
NiPO4 (mp-705637) | 0.4180 | 0.537 | 3 |
PNO (mp-36779) | 0.3625 | 0.015 | 3 |
CoPO4 (mp-704189) | 0.4618 | 0.196 | 3 |
Rb2Al2Si3O10 (mp-975622) | 0.5359 | 0.009 | 4 |
K2Be(Si2O5)2 (mp-557802) | 0.5861 | 0.000 | 4 |
KAlSi3O8 (mp-697670) | 0.6103 | 0.000 | 4 |
KSi2BO6 (mp-1019889) | 0.6357 | 0.000 | 4 |
K2Al2Si3O10 (mp-1019744) | 0.5330 | 0.018 | 4 |
SiO2 (mp-560152) | 0.2659 | 0.098 | 2 |
SiO2 (mp-556319) | 0.3415 | 0.122 | 2 |
CeSe2 (mp-1080370) | 0.2433 | 0.503 | 2 |
SiO2 (mp-557134) | 0.1725 | 0.085 | 2 |
CrN2 (mp-1096890) | 0.2578 | 0.461 | 2 |
KBaAl3Si5O16 (mp-677121) | 0.7129 | 0.009 | 5 |
RbZnB(PO4)2 (mp-557658) | 0.6163 | 0.000 | 5 |
CsZnB(PO4)2 (mp-560244) | 0.5820 | 0.000 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ce Se |
Final Energy/Atom-5.4092 eV |
Corrected Energy-64.9105 eV
-64.9105 eV = -64.9105 eV (uncorrected energy)
|
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)