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 OrderingAFM |
Formation Energy / Atom-2.100 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.048 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. |
Density4.06 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToTe2P2O9 + Ni2P2O7 |
Band Gap2.919 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 MauguinP21/m [11] |
Hall-P 2yb |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
Apply Gaussian smoothing:
Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 346.0 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 -1> | 209.8 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 314.6 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 1> | 219.7 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 -1> | 256.3 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 220.2 |
ZnSe (mp-1190) | <1 0 0> | <1 1 -1> | 256.3 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 346.0 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 251.7 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 1> | 293.0 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 1> | 219.7 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 343.5 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 257.3 |
CdS (mp-672) | <1 0 1> | <1 0 1> | 293.0 |
CdS (mp-672) | <1 1 1> | <1 1 -1> | 256.3 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 251.7 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 294.5 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 251.7 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 157.3 |
Te2W (mp-22693) | <1 0 0> | <1 0 0> | 193.0 |
YVO4 (mp-19133) | <1 0 0> | <0 0 1> | 94.4 |
YVO4 (mp-19133) | <1 0 1> | <0 0 1> | 283.1 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 64.3 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 125.8 |
TePb (mp-19717) | <1 1 0> | <1 0 1> | 293.0 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 196.3 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 31.5 |
AlN (mp-661) | <1 0 1> | <0 1 0> | 196.3 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 157.3 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 283.1 |
Ag (mp-124) | <1 0 0> | <1 1 0> | 242.7 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 291.5 |
GaAs (mp-2534) | <1 0 0> | <1 1 -1> | 256.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 1 0> | 343.5 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 283.1 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 157.3 |
BaF2 (mp-1029) | <1 1 0> | <1 0 -1> | 279.7 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 220.2 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 251.7 |
GaN (mp-804) | <1 0 1> | <0 1 0> | 245.4 |
GaN (mp-804) | <1 1 1> | <1 0 -1> | 279.7 |
BN (mp-984) | <0 0 1> | <0 1 1> | 233.2 |
BN (mp-984) | <1 0 0> | <1 1 1> | 176.3 |
BN (mp-984) | <1 0 1> | <0 0 1> | 157.3 |
BN (mp-984) | <1 1 0> | <1 1 -1> | 170.8 |
BN (mp-984) | <1 1 1> | <0 0 1> | 314.6 |
SiO2 (mp-6930) | <0 0 1> | <0 1 0> | 196.3 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 188.7 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 245.4 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 321.6 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
MnCrO4 (mp-780641) | 0.3374 | 0.104 | 3 |
FePO4 (mp-25001) | 0.3726 | 0.024 | 3 |
Mn3(P2O7)2 (mp-694554) | 0.3641 | 0.162 | 3 |
NiPO4 (mp-540008) | 0.3795 | 0.231 | 3 |
Ni2P3O10 (mp-25610) | 0.3729 | 0.052 | 3 |
Mn3Sn(PO4)4 (mp-775053) | 0.2383 | 0.019 | 4 |
MnNb(PO4)2 (mp-775045) | 0.2143 | 0.093 | 4 |
MnFe(PO4)2 (mp-764401) | 0.2418 | 0.011 | 4 |
CrSn(PO4)2 (mp-772477) | 0.2115 | 0.057 | 4 |
Mn3Ni(PO4)4 (mp-771982) | 0.2310 | 0.027 | 4 |
CrO2 (mvc-11581) | 0.7402 | 0.351 | 2 |
Cr5O12 (mp-19575) | 0.7354 | 0.142 | 2 |
VO2 (mvc-6918) | 0.7236 | 0.095 | 2 |
MoO2 (mvc-6944) | 0.7276 | 0.387 | 2 |
MnFeCo(PO4)3 (mp-764410) | 0.2553 | 0.027 | 5 |
MnFeCo(PO4)3 (mp-764392) | 0.2945 | 0.028 | 5 |
MnFeCo(PO4)3 (mp-763496) | 0.2796 | 0.026 | 5 |
MnFeCo(PO4)3 (mp-764415) | 0.2738 | 0.035 | 5 |
MnFeCo(PO4)3 (mp-763446) | 0.3137 | 0.033 | 5 |
Li4Mn3CrCo2(PO4)6 (mp-763479) | 0.6735 | 0.080 | 6 |
LiMgCr3Se2(SO6)4 (mp-769552) | 0.6242 | 0.003 | 6 |
Li4MnCr2Fe3(PO4)6 (mp-779026) | 0.7145 | 1.367 | 6 |
Li2Mg2MnFe(PO4)4 (mp-849669) | 0.6426 | 0.008 | 6 |
NaLiMn2Fe4(PO4)6 (mp-777193) | 0.6914 | 0.031 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesNi: 6.2 eV |
PseudopotentialsVASP PAW: Ni_pv Te P O |
Final Energy/Atom-6.3957 eV |
Corrected Energy-169.5707 eV
Uncorrected energy = -153.4967 eV
Composition-based energy adjustment (-0.687 eV/atom x 16.0 atoms) = -10.9920 eV
Composition-based energy adjustment (-2.541 eV/atom x 2.0 atoms) = -5.0820 eV
Corrected energy = -169.5707 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)