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-3.459 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density5.94 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap3.005 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 [164] |
Hall-P 3 2" |
Point Group3m |
Crystal Systemtrigonal |
Topological Classificationtrivial*
|
SubclassificationLCEBR†
|
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.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 98.0 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 138.7 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 249.7 |
AlN (mp-661) | <1 1 0> | <1 0 1> | 248.6 |
AlN (mp-661) | <1 1 1> | <1 0 1> | 248.6 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 333.0 |
GaN (mp-804) | <1 0 0> | <1 0 1> | 248.6 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 210.0 |
SiO2 (mp-6930) | <1 0 0> | <1 0 1> | 248.6 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 249.7 |
KCl (mp-23193) | <1 0 0> | <1 1 1> | 200.2 |
KCl (mp-23193) | <1 1 1> | <1 0 0> | 222.0 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 222.0 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 1> | 250.3 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 222.0 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 333.0 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 0> | 288.4 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 0> | 240.3 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 98.0 |
CeO2 (mp-20194) | <1 0 0> | <1 1 0> | 240.3 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 1> | 279.7 |
InAs (mp-20305) | <1 0 0> | <1 1 0> | 192.2 |
CeO2 (mp-20194) | <1 1 0> | <1 0 1> | 341.9 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 166.5 |
GaAs (mp-2534) | <1 1 1> | <1 0 0> | 55.5 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 210.0 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 266.0 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 166.5 |
ZnSe (mp-1190) | <1 1 0> | <1 0 0> | 333.0 |
ZnSe (mp-1190) | <1 1 1> | <1 0 0> | 55.5 |
BaF2 (mp-1029) | <1 0 0> | <1 1 0> | 192.2 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 266.0 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 83.2 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 112.0 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 266.0 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 166.5 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 294.0 |
GaN (mp-804) | <1 1 1> | <1 1 0> | 240.3 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 182.0 |
CdS (mp-672) | <1 0 0> | <1 1 0> | 144.2 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 222.0 |
SiO2 (mp-6930) | <0 0 1> | <1 0 1> | 217.5 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 249.7 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 83.2 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 138.7 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 194.2 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 266.0 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 210.0 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 266.0 |
GaSe (mp-1943) | <1 0 0> | <1 0 1> | 279.7 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
170 | 73 | 64 | 1 | 0 | 0 |
73 | 170 | 64 | -1 | 0 | 0 |
64 | 64 | 157 | 0 | 0 | 0 |
1 | -1 | 0 | 62 | 0 | 0 |
0 | 0 | 0 | 0 | 62 | 1 |
0 | 0 | 0 | 0 | 1 | 48 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
7.8 | -2.6 | -2.2 | -0.2 | 0 | 0 |
-2.6 | 7.8 | -2.2 | 0.2 | 0 | 0 |
-2.2 | -2.2 | 8.2 | 0 | 0 | 0 |
-0.2 | 0.2 | 0 | 16.2 | 0 | 0 |
0 | 0 | 0 | 0 | 16.2 | -0.4 |
0 | 0 | 0 | 0 | -0.4 | 20.8 |
Shear Modulus GV54 GPa |
Bulk Modulus KV100 GPa |
Shear Modulus GR53 GPa |
Bulk Modulus KR100 GPa |
Shear Modulus GVRH53 GPa |
Bulk Modulus KVRH100 GPa |
Elastic Anisotropy0.08 |
Poisson's Ratio0.27 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Nd2SO2 (mp-3211) | 0.0105 | 0.000 | 3 |
Ce2SO2 (mp-3972) | 0.0221 | 0.000 | 3 |
U2PN2 (mp-5381) | 0.0199 | 0.000 | 3 |
Sm2SO2 (mp-5598) | 0.0278 | 0.000 | 3 |
La2SO2 (mp-4511) | 0.0213 | 0.000 | 3 |
Li6Mn(FeO3)2 (mp-764386) | 0.5900 | 0.040 | 4 |
KLiMnO2 (mp-770699) | 0.7491 | 0.027 | 4 |
Na2Li3CoO4 (mp-540990) | 0.6664 | 0.075 | 4 |
LiCaGaN2 (mp-570948) | 0.6490 | 0.000 | 4 |
LiFeCuS2 (mp-755288) | 0.5480 | 0.262 | 4 |
Sm2O3 (mp-10733) | 0.4176 | 0.062 | 2 |
Pr2O3 (mp-2063) | 0.4137 | 0.026 | 2 |
Nd2O3 (mp-2763) | 0.4144 | 0.030 | 2 |
Ac2O3 (mp-11107) | 0.4163 | 0.000 | 2 |
Th2N3 (mp-1940) | 0.4018 | 0.118 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Pr_3 S O |
Final Energy/Atom-7.7646 eV |
Corrected Energy-40.7000 eV
Uncorrected energy = -38.8230 eV
Composition-based energy adjustment (-0.503 eV/atom x 1.0 atoms) = -0.5030 eV
Composition-based energy adjustment (-0.687 eV/atom x 2.0 atoms) = -1.3740 eV
Corrected energy = -40.7000 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)