Final Magnetic Moment0.020 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-1.575 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.088 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. |
Density6.44 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi35(RuO4)12 + Ru + RuO2 |
Band Gap0.000 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 MauguinPnnm [58] |
Hall-P 2 2n |
Point Groupmmm |
Crystal Systemorthorhombic |
Topological ClassificationSM*
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SubclassificationESFD†
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Crossing TypePoint
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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.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 1 1> | 80.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 112.0 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 224.0 |
LaAlO3 (mp-2920) | <1 0 1> | <0 1 1> | 80.2 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 77.7 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 118.4 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 28.0 |
AlN (mp-661) | <1 1 1> | <0 1 1> | 200.6 |
CeO2 (mp-20194) | <1 1 0> | <1 0 1> | 206.1 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 233.0 |
CeO2 (mp-20194) | <1 1 1> | <1 0 1> | 206.1 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 140.0 |
GaAs (mp-2534) | <1 0 0> | <1 0 1> | 206.1 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 280.0 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 28.7 |
BaF2 (mp-1029) | <1 1 0> | <0 1 1> | 280.9 |
BaF2 (mp-1029) | <1 1 1> | <1 0 1> | 264.9 |
GaN (mp-804) | <0 0 1> | <0 1 1> | 80.2 |
GaN (mp-804) | <1 0 0> | <0 1 0> | 100.6 |
GaN (mp-804) | <1 0 1> | <0 1 0> | 129.3 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 181.3 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 70.0 |
SiO2 (mp-6930) | <1 1 1> | <0 1 0> | 158.0 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 280.0 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 233.0 |
SiO2 (mp-6930) | <0 0 1> | <1 0 1> | 88.3 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 28.0 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 143.7 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 56.0 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 182.0 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 229.3 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 129.3 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 224.0 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 129.5 |
DyScO3 (mp-31120) | <1 1 1> | <0 1 1> | 140.4 |
InAs (mp-20305) | <1 0 0> | <1 1 1> | 229.3 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 210.0 |
InAs (mp-20305) | <1 1 1> | <1 0 1> | 264.9 |
ZnSe (mp-1190) | <1 0 0> | <1 0 1> | 206.1 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 140.0 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 112.0 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 1> | 80.2 |
CdS (mp-672) | <1 0 0> | <0 1 1> | 200.6 |
CdS (mp-672) | <1 0 1> | <0 0 1> | 126.0 |
CdS (mp-672) | <1 1 0> | <0 1 1> | 100.3 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 196.5 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 210.0 |
Te2W (mp-22693) | <1 1 0> | <0 1 1> | 220.7 |
YVO4 (mp-19133) | <1 0 1> | <0 1 1> | 140.4 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 196.0 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
290 | 151 | 101 | 0 | 0 | 0 |
151 | 418 | 119 | 0 | 0 | 0 |
101 | 119 | 351 | 0 | 0 | 0 |
0 | 0 | 0 | 82 | 0 | 0 |
0 | 0 | 0 | 0 | 101 | 0 |
0 | 0 | 0 | 0 | 0 | 143 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
4.4 | -1.4 | -0.8 | 0 | 0 | 0 |
-1.4 | 3.1 | -0.6 | 0 | 0 | 0 |
-0.8 | -0.6 | 3.3 | 0 | 0 | 0 |
0 | 0 | 0 | 12.1 | 0 | 0 |
0 | 0 | 0 | 0 | 9.9 | 0 |
0 | 0 | 0 | 0 | 0 | 7 |
Shear Modulus GV111 GPa |
Bulk Modulus KV200 GPa |
Shear Modulus GR106 GPa |
Bulk Modulus KR194 GPa |
Shear Modulus GVRH109 GPa |
Bulk Modulus KVRH197 GPa |
Elastic Anisotropy0.28 |
Poisson's Ratio0.27 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Mn2SbTe (mp-675433) | 0.2101 | 0.268 | 3 |
MnMoN2 (mp-9374) | 0.3120 | 0.000 | 3 |
CdInS2 (mp-20519) | 0.2511 | 0.190 | 3 |
LiTiS2 (mp-9615) | 0.2089 | 0.000 | 3 |
LiZrSe2 (mp-1001615) | 0.1933 | 0.000 | 3 |
Li8Cr(FeO4)3 (mp-767681) | 0.5271 | 1.300 | 4 |
Li8Mn(FeO4)3 (mp-766973) | 0.5347 | 0.073 | 4 |
Na2Li(NiO2)3 (mp-773956) | 0.5506 | 0.031 | 4 |
Li3Ti2CoO6 (mp-769994) | 0.5412 | 0.088 | 4 |
Li8Mn3CrO12 (mp-765119) | 0.5421 | 0.107 | 4 |
VH (mp-1017530) | 0.1647 | 0.285 | 2 |
TiSb (mp-569640) | 0.1712 | 0.289 | 2 |
ScC (mp-999203) | 0.1712 | 0.600 | 2 |
TiH (mp-998969) | 0.1627 | 0.228 | 2 |
FeN (mp-12120) | 0.1626 | 0.190 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.5972 | 0.005 | 5 |
Na (mp-999501) | 0.1987 | 0.116 | 1 |
Xe (mp-979286) | 0.6173 | 0.006 | 1 |
Sb (mp-632286) | 0.5892 | 0.059 | 1 |
Bi (mp-567379) | 0.5516 | 0.062 | 1 |
Te (mp-570459) | 0.5795 | 0.044 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv Ru_pv O |
Final Energy/Atom-6.4938 eV |
Corrected Energy-54.7594 eV
-54.7594 eV = -51.9502 eV (uncorrected energy) - 2.8092 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)