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-0.670 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.020 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. |
Density8.78 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToNdInRh + NdRh |
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 MauguinP4/mbm [127] |
Hall-P 4 2ab |
Point Group4/mmm |
Crystal Systemtetragonal |
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.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 1 0> | 300.7 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 287.8 |
LaAlO3 (mp-2920) | <1 0 1> | <1 1 0> | 300.7 |
AlN (mp-661) | <0 0 1> | <1 0 1> | 260.3 |
AlN (mp-661) | <1 0 0> | <1 1 0> | 171.8 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 214.8 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 57.6 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 121.5 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 171.8 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 151.9 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 300.7 |
SiO2 (mp-6930) | <1 0 0> | <1 0 1> | 195.2 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 287.8 |
SiO2 (mp-6930) | <1 1 1> | <1 0 1> | 325.4 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 300.7 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 172.7 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 1> | 325.4 |
InAs (mp-20305) | <1 1 0> | <1 0 1> | 260.3 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 287.8 |
ZnSe (mp-1190) | <1 1 0> | <1 0 1> | 325.4 |
AlN (mp-661) | <1 0 1> | <1 0 1> | 325.4 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 287.8 |
GaAs (mp-2534) | <1 1 0> | <1 0 1> | 325.4 |
KTaO3 (mp-3614) | <1 0 0> | <1 1 0> | 128.9 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 171.8 |
CdS (mp-672) | <1 1 1> | <1 1 0> | 257.7 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 182.2 |
LiF (mp-1138) | <1 1 1> | <1 0 1> | 260.3 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 151.9 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 273.4 |
GaN (mp-804) | <1 1 1> | <1 1 1> | 215.5 |
SiO2 (mp-6930) | <1 0 1> | <1 0 1> | 325.4 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 214.8 |
Te2W (mp-22693) | <0 1 1> | <1 1 1> | 287.3 |
Te2Mo (mp-602) | <0 0 1> | <1 0 0> | 334.1 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 171.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 91.1 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 1> | 260.3 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 334.1 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 172.7 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 151.9 |
GaSe (mp-1943) | <1 0 0> | <1 0 0> | 273.4 |
BN (mp-984) | <1 0 0> | <0 0 1> | 57.6 |
BN (mp-984) | <1 1 1> | <0 0 1> | 230.2 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 91.1 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 243.0 |
Te2W (mp-22693) | <0 1 0> | <1 0 1> | 260.3 |
YVO4 (mp-19133) | <1 1 1> | <1 0 0> | 243.0 |
LiNbO3 (mp-3731) | <1 0 1> | <1 0 0> | 243.0 |
Al (mp-134) | <1 1 0> | <1 0 0> | 91.1 |
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 |
---|---|---|---|
Pu2SnPd2 (mp-640044) | 0.2272 | 0.670 | 3 |
Np2InNi2 (mp-20091) | 0.1886 | 0.110 | 3 |
La2InRh2 (mp-20907) | 0.1180 | 0.005 | 3 |
Yb2CdPd2 (mp-4663) | 0.2481 | 0.000 | 3 |
Yb2InPd2 (mp-21267) | 0.2503 | 0.014 | 3 |
Hf3Ge2 (mp-976273) | 0.1567 | 0.000 | 2 |
Ta3Ga2 (mp-16756) | 0.2596 | 0.000 | 2 |
Nb3Ga2 (mp-11393) | 0.2720 | 0.000 | 2 |
Hf3Si2 (mp-2105) | 0.2402 | 0.000 | 2 |
Nb3Si2 (mp-1078996) | 0.1278 | 0.022 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Nd_3 In_d Rh_pv |
Final Energy/Atom-6.0737 eV |
Corrected Energy-60.7369 eV
-60.7369 eV = -60.7369 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)