Final Magnetic Moment0.122 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-0.252 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.099 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. |
Density10.09 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToHo5Pb3 + Ho |
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 MauguinI4/mmm [139] |
Hall-I 4 2 |
Point Group4/mmm |
Crystal Systemtetragonal |
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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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 176.2 |
AlN (mp-661) | <1 1 1> | <1 0 0> | 344.8 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 264.3 |
GaAs (mp-2534) | <1 1 0> | <1 0 1> | 323.8 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 198.2 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 344.8 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 242.2 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 198.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 176.2 |
AlN (mp-661) | <1 0 0> | <1 1 1> | 219.2 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 286.3 |
GaAs (mp-2534) | <1 0 0> | <1 0 1> | 269.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 219.2 |
ZnSe (mp-1190) | <1 0 0> | <1 0 1> | 269.8 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 220.2 |
CdS (mp-672) | <1 0 1> | <0 0 1> | 374.4 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 352.3 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 344.8 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 209.0 |
GaN (mp-804) | <1 1 1> | <1 0 1> | 323.8 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 88.1 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 330.3 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 197.0 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 176.2 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 1> | 219.2 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 1> | 269.8 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 197.0 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 44.0 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 308.3 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 88.1 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 330.3 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 198.2 |
ZnSe (mp-1190) | <1 1 0> | <1 0 1> | 323.8 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 330.3 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 246.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 0> | 344.8 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 242.2 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 286.3 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 197.0 |
BN (mp-984) | <0 0 1> | <1 1 0> | 278.7 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 330.3 |
LiNbO3 (mp-3731) | <1 0 0> | <1 0 0> | 147.8 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 110.1 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 220.2 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 286.3 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 286.3 |
GaSe (mp-1943) | <1 0 0> | <1 0 1> | 269.8 |
MoS2 (mp-1434) | <0 0 1> | <1 0 1> | 323.8 |
MoS2 (mp-1434) | <1 0 0> | <1 0 0> | 197.0 |
MoS2 (mp-1434) | <1 0 1> | <1 0 0> | 197.0 |
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 |
---|---|---|---|
GaCo2Ni (mp-20551) | 0.3816 | 0.080 | 3 |
MnGaFe2 (mp-1065753) | 0.4093 | 0.053 | 3 |
Cr8Ni50Mo15W2 (mp-767372) | 0.6637 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.6637 | 0.118 | 4 |
CrFeCoNi (mp-1096923) | 0.6897 | 0.193 | 4 |
K3Sm (mp-973554) | 0.0378 | 0.565 | 2 |
Sm3I (mp-978798) | 0.0423 | 0.366 | 2 |
Li3Al (mp-975868) | 0.0440 | 0.043 | 2 |
NbAl3 (mp-1842) | 0.0440 | 0.000 | 2 |
TiAl3 (mp-542915) | 0.0376 | 0.000 | 2 |
Na (mp-974920) | 0.4393 | 0.002 | 1 |
Rb (mp-975519) | 0.3659 | 0.017 | 1 |
Ba (mp-1058581) | 0.3593 | 0.019 | 1 |
Tl (mp-151) | 0.4510 | 0.010 | 1 |
In (mp-1055994) | 0.3437 | 0.030 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ho_3 Pb_d |
Final Energy/Atom-4.6174 eV |
Corrected Energy-18.4697 eV
-18.4697 eV = -18.4697 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)