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-0.467 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.133 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. |
Density7.27 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToZrInPd2 + ZrIn + ZrPd |
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 MauguinP42/mnm [136] |
Hall-P 4n 2n |
Point Group4/mmm |
Crystal Systemtetragonal |
Topological ClassificationSM*
|
SubclassificationES†
|
Crossing TypeLine
|
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] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 290.7 |
AlN (mp-661) | <1 0 0> | <1 0 1> | 173.4 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 192.9 |
AlN (mp-661) | <1 1 0> | <1 0 0> | 290.7 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 64.3 |
GaN (mp-804) | <1 1 1> | <1 1 0> | 246.7 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 232.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 321.6 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 321.6 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 257.2 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 321.6 |
KCl (mp-23193) | <1 1 0> | <1 0 1> | 173.4 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 232.6 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 321.6 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 321.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 246.7 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 86.7 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 64.3 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 64.3 |
ZnSe (mp-1190) | <1 1 0> | <1 0 0> | 232.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 321.6 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 246.7 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 232.6 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 246.7 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 257.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 64.3 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 321.6 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 257.2 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 290.7 |
YVO4 (mp-19133) | <1 0 0> | <1 0 0> | 232.6 |
Te2Mo (mp-602) | <0 0 1> | <1 0 0> | 174.4 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 290.7 |
Ag (mp-124) | <1 1 0> | <1 0 0> | 290.7 |
BN (mp-984) | <1 0 0> | <0 0 1> | 192.9 |
BN (mp-984) | <1 0 1> | <0 0 1> | 257.2 |
LiNbO3 (mp-3731) | <0 0 1> | <1 0 1> | 260.1 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 0> | 246.7 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 290.7 |
BN (mp-984) | <1 1 1> | <1 0 0> | 232.6 |
LiNbO3 (mp-3731) | <1 0 0> | <1 0 0> | 232.6 |
MoS2 (mp-1434) | <0 0 1> | <1 1 0> | 246.7 |
MoS2 (mp-1434) | <1 1 0> | <1 1 0> | 246.7 |
Al (mp-134) | <1 0 0> | <0 0 1> | 64.3 |
Al (mp-134) | <1 1 0> | <0 0 1> | 321.6 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 1> | 86.7 |
TeO2 (mp-2125) | <1 1 0> | <0 0 1> | 192.9 |
SiC (mp-7631) | <0 0 1> | <1 0 1> | 173.4 |
LiTaO3 (mp-3666) | <0 0 1> | <1 0 1> | 260.1 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 321.6 |
TiO2 (mp-2657) | <1 1 0> | <1 0 1> | 173.4 |
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 |
---|---|---|---|
Ti2InNi2 (mp-20339) | 0.2117 | 0.000 | 3 |
Hf2InNi2 (mp-669575) | 0.4854 | 0.004 | 3 |
Zr2Ni2Sn (mp-510040) | 0.4508 | 0.017 | 3 |
Hf2Ni2Sn (mp-510041) | 0.4920 | 0.010 | 3 |
Er2SnAu2 (mp-31143) | 0.4948 | 0.024 | 3 |
Hf3Al2 (mp-8462) | 0.4361 | 0.037 | 2 |
Ca3Cd2 (mp-18167) | 0.4829 | 0.000 | 2 |
Zr3Al2 (mp-13470) | 0.3095 | 0.031 | 2 |
Lu3Al2 (mp-16508) | 0.5095 | 0.000 | 2 |
Na3Hg2 (mp-17974) | 0.5046 | 0.003 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Zr_sv In_d Pd |
Final Energy/Atom-6.5073 eV |
Corrected Energy-130.1455 eV
Uncorrected energy = -130.1455 eV
Corrected energy = -130.1455 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)