Final Magnetic Moment0.326 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-1.175 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.096 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. |
Density12.33 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToIrO2 |
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 MauguinPa3 [205] |
Hall-P 2ac 2ab 3 |
Point Groupm3 |
Crystal Systemcubic |
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%)
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 |
---|---|---|---|
LiAsO3 (mp-9657) | 0.5964 | 0.000 | 3 |
BaSr2I6 (mp-752439) | 0.6162 | 0.027 | 3 |
TlCoO3 (mp-770150) | 0.6196 | 0.054 | 3 |
CuAsO3 (mp-776320) | 0.5681 | 0.092 | 3 |
ZnSiO3 (mp-1020623) | 0.5779 | 0.148 | 3 |
LiMnOF2 (mp-765319) | 0.6718 | 0.107 | 4 |
LiV2OF5 (mp-765917) | 0.7067 | 0.211 | 4 |
Li2TiTeO6 (mp-756117) | 0.6924 | 0.000 | 4 |
Na2GeTeO6 (mp-10340) | 0.6866 | 0.000 | 4 |
Zn2MoWO6 (mvc-16352) | 0.6901 | 0.028 | 4 |
SiO2 (mp-9258) | 0.1940 | 0.571 | 2 |
PdF2 (mp-20284) | 0.2384 | 0.041 | 2 |
GeO2 (mp-2633) | 0.2273 | 0.225 | 2 |
RuO2 (mp-8909) | 0.1400 | 0.067 | 2 |
OsO2 (mp-1095264) | 0.0846 | 0.077 | 2 |
Li4ZrNb(TeO6)2 (mp-756177) | 0.6920 | 0.058 | 5 |
Explore more synthesis descriptions for materials of composition IrO2.
Text computed by synthesisproject.org.
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ir O |
Final Energy/Atom-6.9519 eV |
Corrected Energy-89.0408 eV
-89.0408 eV = -83.4225 eV (uncorrected energy) - 5.6183 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)