material
CrN2
ID:
mp-1014565
DOI:
10.17188/1337376
- Large change in a lattice parameter during relaxation.
- Large change in volume during relaxation.
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-0.127 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.347 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. |
Density1.95 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCrN + N2 |
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 MauguinCmcm [63] |
Hall-C 2c 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
X-Ray Diffraction
-
Select radiation source:
- Cu
- Ag
- Mo
- Fe
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%)
Substrates
Reference for minimal coincident interface area (MCIA) and elastic energy:substrate orientation:
| substrate material | substrate orientation | film orientation | MCIA† [Å2] |
|---|---|---|---|
| KCl (mp-23193) | <1 1 1> | <0 1 0> | 146.1 |
| TePb (mp-19717) | <1 1 1> | <0 1 0> | 146.1 |
| CdTe (mp-406) | <1 1 1> | <0 1 0> | 146.1 |
| YAlO3 (mp-3792) | <0 1 1> | <0 1 0> | 146.1 |
| YAlO3 (mp-3792) | <1 0 1> | <0 1 0> | 146.1 |
| MgF2 (mp-1249) | <1 0 0> | <0 1 0> | 146.1 |
| InSb (mp-20012) | <1 1 1> | <0 1 0> | 146.1 |
Elasticity
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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Similar Structures
Explanation of dissimilarity measure:
Documentation.
| material | dissimilarity | Ehull | # of elements |
|---|---|---|---|
| AlPO4 (mp-5724) | 0.4328 | 0.003 | 3 |
| AlPO4 (mp-5859) | 0.3709 | 0.011 | 3 |
| AlPO4 (mp-37990) | 0.3504 | 0.014 | 3 |
| AlPO4 (mp-557842) | 0.3496 | 0.011 | 3 |
| AlPO4 (mp-675254) | 0.3356 | 0.011 | 3 |
| CsAlSiO4 (mp-561457) | 0.6558 | 0.000 | 4 |
| CsBePO4 (mp-15395) | 0.5590 | 0.000 | 4 |
| SiO2 (mp-559313) | 0.1434 | 0.009 | 2 |
| SiO2 (mp-555891) | 0.1008 | 0.008 | 2 |
| SiO2 (mp-7648) | 0.1487 | 0.009 | 2 |
| SiO2 (mp-600018) | 0.1580 | 0.011 | 2 |
| CrN2 (mp-1096957) | 0.1355 | 0.352 | 2 |
Calculation Summary
Structure Optimization
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Cr_pv N |
Final Energy/Atom-8.6412 eV |
Corrected Energy-622.1663 eV
-622.1663 eV = -622.1663 eV (uncorrected energy)
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Detailed input parameters and outputs for all calculations
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)