material

Lu2(NiB2)3
ID:

mp-8771
DOI:

10.17188/1312704

Tags: Dilutetium trinickel boride

Material Details

Final Magnetic Moment
0.003 μB

Calculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit.
Magnetic Ordering
NM
Formation Energy / Atom
-0.597 eV

Calculated formation energy from the elements normalized to per atom in the unit cell.

Energy Above Hull / Atom
0.000 eV

The 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.

Density
8.76 g/cm3

The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%)

Decomposes To
Stable
Band Gap
0.000 eV

In 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.

Space Group

Hermann Mauguin
Cmmm [65]
Hall
-C 2 2
Point Group
mmm
Crystal System
orthorhombic

Band Structure

Density of States
Warning! Semi-local DFT tends to severely underestimate bandgaps. Please see the wiki for more info.

sign indicates spin ↑ ↓

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%)

X-Ray Absorption Spectra

FEFF XANES

Select an element to display a spectrum averaged over all sites of that element in the structure.

Apply Gaussian smoothing:

0 eV
3 eV
FWHM: 0 eV

Download spectra for every symmetrically equivalent absorption site in the structure.

Download FEFF Input parameters.

Warning: These results are intended to be semi-quantitative in that corrections, such as edge shifts and Debye-Waller damping, have not been included.

Substrates

Reference for minimal coincident interface area (MCIA) and elastic energy:
substrate orientation:
No elastic tensor calculated for this material, so elastic energies not avaialable. Sorting by MCIA instead.
substrate material substrate orientation film orientation MCIA† [Å2]
GaAs (mp-2534) <1 1 0> <1 0 1> 143.2
GaN (mp-804) <0 0 1> <0 1 0> 261.8
GaN (mp-804) <1 1 1> <0 1 0> 157.1
SiO2 (mp-6930) <1 0 0> <0 0 1> 196.0
SiO2 (mp-6930) <1 1 0> <1 0 1> 143.2
InAs (mp-20305) <1 0 0> <1 0 0> 146.8
InAs (mp-20305) <1 1 0> <1 0 0> 205.5
ZnSe (mp-1190) <1 0 0> <1 1 0> 196.7
ZnSe (mp-1190) <1 1 0> <1 0 1> 143.2
CdS (mp-672) <0 0 1> <0 1 0> 340.3
CdS (mp-672) <1 0 0> <1 1 1> 228.8
CdS (mp-672) <1 1 0> <1 0 0> 264.2
LiF (mp-1138) <1 1 1> <1 1 0> 118.0
Te2W (mp-22693) <0 0 1> <1 0 0> 88.1
Te2W (mp-22693) <0 1 1> <1 0 0> 58.7
YVO4 (mp-19133) <1 0 0> <0 1 0> 183.3
YVO4 (mp-19133) <1 0 1> <1 1 0> 275.4
Te2Mo (mp-602) <0 0 1> <0 1 0> 235.6
Te2Mo (mp-602) <1 1 0> <0 1 1> 281.5
Bi2Te3 (mp-34202) <0 0 1> <0 1 0> 235.6
BN (mp-984) <0 0 1> <0 0 1> 65.3
BN (mp-984) <1 1 1> <1 0 0> 264.2
LiNbO3 (mp-3731) <0 0 1> <1 1 1> 305.0
LiNbO3 (mp-3731) <1 0 0> <0 1 0> 209.4
Bi2Se3 (mp-541837) <0 0 1> <0 1 0> 340.3
LaAlO3 (mp-2920) <0 0 1> <1 0 0> 205.5
MoS2 (mp-1434) <0 0 1> <0 1 0> 366.5
Al (mp-134) <1 0 0> <1 1 0> 196.7
Al (mp-134) <1 1 0> <0 1 0> 209.4
AlN (mp-661) <0 0 1> <0 1 0> 183.3
AlN (mp-661) <1 0 0> <0 1 1> 140.8
AlN (mp-661) <1 0 1> <1 0 0> 205.5
AlN (mp-661) <1 1 0> <1 1 1> 305.0
CeO2 (mp-20194) <1 0 0> <0 1 0> 235.6
CeO2 (mp-20194) <1 1 0> <0 1 0> 209.4
GaAs (mp-2534) <1 0 0> <1 1 0> 196.7
LiGaO2 (mp-5854) <0 0 1> <1 0 0> 352.3
LiGaO2 (mp-5854) <0 1 0> <1 0 0> 264.2
LiGaO2 (mp-5854) <0 1 1> <1 0 0> 88.1
LiGaO2 (mp-5854) <1 0 0> <0 1 0> 340.3
LiGaO2 (mp-5854) <1 0 1> <0 1 0> 314.2
LiGaO2 (mp-5854) <1 1 0> <0 0 1> 196.0
LiGaO2 (mp-5854) <1 1 1> <1 1 1> 228.8
GaN (mp-804) <1 0 0> <0 1 0> 235.6
GaN (mp-804) <1 0 1> <1 0 0> 264.2
GaN (mp-804) <1 1 0> <1 1 0> 118.0
SiO2 (mp-6930) <0 0 1> <1 0 0> 88.1
SiO2 (mp-6930) <1 0 1> <1 0 0> 234.9
SiO2 (mp-6930) <1 1 1> <1 0 0> 205.5
DyScO3 (mp-31120) <0 0 1> <1 0 1> 286.5
Up to 50 entries displayed.
†minimal coincident interface area.

Elasticity

Reference for tensor and properties:
Visualize with ELATE
Stiffness Tensor Cij (GPa)
349 110 116 0 0 0
110 409 92 0 0 0
116 92 358 0 0 0
0 0 0 142 0 0
0 0 0 0 159 0
0 0 0 0 0 131
Compliance Tensor Sij (10-12Pa-1)
3.4 -0.7 -0.9 0 0 0.0
-0.7 2.7 -0.5 0 0 0.0
-0.9 -0.5 3.2 0 0 -0.0
0 0 0 7.0 0.0 0
0 0 0 0.0 6.3 0
0.0 0.0 -0.0 0 0 7.6
Shear Modulus GV
140 GPa
Bulk Modulus KV
195 GPa
Shear Modulus GR
138 GPa
Bulk Modulus KR
194 GPa
Shear Modulus GVRH
139 GPa
Bulk Modulus KVRH
194 GPa
Elastic Anisotropy
0.06
Poisson's Ratio
0.21

Similar Structures beta feature

Explanation of dissimilarity measure: Documentation.
material dissimilarity Ehull # of elements
Yb2(NiB2)3 (mp-14344) 0.2409 0.056 3
Er2(NiB2)3 (mp-4071) 0.0322 0.000 3
Ho2(NiB2)3 (mp-1095435) 0.1007 0.000 3
Up to 5 similar elemental, binary, ternary, quaternary, etc. structures displayed (dissimilarity threshold 0.75). Ehull: energy above hull per atom [eV].

Calculation Summary

Elasticity

Methodology

Structure Optimization

Run Type
GGA
Energy Cutoff
520 eV
# of K-points
24
U Values
--
Pseudopotentials
VASP PAW: B Ni_pv Lu_3
Final Energy/Atom
-6.6392 eV
Corrected Energy
-73.0309 eV
-73.0309 eV = -73.0309 eV (uncorrected energy)

Detailed input parameters and outputs for all calculations

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ICSD IDs
  • 68002
Submitted by
User remarks:
  • Dilutetium trinickel boride

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)