material

HfBe
ID:

mp-1018057
DOI:

10.17188/1350146

Tags: TlI BeHf Beryllium hafnium (1/1)

Material Details

Final Magnetic Moment
0.131 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
-0.083 eV

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

Energy Above Hull / Atom
0.063 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
9.95 g/cm3

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

Decomposes To
HfBe5 + Hf
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
Cmcm [63]
Hall
-C 2c 2
Point Group
mmm
Crystal System
orthorhombic

Electronic Structure

Topological data for ICSD ID 616286 from Topological Materials Database
Topological Classification
trivial*
Subclassification
LCEBR†
* trivial insulator or metal
† Linear Combination of Elementary Band Representations
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%)

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]
C (mp-48) <0 0 1> <1 1 0> 79.1
C (mp-48) <1 0 0> <0 1 0> 174.7
C (mp-48) <1 0 1> <0 1 0> 224.7
C (mp-48) <1 1 1> <0 1 0> 237.2
LaAlO3 (mp-2920) <0 0 1> <1 1 0> 197.6
AlN (mp-661) <0 0 1> <0 1 0> 212.2
AlN (mp-661) <1 0 0> <0 1 0> 112.3
AlN (mp-661) <1 1 0> <0 1 1> 107.2
CeO2 (mp-20194) <1 1 0> <0 1 1> 250.2
GaAs (mp-2534) <1 0 0> <1 0 1> 251.4
GaAs (mp-2534) <1 1 0> <0 1 0> 187.2
BaF2 (mp-1029) <1 1 0> <1 1 0> 118.6
SiO2 (mp-6930) <0 0 1> <0 1 0> 237.2
SiO2 (mp-6930) <1 0 0> <0 1 1> 107.2
SiO2 (mp-6930) <1 1 1> <1 1 0> 158.1
KCl (mp-23193) <1 0 0> <0 0 1> 200.9
KCl (mp-23193) <1 1 0> <1 1 0> 118.6
DyScO3 (mp-31120) <0 0 1> <0 1 1> 214.5
DyScO3 (mp-31120) <0 1 1> <0 1 1> 107.2
DyScO3 (mp-31120) <1 0 0> <0 1 0> 187.2
DyScO3 (mp-31120) <1 0 1> <0 1 1> 285.9
InAs (mp-20305) <1 1 1> <0 1 0> 262.1
ZnSe (mp-1190) <1 0 0> <1 0 1> 251.4
ZnSe (mp-1190) <1 1 0> <0 1 0> 187.2
C (mp-48) <1 1 0> <0 1 0> 262.1
CdWO4 (mp-19387) <0 0 1> <1 0 1> 150.9
CdWO4 (mp-19387) <0 1 0> <0 1 0> 187.2
CdWO4 (mp-19387) <0 1 1> <0 1 0> 162.3
CdWO4 (mp-19387) <1 0 0> <0 1 1> 250.2
CdWO4 (mp-19387) <1 0 1> <0 1 0> 224.7
CdWO4 (mp-19387) <1 1 0> <0 1 0> 162.3
CdWO4 (mp-19387) <1 1 1> <1 1 0> 158.1
LaAlO3 (mp-2920) <1 0 0> <1 1 0> 276.7
TePb (mp-19717) <1 0 0> <0 0 1> 134.0
TePb (mp-19717) <1 1 0> <1 1 0> 118.6
AlN (mp-661) <1 0 1> <0 1 0> 199.7
AlN (mp-661) <1 1 1> <0 1 1> 178.7
CeO2 (mp-20194) <1 0 0> <0 1 1> 178.7
BaF2 (mp-1029) <1 0 0> <0 0 1> 200.9
Te2Mo (mp-602) <0 0 1> <1 1 0> 197.6
Te2Mo (mp-602) <1 0 0> <1 1 0> 158.1
Te2Mo (mp-602) <1 0 1> <0 0 1> 167.5
Te2Mo (mp-602) <1 1 1> <0 1 0> 274.6
SiO2 (mp-6930) <1 0 1> <0 1 0> 249.6
SiO2 (mp-6930) <1 1 0> <0 1 1> 321.7
Ni (mp-23) <1 0 0> <1 0 1> 50.3
Ni (mp-23) <1 1 0> <1 1 0> 158.1
Ni (mp-23) <1 1 1> <0 0 1> 167.5
Bi2Te3 (mp-34202) <0 0 1> <0 1 0> 287.1
GaSe (mp-1943) <0 0 1> <0 1 1> 143.0
Up to 50 entries displayed.
†minimal coincident interface area.

Elasticity

Reference for tensor and properties:
Visualize with ELATE
Stiffness Tensor Cij (GPa)
190 83 65 0 0 0
83 172 92 0 0 0
65 92 161 0 0 0
0 0 0 71 0 0
0 0 0 0 83 0
0 0 0 0 0 94
Compliance Tensor Sij (10-12Pa-1)
6.8 -2.6 -1.3 0 0 0
-2.6 9.4 -4.3 0 0 0
-1.3 -4.3 9.2 0 0 0
0 0 0 14.1 0 0
0 0 0 0 12 0
0 0 0 0 0 10.7
Shear Modulus GV
68 GPa
Bulk Modulus KV
111 GPa
Shear Modulus GR
61 GPa
Bulk Modulus KR
111 GPa
Shear Modulus GVRH
65 GPa
Bulk Modulus KVRH
111 GPa
Elastic Anisotropy
0.60
Poisson's Ratio
0.26

Similar Structures beta feature

Explanation of dissimilarity measure: Documentation.
material dissimilarity Ehull # of elements
Hf2NiP (mp-5918) 0.6151 0.000 3
Zr2CoP (mp-29152) 0.5344 0.000 3
Zr2NiP (mp-29153) 0.5573 0.000 3
Hf2CoP (mp-29154) 0.5995 0.000 3
TaNiB2 (mp-22709) 0.6803 0.000 3
SrCa2In2Ge (mp-619206) 0.5915 0.105 4
EuAl (mp-1079783) 0.1191 0.086 2
BMo (mp-1890) 0.3477 0.000 2
YAl (mp-11228) 0.3680 0.005 2
BW (mp-7832) 0.3340 0.000 2
BW (mp-1008487) 0.3746 0.013 2
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
None
U Values
--
Pseudopotentials
VASP PAW: Hf_pv Be_sv
Final Energy/Atom
-6.9251 eV
Corrected Energy
-27.7004 eV
-27.7004 eV = -27.7004 eV (uncorrected energy)

Detailed input parameters and outputs for all calculations

Show JSON History Show BibTex Citation Download BibTex Citation
ICSD IDs
  • 616286
Submitted by
User remarks:
  • Beryllium hafnium (1/1)

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)