material

HoCu4Ag
ID:

mp-1024987
DOI:

10.17188/1355259

Tags: Holmium copper silver (1/4/1) Friauf-Laves phase MgCu4Sn AgCu4Ho

Material Details

Final Magnetic Moment
0.159 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
-0.232 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
9.62 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
F43m [216]
Hall
F 4 2 3
Point Group
43m
Crystal System
cubic

Electronic Structure

Topological data for ICSD ID 605023 from Topological Materials Database
Topological Classification
SM*
Subclassification
ESFD†
Crossing Type
Point
* Semimetal
† Enforced Semimetal with Fermi point Degeneracy

Band Structure and Density of States

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

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 0 0> 254.8
C (mp-48) <1 0 0> <1 1 0> 288.2
AlN (mp-661) <0 0 1> <1 1 1> 264.8
AlN (mp-661) <1 0 0> <1 0 0> 152.9
AlN (mp-661) <1 1 0> <1 1 0> 216.2
GaAs (mp-2534) <1 0 0> <1 0 0> 254.8
GaAs (mp-2534) <1 1 0> <1 1 0> 144.1
GaAs (mp-2534) <1 1 1> <1 1 0> 288.2
BaF2 (mp-1029) <1 0 0> <1 0 0> 203.8
BaF2 (mp-1029) <1 1 0> <1 1 0> 216.2
BaF2 (mp-1029) <1 1 1> <1 1 1> 264.8
SiO2 (mp-6930) <0 0 1> <1 1 1> 88.3
SiO2 (mp-6930) <1 0 0> <1 1 0> 216.2
SiO2 (mp-6930) <1 1 1> <1 1 0> 216.2
KCl (mp-23193) <1 0 0> <1 0 0> 203.8
DyScO3 (mp-31120) <0 0 1> <1 1 0> 288.2
DyScO3 (mp-31120) <0 1 0> <1 0 0> 254.8
DyScO3 (mp-31120) <0 1 1> <1 1 0> 216.2
DyScO3 (mp-31120) <1 1 0> <1 0 0> 254.8
InAs (mp-20305) <1 1 0> <1 1 0> 216.2
InAs (mp-20305) <1 1 1> <1 1 1> 264.8
ZnSe (mp-1190) <1 0 0> <1 0 0> 254.8
ZnSe (mp-1190) <1 1 0> <1 1 0> 144.1
ZnSe (mp-1190) <1 1 1> <1 1 0> 288.2
KTaO3 (mp-3614) <1 0 0> <1 0 0> 254.8
KTaO3 (mp-3614) <1 1 1> <1 0 0> 254.8
InP (mp-20351) <1 1 0> <1 1 0> 144.1
InP (mp-20351) <1 1 1> <1 0 0> 305.7
Te2W (mp-22693) <0 0 1> <1 1 0> 216.2
Te2W (mp-22693) <0 1 0> <1 1 0> 216.2
Te2W (mp-22693) <1 1 0> <1 1 0> 216.2
TePb (mp-19717) <1 0 0> <1 0 0> 203.8
Te2Mo (mp-602) <1 0 0> <1 1 0> 216.2
Te2Mo (mp-602) <1 0 1> <1 1 1> 264.8
Ni (mp-23) <1 1 1> <1 0 0> 254.8
GaSe (mp-1943) <0 0 1> <1 1 1> 88.3
BN (mp-984) <1 0 0> <1 0 0> 152.9
BN (mp-984) <1 1 0> <1 1 1> 264.8
Bi2Se3 (mp-541837) <0 0 1> <1 0 0> 152.9
MoS2 (mp-1434) <0 0 1> <1 0 0> 305.7
Al (mp-134) <1 0 0> <1 0 0> 254.8
Al (mp-134) <1 1 1> <1 0 0> 254.8
LiGaO2 (mp-5854) <0 0 1> <1 1 0> 216.2
LiGaO2 (mp-5854) <0 1 0> <1 0 0> 254.8
LiGaO2 (mp-5854) <0 1 1> <1 0 0> 254.8
TeO2 (mp-2125) <0 0 1> <1 1 0> 288.2
SiC (mp-7631) <0 0 1> <1 1 0> 288.2
Fe3O4 (mp-19306) <1 1 0> <1 1 0> 216.2
MgO (mp-1265) <1 1 0> <1 1 0> 288.2
TiO2 (mp-2657) <1 0 0> <1 1 0> 288.2
Up to 50 entries displayed.
†minimal coincident interface area.

Elasticity

Reference for tensor and properties:
Visualize with ELATE
Stiffness Tensor Cij (GPa)
150 91 91 0 0 0
91 150 91 0 0 0
91 91 150 0 0 0
0 0 0 30 0 0
0 0 0 0 30 0
0 0 0 0 0 30
Compliance Tensor Sij (10-12Pa-1)
12.4 -4.7 -4.7 0 0 0
-4.7 12.4 -4.7 0 0 0
-4.7 -4.7 12.4 0 0 0
0 0 0 33.8 0 0
0 0 0 0 33.8 0
0 0 0 0 0 33.8
Shear Modulus GV
29 GPa
Bulk Modulus KV
111 GPa
Shear Modulus GR
29 GPa
Bulk Modulus KR
111 GPa
Shear Modulus GVRH
29 GPa
Bulk Modulus KVRH
111 GPa
Elastic Anisotropy
0.00
Poisson's Ratio
0.38

Similar Structures beta feature

Explanation of dissimilarity measure: Documentation.
material dissimilarity Ehull # of elements
ErCdNi4 (mp-1072598) 0.0025 0.000 3
GdCu4Au (mp-1072041) 0.0014 0.000 3
TbCdNi4 (mp-1077082) 0.0023 0.000 3
ErCu4Pd (mp-1077518) 0.0024 0.000 3
TbCu4Au (mp-1077752) 0.0000 0.000 3
TmCu5 (mp-30600) 0.0023 0.000 2
Be5Fe (mp-1025010) 0.0035 0.014 2
LuCu5 (mp-580136) 0.0035 0.000 2
HfNi5 (mp-569516) 0.0026 0.015 2
CeIr5 (mp-1077075) 0.0014 0.327 2
Co (mp-1072089) 0.0268 0.199 1
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: Ho_3 Cu_pv Ag
Final Energy/Atom
-4.2006 eV
Corrected Energy
-25.2034 eV
Uncorrected energy = -25.2034 eV Corrected energy = -25.2034 eV

Detailed input parameters and outputs for all calculations

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ICSD IDs
  • 605023
Submitted by
User remarks:
  • Holmium copper silver (1/4/1)

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)