material

HfTe3
ID:

mp-1025459
DOI:

10.17188/1355260

Warnings: [?]
  1. Large change in a lattice parameter during relaxation.
  2. Large change in volume during relaxation.
Tags: ZrSe3 High pressure experimental phase HfTe3 Hafnium telluride (1/3)

Material Details

Final Magnetic Moment
-0.000 μB

Calculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit.
Magnetic Ordering
Non-magnetic
Formation Energy / Atom
-0.626 eV

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

Energy Above Hull / Atom
0.015 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
7.63 g/cm3

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

Decomposes To
HfTe5 + HfTe2
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
P21/m [11]
Hall
-P 2yb
Point Group
2/m
Crystal System
monoclinic
We have not yet calculated a detailed bandstructure for this material

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) <1 1 0> <1 0 1> 100.1
AlN (mp-661) <1 0 1> <0 0 1> 258.7
AlN (mp-661) <1 1 0> <1 1 0> 295.4
CeO2 (mp-20194) <1 1 0> <1 1 0> 295.4
CeO2 (mp-20194) <1 1 1> <1 0 -1> 267.9
C (mp-48) <0 0 1> <1 0 0> 205.9
C (mp-48) <1 0 0> <1 0 -1> 178.6
C (mp-48) <1 0 1> <0 0 1> 164.6
C (mp-48) <1 1 1> <0 0 1> 305.7
GaAs (mp-2534) <1 0 0> <0 0 1> 94.1
GaAs (mp-2534) <1 1 1> <1 0 0> 164.8
BaF2 (mp-1029) <1 1 0> <1 0 0> 288.3
LaAlO3 (mp-2920) <0 0 1> <0 0 1> 282.2
LaAlO3 (mp-2920) <1 0 1> <1 0 0> 288.3
SiO2 (mp-6930) <0 0 1> <0 0 1> 258.7
SiO2 (mp-6930) <1 0 0> <1 0 -1> 223.3
SiO2 (mp-6930) <1 1 0> <1 1 0> 147.7
AlN (mp-661) <0 0 1> <0 1 1> 197.0
AlN (mp-661) <1 0 0> <1 0 1> 200.2
AlN (mp-661) <1 1 1> <1 0 0> 288.3
CeO2 (mp-20194) <1 0 0> <0 0 1> 94.1
DyScO3 (mp-31120) <0 0 1> <1 0 -1> 312.6
DyScO3 (mp-31120) <0 1 0> <0 0 1> 258.7
DyScO3 (mp-31120) <1 0 1> <1 0 -1> 223.3
KTaO3 (mp-3614) <1 0 0> <0 0 1> 47.0
KTaO3 (mp-3614) <1 1 0> <1 0 -1> 44.7
KTaO3 (mp-3614) <1 1 1> <1 0 -1> 223.3
InP (mp-20351) <1 0 0> <0 0 1> 70.5
Te2W (mp-22693) <0 1 1> <0 0 1> 117.6
Te2W (mp-22693) <1 1 0> <1 1 -1> 227.5
Te2W (mp-22693) <1 1 1> <1 1 0> 221.6
SiO2 (mp-6930) <1 0 1> <1 1 1> 316.6
SiO2 (mp-6930) <1 1 1> <0 0 1> 211.6
KCl (mp-23193) <1 1 0> <1 0 -1> 178.6
CdWO4 (mp-19387) <1 0 0> <0 0 1> 94.1
CdWO4 (mp-19387) <1 0 1> <0 0 1> 258.7
CdWO4 (mp-19387) <1 1 0> <0 0 1> 211.6
CdWO4 (mp-19387) <1 1 1> <1 0 0> 205.9
TePb (mp-19717) <1 1 0> <1 0 -1> 178.6
DyScO3 (mp-31120) <1 1 0> <0 0 1> 188.1
ZnSe (mp-1190) <1 0 0> <0 0 1> 94.1
ZnSe (mp-1190) <1 1 1> <1 0 0> 164.8
Te2Mo (mp-602) <1 0 0> <1 1 0> 221.6
Ni (mp-23) <1 1 0> <1 0 0> 205.9
Bi2Te3 (mp-34202) <0 0 1> <0 0 1> 188.1
InP (mp-20351) <1 1 0> <0 1 0> 245.2
Te2W (mp-22693) <0 0 1> <1 1 0> 221.6
Te2W (mp-22693) <0 1 0> <1 0 0> 164.8
GaSe (mp-1943) <0 0 1> <1 0 -1> 223.3
BN (mp-984) <1 0 0> <0 0 1> 94.1
Up to 50 entries displayed.
†minimal coincident interface area.

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.

Once you have registered you can also "vote" for full calculation of this material's elastic properties.

Similar Structures beta feature

Explanation of dissimilarity measure: Documentation.
material dissimilarity Ehull # of elements
Rb(ThSe3)2 (mp-9523) 0.6195 0.000 3
HfSiTe (mp-13963) 0.6331 0.000 3
K(USe3)2 (mp-12414) 0.6527 0.000 3
ZrSiTe (mp-19917) 0.6501 0.000 3
U2TlSe6 (mp-1078777) 0.6720 0.000 3
CeMnSbO (mp-542723) 0.5268 0.114 4
LaMnSbO (mp-18745) 0.5329 0.001 4
SmMnSbO (mp-510488) 0.4856 0.078 4
NdMnSbO (mp-18755) 0.5000 0.054 4
NdZnSbO (mp-12516) 0.5587 0.000 4
UTe3 (mp-8357) 0.3111 0.000 2
HfSe3 (mp-15622) 0.3402 0.000 2
ZrTe3 (mp-2089) 0.1908 0.000 2
ZrSe3 (mp-1683) 0.3796 0.000 2
UTe3 (mp-568948) 0.2970 0.000 2
Nd5Fe5As5O4F (mp-698941) 0.6749 0.160 5
Ce8Fe8As8O7F (mp-705511) 0.6798 0.113 5
SrNd7Fe8(AsO)8 (mp-705458) 0.5946 0.162 5
Sm6Fe6As6O5F (mp-697821) 0.6287 0.169 5
SrNd5Fe6(AsO)6 (mp-694989) 0.6113 0.172 5
Up to 5 similar elemental, binary, ternary, quaternary, etc. structures displayed (dissimilarity threshold 0.75). Ehull: energy above hull per atom [eV].

Calculation Summary

Structure Optimization

Run Type
GGA
Energy Cutoff
520 eV
# of K-points
None
U Values
--
Pseudopotentials
VASP PAW: Hf_pv Te
Final Energy/Atom
-5.4714 eV
Corrected Energy
-43.7712 eV
-43.7712 eV = -43.7712 eV (uncorrected energy)

Detailed input parameters and outputs for all calculations

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ICSD IDs
  • 638958
  • 638962
Submitted by
User remarks:
  • Hafnium telluride (1/3)
  • High pressure experimental phase

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)