JVASP-10671_Tm6ReO12
JARVIS-ID:JVASP-10671 Functional:optB88-vdW Primitive cell Primitive cell Conventional cell Conventional cell
Chemical formula:Tm6ReO12 Formation energy/atom (eV):-3.489 a 6.362 Å α:98.81 ° a 9.662 Å α:90.0 °
Space-group :R-3, 148 Relaxed energy/atom (eV):-6.5684 b 6.362 Å β:98.81 ° b 9.662 Å β:90.0 °
Calculation type:Bulk SCF bandgap (eV):0.024 c 6.362 Å γ:98.81 ° c 9.178 Å γ:120.0 °
Crystal system:trigonal Point group:-3 Density (gcm-3):9.34 Volume (3):247.35 nAtoms_prim:19 nAtoms_conv:57
Download input files

Convergence [Reference]

Calculations are done using VASP software [Source-code]. Convergence on KPOINTS [Source-code] and ENCUT [Source-code] is done with respect to total energy of the system within 0.001 eV tolerance. Please note convergence on KPOINTS and ENCUT is generally done for target properties, but here we assume energy-convergence with 0.001 eV should be sufficient for other properties also. The points on the curves are obtained with single-point calculation (number of ionic steps, NSW=1 ). However, for very accurate calculations, NSW>1 might be needed.


Structural analysis [Reference]

The following shows the X-ray diffraction (XRD)[Source-code] pattern and the Radial distribution function (RDF) plots [Source-code]. XRD peaks should be comparable to experiments for bulk structures. Relative intensities may differ. For mono- and multi-layer structures , we take the z-dimension during DFT calculation for XRD calculations, which may differ from the experimental set-up.


Electronic structure [Reference]

The following shows the electronic density of states and bandstructure [Source-code]. DFT is generally predicted to underestimate bandgap of materials. Accurate band-gaps are obtained with higher level methods (with high computational requirement) such as HSE, GW , which are under progress. If available, MBJ data should be comparable to experiments also. Total DOS, Orbital DOS and Element dos [Source-code] buttons are provided for density of states options. Energy is rescaled to make Fermi-energy zero. In the bandstructure plot [Source-code], spin up is shown with blue lines while spin down are shown with red lines. Non-degenerate spin-up and spin-down states (if applicable) would imply a net orbital magnetic moment in the system. Fermi-occupation tolerance for bandgap calculation is chosen as 0.001.

High-symmetry kpoints based bandgap (eV): 0.017I


Electrostatic potential [Reference]

The following plot shows the plane averaged electrostatic potential (ionic+Hartree) along x, y and z-directions. The red line shows the Fermi-energy while the green line shows the maximum value of the electrostatic potential. For slab structures (with vacuum along z-direction), the difference in these two values can be used to calculate work-function of the material.


Optoelectronic properties Semi-local [Reference]

Incident photon energy dependence of optical is shown below [Source-code]. Only interband optical transitions are taken into account.Please note the underestimatation of band-gap problem with DFT will reflect in the spectra as well. For very accurate optical properties GW/BSE calculation would be needed, which is yet to be done because of their very high computational cost. Optical properties for mono-/multi-layer materials were rescaled with the actual thickness to simulation z-box ratio. Absorption coeffiecient is in cm-1 unit. Also, ionic contributions were neglected.

Dense k-mesh based bandgap is : 0.0272 eV

Static real-parts of dielectric function in x,y,z: 10.04,9.97,10.08


Optoelectronic properties METAGGA-MBJ [Reference]

Single point DFT calculation was carried out with meta-gga MBJ potential [Source-code]. This should give reasonable bandgap, and optical properties assuming the calculation was properly converged. Incident photon energy dependence of optical is shown below. Only interband optical transitions are taken into account. Also, ionic contributions were neglected.

MBJ bandgap is : 0.0044 eV

Static real-parts of dielectric function in x,y,z: -7.58,7.78,8.87


Finite-difference: elastic tensor and derived phonon properties [Reference]

Elastic tensor calculated for the conventional cell of the system with finite-difference method [Source-code]. For bulk structures, elastic constants are given in GPa unit . For layered materials, the elastic constants are rescaled with respect to vacuum padding (see the input files) and the units for elastic coefficients are in N/m . Phonons obtained [Source-code] from this calculation are also shown.

WARNING: Please note we provide finite-size cell phonons only. At least 1.2 nm x1.2 nm x1.2 nm size cell or more is generally needed for obtaining reliable phonon spectrum, but we take conventional cell of the structure only. For systems having primitive-cell phonon representation tables, I denotes infrared activity and R denotes Raman active modes (where applicabale). Selection of particular q-point mesh can give rise to unphysical negative modes in phonon density of states and phonon bandstructre. The minimum thermal conductivity was calculated using elastic tensor information following Clarke and Cahill formalism.

Voigt-bulk modulus (KV): 163.87 GPa, Voigt-shear modulus (GV): 72.24 GPa

Reuss-bulk modulus (KR): 163.87 GPa, Reuss-shear modulus (GR): 66.48 GPa

Poisson's ratio: 0.31, Elastic anisotropy parameter: 0.43

Clarke's lower limit of thermal conductivity (W/(m.K)): 0.96

Cahill's lower limit of thermal conductivity (W/(m.K)): 1.08

Elastic tensor
250.1 137.1 103.8 0.0 11.5 -10.2
137.1 250.1 103.8 0.0 -11.5 10.2
103.8 103.8 285.2 0.0 -0.0 -0.0
0.0 0.0 0.0 56.5 10.2 11.5
11.5 -11.5 -0.0 10.2 78.9 0.0
-10.2 10.2 -0.0 11.5 0.0 78.9

Phonon mode (cm-1)
-99.28
-99.28
-90.54
-85.99
-85.99
-80.66
-69.32
-64.66
-64.66
-61.9
-61.9
-56.5
-55.3
-55.27
-55.27
-51.15
-51.15
-48.12
-0.41
-0.14
-0.13
91.05
91.05
103.66
111.86
111.86
123.03
125.14
125.14
137.26
143.71
143.71
155.14
175.06
181.62
181.62
203.26
203.48
203.48
256.5
256.72
256.72
257.89
257.89
258.77
329.65
333.32
333.32
337.4
337.4
363.32
373.79
373.79
382.13
395.49
396.06
396.06
407.49
418.96
418.96
432.87
432.87
482.14
515.53
549.2
549.54
549.54
552.95
552.95
587.56
594.21
594.21
654.41
654.41
753.18

Point group

point_group_type: -3

Visualize Phonons here
Phonon mode (cm-1) Representation
-0.41
-0.4052634901
-0.14
-0.144345269
-0.13
-0.1328602985
84.28
84.2763560651
95.41
95.4056391571
105.38
105.381547184
112.88
112.87752783
114.99
114.989012371
126.16
126.1642533
137.78
137.777379641
151.23
151.231513601
161.61
161.614790164
167.14
167.137482033
186.7
186.70416071
191.4
191.395881086
249.57
249.56856667
251.63
251.632158134
254.89
254.8873788
257.07
257.073864097
327.65
327.645943179
331.68
331.681321522
334.46
334.463881229
363.27
363.267514346
373.07
373.067341602
380.89
380.888324792
394.93
394.927940851
395.2
395.200617749
406.41
406.412729221
418.28
418.28084371
430.27
430.272859762
481.52
481.515986354
515.25
515.249674501
548.29
548.289496364
549.26
549.262118312
552.75
552.748429048
587.48
587.478841866
593.72
593.7177648
653.79
653.789009764
753.06
753.064312074

Thermoelectric properties [Reference]

Thermoelectric properties are calculated using BoltzTrap code [Source-code]. Electron and hole mass tensors (useful for semiconductors and insulators mainly)are given at 300 K [Source-code]. Following plots show the Seebeck coefficient and ZT factor (eigenvalues of the tensor shown) at 300 K along three different crystallographic directions. Seebeck coefficient and ZT plots can be compared for three different temperatures available through the buttons given below. Generally very high Kpoints are needed for obtaining thermoelectric properties. We assume the Kpoints obtained from above convergence were sufficient [Source-code].

WARNING: Constant relaxation time approximation (10-14 s) and only electronic contribution to thermal conductivity were utilized for calculating ZT.

Electron mass tensor (me unit)

0.0 -0.0 -0.0
-0.0 0.0 -0.0
-0.0 -0.0 0.0

Hole mass tensor (me unit)

0.0 -0.0 -0.0
-0.0 0.0 -0.0
-0.0 -0.0 0.0

n-& p-type Seebeck coeff. (µV/K), power-factor (µW/(mK2)), conductivity (1/(*m)), zT (assuming lattice part of thermal conductivity as 1 W/(mK)) at 600K and 1020 cm-3 doping. For mono/multi-layer materials consider Seebeck-coeff only.)

Property xx yy zz
n-Seebeck -59.14 -59.14 -3.61
n-PowerFactor 0.74 82.03 82.03
n-Conductivity 23453.57 23453.59 56607.73
n-ZT 0.0 0.04 0.04
p-Seebeck -56.61 -56.61 -0.52
p-PowerFactor 0.02 72.54 72.54
p-Conductivity 22636.44 22636.45 56696.79
p-ZT 0.0 0.03 0.03

Magnetic moment [Reference]

The orbital magnetic moment was obtained after SCF run. This is not a DFT+U calculation, hence the data could be used to predict zero or non-zero magnetic moment nature of the material only.

Total magnetic moment: 0.9976 μB

Magnetic moment per atom: 0.0525052631579 μB

Magnetization
Elementsspdtot
O0.00.0010.00.001
O0.00.00.00.0
O0.00.0010.00.001
O0.00.0010.00.001
O0.00.00.00.0
O0.00.0010.00.001
O0.00.0230.00.024
O0.00.0240.00.025
O0.00.0250.00.025
O0.00.0230.00.024
O0.00.0240.00.025
O0.00.0250.00.025
Tm0.0010.0040.0040.01
Tm0.0020.0040.0050.012
Tm0.0030.0040.0050.011
Tm0.0010.0040.0040.01
Tm0.0020.0040.0050.012
Tm0.0030.0040.0050.011
Re0.0080.0060.7260.739

See also

Links to other databases or papers are provided below


mp-10342

ICSD-ID: 88796

AFLOW link

MP link
mp-10342

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