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Structural formula: Na4 Cd1 P2

Functional: optB88-vDW

Space group : P3m1

Calculation type: 1L

JARVIS ID: JVASP-13646

Formation energy/atom (eV): -0.303

Relaxed energy/atom (eV): -0.5359

Primitive cell lattice parameters

a 4.938 Å , b 4.938 Å , c 29.805 Å

α 90.0 ° , β 90.0 ° , γ 120.0 °

Conventional cell lattice parameters

a 4.938 Å , b 4.938 Å , c 29.805 Å

α 90.0 ° , β 90.0 ° , γ 120.0 °

Download input files

Convergence

Calculations are done using VASP software. Convergence on KPOINTS and ENCUT 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 (nuber of ionic steps,NSW=1). However, for very accurate calculations, NSW>1 might be needed.

Structural analysis

The following shows the X-ray diffraction (XRD) pattern and the Radial distribution function (RDF) plots. XRD peaks should be comparable to experiments for bulk structures. Relative intensities may differ.

Optical properties Semi-local

Incident photon energy dependence of optical is shown below. 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 layered materials needs to be rescaled with the actual thickness to simulation z-box ratio. Absorption coeffiecient is in cm-1 unit.

Dense k-mesh based bandgap is : 0.9809 eV

Elastic tensor and derived phonon properties

Elastic tensor calculated for the conventional cell of the system with finite-difference method. 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 from this calcuation are also shown.

WARNING: Please note this may not be the exact phonon modes of the system as we did not test the cell-size dependence of phonons yet. At least 1.2 nm x1.2 nm x1.2 nm or more is needed for obtaining reliable phonon spectrum. For systems having primitive-cell phonon representation tables, I denotes infrared activity and R denotes Raman active modes (where applicabale). The minimum thermal conductivity was calculated using elastic tensor information following Clarke and Cahill formalism.

Bulk Modulus BV 10.356 GPa

Shear Modulus GV 6.093 GPa

41.3 8.6 -2.3 -0.0 -0.3 -0.0
8.6 41.3 -2.3 -0.0 0.3 -0.0
-0.8 -0.8 -0.4 -0.0 -0.0 -0.0
-0.0 -0.0 -0.0 5.5 0.0 -0.1
-0.1 0.1 -0.0 0.0 -0.3 -0.0
-0.0 -0.0 -0.0 -0.1 -0.0 -0.3
Phonon mode (cm-1)
-17.6032476313
-0.3041137814
-0.3029098758
33.9856389929
33.9856452459
86.3302590565
86.3302617484
93.9403733061
104.236085802
119.503604525
134.939045348
185.044017829
185.044022669
186.017109891
186.017113846
208.990021537
208.990025326
216.092907748
216.092913629
286.783354815
340.212618143

Point group

point_group_type: 3m

Visualize Phonons here
Phonon mode (cm-1) Representation
-17.6032476313 A1 I+R
-0.3041137814 None
-0.3029098759 None
33.9856389929 E I+R
86.3302590565 E I+R
93.9403733061 A1 I+R
104.236085802 A1 I+R
119.503604525 A1 I+R
134.939045348 A1 I+R
185.044017829 E I+R
186.017109891 E I+R
208.990021537 E I+R
216.092907748 E I+R
286.783354815 A1 I+R
340.212618143 A1 I+R

Magnetic moment

The orbital magnetic moment was obtained after SCF run. Please note no DFT+U parameters were taken into account.

-0.001 μB

Reference


mp-8752-1L
mp-8752-1L

ICSD-ID: None