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Structural formula: ZrNi

Force-field: Ni-Zr_Mendelev_2014.eam.fs

Space group : Cmcm

JARVIS ID: JLMP-1665

Download input files

Elastic tensor (GPa)

Elastic tensor for the conventional cell of the system were calculated with LAMMPS in.elastic script at 0 K [Source] . Similar script can be used for temperature dependent elastic constants and will be available here soon. WARNING! Please note that the starting lattice parameters of crystal structures were taken from density functional theory (DFT) and not from experiments. Generic minimization parameters were chosen for LAMMPS run rather than testing them for each individual case such as energy convergence criterion and so on. Hence, there are chances that the calculation gets trapped in a local energy minima. Please read carefully the assumptions taken during calculations in the in.elastic script and use the data at your own risk

328.3 175.0 190.6 -0.0 0.0 0.0
175.0 323.7 175.1 0.0 0.0 0.0
190.6 175.1 212.2 0.0 0.0 0.0
-0.0 0.0 0.0 74.6 0.0 -0.0
0.0 0.0 0.0 0.0 92.0 0.0
0.0 0.0 0.0 -0.0 0.0 75.3

Bv: 216.2 GPa

Gv: 69.9 GPa

Vacancy-formation energy (eV)

Vacancy formation energies were calculated by deleting the symmterically distinct atoms in the system [Source]. In the table, vacancy forming element, its multiplicity, and defect-formation energy are given. The reference element cohesive energies were calculated with the most stable structure for the element found on materials project database. Defect structures were constructed with the fully-relaxed bulk system as input. For defect-structures energetics calculations, constant volume ensemble was used. We impose the defect structures to be at least 1.5 nm large in all directions.

Element Mult. Value
Zr 4 5.48 Download cif file
Ni 4 1.654 Download cif file

Surface energy (J/m2)

Surface energies were calculated for symmterically distinct crystal surfaces . In the table, (hkl) indices and surface enegies are given. For surface-structure energetics, constant volume ensemble was used. We impose the slab thickness to be at least 2 nm and vaccum size of 2.5 nm. The maximum miller index is taken as 3.

Surface Value
(2 1 2) 1.7 Download cif file
(3 1 3) 1.707 Download cif file
(1 0 1) 1.711 Download cif file
(1 3 0) 1.746 Download cif file
(0 0 1) 1.775 Download cif file
(2 0 3) 1.806 Download cif file
(0 1 1) 1.807 Download cif file
(0 3 1) 1.811 Download cif file
(0 1 3) 1.815 Download cif file
(1 1 2) 1.815 Download cif file
(2 3 2) 1.822 Download cif file
(0 2 3) 1.824 Download cif file
(3 2 3) 1.83 Download cif file
(1 1 3) 1.834 Download cif file
(1 0 2) 1.835 Download cif file
(1 2 2) 1.84 Download cif file
(2 3 3) 1.841 Download cif file
(1 0 3) 1.847 Download cif file
(3 1 2) 1.85 Download cif file
(2 1 3) 1.853 Download cif file
(3 0 2) 1.858 Download cif file
(3 2 2) 1.876 Download cif file
(2 2 3) 1.877 Download cif file
(1 3 3) 1.879 Download cif file
(0 3 2) 1.884 Download cif file
(0 1 0) 1.898 Download cif file
(1 2 0) 1.911 Download cif file
(2 0 1) 1.914 Download cif file
(1 0 0) 1.917 Download cif file
(1 2 3) 1.921 Download cif file
(2 3 1) 1.928 Download cif file
(1 3 2) 1.933 Download cif file
(3 0 1) 1.939 Download cif file
(0 1 2) 1.944 Download cif file
(2 2 1) 1.948 Download cif file
(3 3 2) 1.95 Download cif file
(2 3 0) 1.955 Download cif file
(2 1 1) 1.976 Download cif file
(1 2 1) 2.001 Download cif file
(3 1 0) 2.006 Download cif file
(3 2 0) 2.011 Download cif file
(3 2 1) 2.013 Download cif file
(2 1 0) 2.021 Download cif file
(3 1 1) 2.048 Download cif file
(3 3 1) 2.058 Download cif file
(1 1 0) 2.1 Download cif file
(1 1 1) 2.109 Download cif file
(1 3 1) 2.207 Download cif file
(0 2 1) 2.347 Download cif file

Phonon

Phonons were obtained by making an interface of JARVIS-FF with Phonopy package at 0 K [Source] . For deformed-structures, constant volume ensemble was used. The deofrmed structures were taken of at least 1.5 nm size in all directions. The band-indices for phonon bandstructure was obtained with Pymatgen. The phonon representation were obtained with phonopy. "I" and "R" denotes infrared and Raman active modes respectively

Visualize Phonons here
Phonon mode (cm-1) Representation
-8.29876e-05 None
137.637974228 B3g R
156.462757958 B2g R
168.088395808 Ag R
180.89831921 B3u I
181.280823997 B3g R
188.724598112 B1u I
208.574785354 B2u I
223.02829112 Ag R
227.532555944 B2g R
All phonon mode at Gamma point (cm-1)
-8.30247e-05
-4.78826e-05
-1.08658e-05
90.9056026584
92.9104283401
101.105949975
109.054041544
137.637974228
152.692356731
154.953241986
156.462757958
168.088395808
173.579709752
177.163771814
180.89831921
181.280823997
188.724598112
190.376733924
206.98812521
208.574785354
213.695100096
223.02829112
226.555988514
227.532555944

See also

Links to other databases or papers are provided below

JVASP-14779

mp-556

Energy above hull from mp (eV): 0.0