Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
DFT-computed cubic BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed wurtzite BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
2 properties
Simulated Supercell DftBNStudied Material
DFT-computed hexagonal BN polymorph BN-Aa used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
6 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-Ab polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
DFT-computed rhombohedral BN polymorph BN-ABC used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-ABb polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
Materials
c-BN
BN
Studied Material
Also known as
cubic BNcubic boron nitride
Variables
bonding= sp3
polytype= cubic
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
DFT-computed cubic BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed wurtzite BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
2 properties
Simulated Supercell DftBNStudied Material
DFT-computed hexagonal BN polymorph BN-Aa used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
6 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-Ab polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
DFT-computed rhombohedral BN polymorph BN-ABC used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-ABb polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
Materials
c-BN
BN
Studied Material
Also known as
cubic BNcubic boron nitride
Variables
bonding= sp3
polytype= cubic
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
DFT-computed cubic BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed wurtzite BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
2 properties
Simulated Supercell DftBNStudied Material
DFT-computed hexagonal BN polymorph BN-Aa used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
6 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-Ab polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
DFT-computed rhombohedral BN polymorph BN-ABC used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-ABb polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
Materials
c-BN
BN
Studied Material
Also known as
cubic BNcubic boron nitride
Variables
bonding= sp3
polytype= cubic
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
DFT-computed cubic BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed wurtzite BN polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
2 properties
Simulated Supercell DftBNStudied Material
DFT-computed hexagonal BN polymorph BN-Aa used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
6 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-Ab polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
DFT-computed rhombohedral BN polymorph BN-ABC used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
4 properties
Simulated Supercell DftBNStudied Material
DFT-computed BN-ABb polymorph used for total-energy, lattice-parameter, zero-point renormalization, and electron-phonon interaction analysis.
3 properties
Simulated Supercell DftBNStudied Material
Materials
c-BN
BN
Studied Material
Also known as
cubic BNcubic boron nitride
Variables
bonding= sp3
polytype= cubic
studied material
Why these are connected
Related documents with shared materials, methods, properties, or citations.
ABINIT DFT total-energy and lattice-parameter calculations with PBE exchange-correlation, ONCV pseudopotentials, and vdW corrections DFT-D3 and DFT-D3(BJ); electron-phonon interaction corrections evaluated with ABINIT TDepES module.ABINIT
Settings
epi moduleTDepES
polymorphsc-BN, w-BN, h-BN, BN-Ab, r-BN, BN-ABb
property scopeBN polymorph energetics
pseudopotentialONCV
vdw approximationsDFT-D3, DFT-D3(BJ)
exchange correlationPBE
Conditions
context:electronic-structure and electron-phonon study of BN polymorph stability
ABINIT DFT total-energy and lattice-parameter calculations with PBE exchange-correlation, ONCV pseudopotentials, and vdW corrections DFT-D3 and DFT-D3(BJ); electron-phonon interaction corrections evaluated with ABINIT TDepES module.ABINIT
Settings
epi moduleTDepES
polymorphsc-BN, w-BN, h-BN, BN-Ab, r-BN, BN-ABb
property scopeBN polymorph energetics
pseudopotentialONCV
vdw approximationsDFT-D3, DFT-D3(BJ)
exchange correlationPBE
Conditions
context:electronic-structure and electron-phonon study of BN polymorph stability
ABINIT DFT total-energy and lattice-parameter calculations with PBE exchange-correlation, ONCV pseudopotentials, and vdW corrections DFT-D3 and DFT-D3(BJ); electron-phonon interaction corrections evaluated with ABINIT TDepES module.ABINIT
Settings
epi moduleTDepES
polymorphsc-BN, w-BN, h-BN, BN-Ab, r-BN, BN-ABb
property scopeBN polymorph energetics
pseudopotentialONCV
vdw approximationsDFT-D3, DFT-D3(BJ)
exchange correlationPBE
Conditions
context:electronic-structure and electron-phonon study of BN polymorph stability
ABINIT DFT total-energy and lattice-parameter calculations with PBE exchange-correlation, ONCV pseudopotentials, and vdW corrections DFT-D3 and DFT-D3(BJ); electron-phonon interaction corrections evaluated with ABINIT TDepES module.ABINIT
Settings
epi moduleTDepES
polymorphsc-BN, w-BN, h-BN, BN-Ab, r-BN, BN-ABb
property scopeBN polymorph energetics
pseudopotentialONCV
vdw approximationsDFT-D3, DFT-D3(BJ)
exchange correlationPBE
Conditions
context:electronic-structure and electron-phonon study of BN polymorph stability