Temperature Dependence of Phonon Energies and Lifetimes in Single- and Few-layered Graphene | Matter42 LiteratureSamples
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Related documents with shared materials, methods, properties, or citations.
Samples
5
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Samples
5
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Samples
5
Why these are connected
Related documents with shared materials, methods, properties, or citations.
Pristine monolayer graphene simulated under periodic boundar
md
Calculated PhononCalculated
Conditions
methodk-VACS
outputsphonon dispersion curves,phonon density of states,Γ-point phonon energies,phonon lifetimes
interlayer potentialLJ
a
ngstrom":3.276}
supercell size40x40 primitive cells
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialKolmogorov-Crespi (KC)
intralayer potentialreparametrised Tersoff potential by Broido et al.
frequency resolution cm^-11.1
kc total production time ns3.28
kc production time per run ps327.68
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
classical molecular dynamicsk-space autocorrelation sequence (k-VACS)spectral energy density fitting
Settings
run typeindependent equilibrium NVE runs
stackingBernal (-AB-)
lJ parameters{"epsilonmeV":4.6,"sigmaangstrom":3.276}
supercell size40x40 primitive cells
lattice size nm1
production runs10
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialLennard-Jones (LJ)
intralayer potentialreparametrised Tersoff potential by Broido et al.
kc total production time nsnull
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
resolution note:higher resolution convergence tests performed for 2L case
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
Pristine monolayer graphene simulated under periodic boundar
md
Calculated PhononCalculated
Conditions
methodk-VACS
outputsphonon dispersion curves,phonon density of states,Γ-point phonon energies,phonon lifetimes
interlayer potentialLJ
a
ngstrom":3.276}
supercell size40x40 primitive cells
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialKolmogorov-Crespi (KC)
intralayer potentialreparametrised Tersoff potential by Broido et al.
frequency resolution cm^-11.1
kc total production time ns3.28
kc production time per run ps327.68
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
classical molecular dynamicsk-space autocorrelation sequence (k-VACS)spectral energy density fitting
Settings
run typeindependent equilibrium NVE runs
stackingBernal (-AB-)
lJ parameters{"epsilonmeV":4.6,"sigmaangstrom":3.276}
supercell size40x40 primitive cells
lattice size nm1
production runs10
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialLennard-Jones (LJ)
intralayer potentialreparametrised Tersoff potential by Broido et al.
kc total production time nsnull
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
resolution note:higher resolution convergence tests performed for 2L case
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
Pristine monolayer graphene simulated under periodic boundar
md
Calculated PhononCalculated
Conditions
methodk-VACS
outputsphonon dispersion curves,phonon density of states,Γ-point phonon energies,phonon lifetimes
interlayer potentialLJ
a
ngstrom":3.276}
supercell size40x40 primitive cells
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialKolmogorov-Crespi (KC)
intralayer potentialreparametrised Tersoff potential by Broido et al.
frequency resolution cm^-11.1
kc total production time ns3.28
kc production time per run ps327.68
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
classical molecular dynamicsk-space autocorrelation sequence (k-VACS)spectral energy density fitting
Settings
run typeindependent equilibrium NVE runs
stackingBernal (-AB-)
lJ parameters{"epsilonmeV":4.6,"sigmaangstrom":3.276}
supercell size40x40 primitive cells
lattice size nm1
production runs10
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialLennard-Jones (LJ)
intralayer potentialreparametrised Tersoff potential by Broido et al.
kc total production time nsnull
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
resolution note:higher resolution convergence tests performed for 2L case
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
Pristine monolayer graphene simulated under periodic boundar
md
Calculated PhononCalculated
Conditions
methodk-VACS
outputsphonon dispersion curves,phonon density of states,Γ-point phonon energies,phonon lifetimes
interlayer potentialLJ
a
ngstrom":3.276}
supercell size40x40 primitive cells
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialKolmogorov-Crespi (KC)
intralayer potentialreparametrised Tersoff potential by Broido et al.
frequency resolution cm^-11.1
kc total production time ns3.28
kc production time per run ps327.68
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
classical molecular dynamicsk-space autocorrelation sequence (k-VACS)spectral energy density fitting
Settings
run typeindependent equilibrium NVE runs
stackingBernal (-AB-)
lJ parameters{"epsilonmeV":4.6,"sigmaangstrom":3.276}
supercell size40x40 primitive cells
lattice size nm1
production runs10
boundary conditionsperiodic boundary conditions
temperature range k80, 1000
interlayer potentialLennard-Jones (LJ)
intralayer potentialreparametrised Tersoff potential by Broido et al.
kc total production time nsnull
lJ production time per run ps655.36
velocity sampling interval fs5
velocity sampling interval timesteps10
Conditions
resolution note:higher resolution convergence tests performed for 2L case
relaxation sequence:conjugate gradient static energy minimization, 125 ps NVE equilibration, 250 ps NPT structural relaxation, 125 ps NVT thermal equilibration
Bulk graphite in Bernal (-AB-) stacking.
Bulk graphite in Bernal (-AB-) stacking.
Bulk graphite in Bernal (-AB-) stacking.
Bulk graphite in Bernal (-AB-) stacking.