Ultrafast solid-liquid-vapor phase change of a thin gold film irradiated by femtosecond laser pulses and pulse trains

Jing HUANG, Yuwen ZHANG, J. K. CHEN, Mo YANG

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PDF(335 KB)
Front. Energy ›› 2012, Vol. 6 ›› Issue (1) : 1-11. DOI: 10.1007/s11708-012-0179-9
FEATURE ARTICLE
FEATURE ARTICLE

Ultrafast solid-liquid-vapor phase change of a thin gold film irradiated by femtosecond laser pulses and pulse trains

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Abstract

Effects of different parameters on the melting, vaporization and resolidification processes of thin gold film irradiated by femtosecond pulses and pulse train were systematically studied. The classical two-temperature model was adopted to depict the non-equilibrium heat transfer in electrons and lattice. The melting and resolidification processes, which was characterized by the solid-liquid interfacial velocity, as well as elevated melting temperature and depressed solidification temperature, was obtained by considering the interfacial energy balance and nucleation dynamics. Vaporization process which leads to ablation was described by tracking the location of liquid-vapor interface with an iterative procedure based on energy balance and gas kinetics law. The parameters in discussion included film thickness, laser fluence, pulse duration, pulse number, repetition rate, pulse train number, etc. Their effects on the maximum lattice temperature, melting depth and ablation depth were discussed based on the simulation results.

Keywords

melting / evaporation / nucleation dynamics / nanoscale heat transfer

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Jing HUANG, Yuwen ZHANG, J. K. CHEN, Mo YANG. Ultrafast solid-liquid-vapor phase change of a thin gold film irradiated by femtosecond laser pulses and pulse trains. Front Energ, 2012, 6(1): 1‒11 https://doi.org/10.1007/s11708-012-0179-9

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Acknowledgments

This work was supported by the U.S. National Science Foundation (NSF) (Grant No. CBET-0730143) and the National Natural Science Foundation of China (Grant No. 51129602).
Notations
BeCoefficient for electron heat capacity/(J·m-3·K-2)
CHeat capacity/(J·m-3·K-1)
cpspecific heat/(J·kg-1·K-1)
frepRepetition rate/Hz
Gelectron-lattice coupling factor/(W·m-3·K-1)
hLatent heat of phase change/(J·kg-1)
JiSingle pulse fluence/(J·cm-2)
JtTotal energy of a pulse train/(J·cm-2)
kThermal conductivity/(W·m-1·K-1)
LThickness of the metal film/m
MMolar mass/(kg·kmol-1)
q''Heat flux/(W·m-2)
RReflectivity
RgSpecific gas constant/(J·kg-1·K-1)
RuUniversal gas constant/(J·kmol-1·K-1)
sInterfacial location/m
SIntensity of the internal heat source/(W·m-3)
tTime/s
tpPulse width/s
tsepSeparation time/s
TTemperature/K
TFFermi temperature/K
TmMelting point/K
uInterfacial velocity/(m·s-1)
V0Interfacial velocity factor/(m·s-1)
xCoordinate/m
Greek Symbols
δOptical penetration depth/m
δbBallistic range/m
ϵTotal emissivity
ρDensity/(kg·m-3)
σStefan-Boltzmann constant/(W·m-2·K-4)
Superscripts
0Last time step
Subscripts
0Initial condition
eElectron
eqThermal equilibrium state
iPulse sequence
lLattice
Liquid
RThermal radiation
sSolid
surSurface
Ambient environment

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