2003
DOI: 10.1080/716100504
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Heat Transfer in Femtosecond Laser Processing of Metal

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Cited by 133 publications
(58 citation statements)
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“…Various descriptions of melting, resolidification, surface vaporization, and ablation can be incorporated into such models, albeit at a rather simplified level. In particular, laser melting and resolidification are often described with a phase-change model based on an assumption of local equilibrium at the solid-liquid interface (heat-flow limited, interface kinetics formulated within the framework of the Stephan problem), e.g., [37][38][39], or using a kinetic equation relating the interface velocity to the interface temperature, e.g., [40][41][42][43][44]. The latter nonequilibrium kinetic description has been shown to be necessary for subnanosecond pulses, when a fast thermal energy flow to/from the liquid-solid interface creates conditions for significant overheating/undercooling of the interface [43,44].…”
Section: Introductionmentioning
confidence: 99%
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“…Various descriptions of melting, resolidification, surface vaporization, and ablation can be incorporated into such models, albeit at a rather simplified level. In particular, laser melting and resolidification are often described with a phase-change model based on an assumption of local equilibrium at the solid-liquid interface (heat-flow limited, interface kinetics formulated within the framework of the Stephan problem), e.g., [37][38][39], or using a kinetic equation relating the interface velocity to the interface temperature, e.g., [40][41][42][43][44]. The latter nonequilibrium kinetic description has been shown to be necessary for subnanosecond pulses, when a fast thermal energy flow to/from the liquid-solid interface creates conditions for significant overheating/undercooling of the interface [43,44].…”
Section: Introductionmentioning
confidence: 99%
“…In particular, laser melting and resolidification are often described with a phase-change model based on an assumption of local equilibrium at the solid-liquid interface (heat-flow limited, interface kinetics formulated within the framework of the Stephan problem), e.g., [37][38][39], or using a kinetic equation relating the interface velocity to the interface temperature, e.g., [40][41][42][43][44]. The latter nonequilibrium kinetic description has been shown to be necessary for subnanosecond pulses, when a fast thermal energy flow to/from the liquid-solid interface creates conditions for significant overheating/undercooling of the interface [43,44]. The material removal from the target can be incorporated into continuum models in the form of surface or volumetric vaporization models, e.g., [45][46][47][48][49], whereas the expansion of the vaporized plume is commonly described by solving gas dynamics equations, e.g., [45][46][47][48][49] or using the Direct Simulation Monte Carlo (DSMC) technique, e.g., [50][51][52][53][54][55].…”
Section: Introductionmentioning
confidence: 99%
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“…thermal explosion basing on the existing quantum Two Temperature Model (TTMq) [5,7,8]. But the problem is that this model does not give any information on the ablation state at low fluence (aroud ablation thershold), also the phase explosion model does not explane the absense of liquid around the crater at low fluence.…”
Section: Introductionmentioning
confidence: 99%
“…It should be noted that the explosive-type vaporization (e.g. [4,5]) is not considered here. At the stage of numerical computations the algorithm based on the explicit scheme of the finite difference method with the staggered grid [6,7] is used.…”
Section: Introductionmentioning
confidence: 99%