2007
DOI: 10.1016/j.apsusc.2007.01.077
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Dynamics of plume and crater formation after action of femtosecond laser pulse

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Cited by 58 publications
(31 citation statements)
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“…The results of earlier MD simulations of laser irradiation of bulk molecular targets, 16,17,29,67 metal films, 50,68-70 bulk metal targets, 16,71 and systems where interatomic interaction is described by LennardJones potential [72][73][74] suggest that the photomechanical spallation is a general process that can occur in a wide class of materials and different types of targets. The mechanisms of spallation are found to be similar in molecular and metal targets and are described in detail in ref 16.…”
Section: From Melting To Spallation and Phase Explosionmentioning
confidence: 99%
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“…The results of earlier MD simulations of laser irradiation of bulk molecular targets, 16,17,29,67 metal films, 50,68-70 bulk metal targets, 16,71 and systems where interatomic interaction is described by LennardJones potential [72][73][74] suggest that the photomechanical spallation is a general process that can occur in a wide class of materials and different types of targets. The mechanisms of spallation are found to be similar in molecular and metal targets and are described in detail in ref 16.…”
Section: From Melting To Spallation and Phase Explosionmentioning
confidence: 99%
“…The transition from spallation to phase explosion can also be related to the experimental observation of the disappearance of optical interference patterns (Newton rings), observed in pump-probe experiments, 74,82 with an increase in laser fluence. The observation of the Newton rings has been explained by the spallation of a thin liquid layer from the irradiated target, 16,73,83 whereas the disappearance of the interference fringes in the central part of the laser spot 74 may be related to the transition to the phase explosion regime.…”
Section: From Melting To Spallation and Phase Explosionmentioning
confidence: 99%
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“…Above this limit, cohesive property is weak against strong stretching in a hydrodynamic rarefaction waveexpansion proceeds similar to expansion of heated gas (that is, without spallative plate). The cohesive property is responsible for creation of a spallative plate and spallative cupola [16]. The cupola is necessary for the interference which results in appearance of the varying in time Newton rings [16].…”
Section: Introductionmentioning
confidence: 99%
“…The cohesive property is responsible for creation of a spallative plate and spallative cupola [16]. The cupola is necessary for the interference which results in appearance of the varying in time Newton rings [16].…”
Section: Introductionmentioning
confidence: 99%