1996
DOI: 10.1016/0169-4332(95)00463-7
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Laser-solid interaction and dynamics of laser-ablated materials

Abstract: An annealing model is extended t.0 treat the vaporization process, and a hydrodynamic model describes the ablated material. We find that dynamic source and ionization effects accelerate the expansion front of the ablated plume with thermal vaporization temperature.The vaporization process and plume propagation in high background gas pressure are studied.

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Cited by 38 publications
(6 citation statements)
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“…The electron temperature is in the range of 1-5 eV, and the ion temperature has nearly the same order of magnitude as the electron temperature. However, since the plasma formation area in front of the target is very small and the plasma flux velocity is very large, the formation of a large area uniform laser plasma tends to be difficult in practice [34]. …”
Section: à2mentioning
confidence: 99%
“…The electron temperature is in the range of 1-5 eV, and the ion temperature has nearly the same order of magnitude as the electron temperature. However, since the plasma formation area in front of the target is very small and the plasma flux velocity is very large, the formation of a large area uniform laser plasma tends to be difficult in practice [34]. …”
Section: à2mentioning
confidence: 99%
“…The first one consists of an intense and narrow peak caused by the interaction at the shock front and thus marks the boundary between the plasma region and background gas. 10 The second one is considerably broader and caused by the species ejected from the target at later times. As the delay is increased ͓Figs.…”
mentioning
confidence: 99%
“…Clustering when vapor plume expands into a background oxygen gas, collisions may cause atoms and ions in the plume to coalesce into nm-scale clusters [25]. On the other hand, the roughness starts to decrease after reaching the maximum value, as increasing the number of laser pulses thermal energy of the vapor above the target will increase and hence the plume expands and compresses the background gas, creating a shock-wave which slows the plume expansion [23,26]. As in this work where the targetto-substrate distance is too close, the expanding vapor reaches the substrate with typical energies of 0.1-100 eV per atom [27], depositing sub-monolayer thicknesses of material per pulse.…”
Section: Resultsmentioning
confidence: 99%