2012
DOI: 10.1063/1.4745867
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Experimental and computational study of complex shockwave dynamics in laser ablation plumes in argon atmosphere

Abstract: We investigated spatio-temporal evolution of ns laser ablation plumes at atmospheric pressure, a favored condition for laser-induced breakdown spectroscopy and laser-ablation inductively coupled plasma mass-spectrometry. The 1064 nm, 6 ns pulses from a Nd:YAG laser were focused on to an Al target and the generated plasma was allowed to expand in 1 atm Ar. The hydrodynamic expansion features were studied using focused shadowgraphy and gated 2 ns self-emission visible imaging. Shadowgram images showed material e… Show more

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Cited by 194 publications
(103 citation statements)
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References 48 publications
(66 reference statements)
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“…The shock front is a region characterized by strong gradients of temperature, velocity and pressure, where clustering of the ablated species can occur in out-of-equilibrium conditions [39][40][41][42].…”
Section: Figure 3 Cross Sectional Sem Images Of Carbon Pld Films On mentioning
confidence: 99%
“…The shock front is a region characterized by strong gradients of temperature, velocity and pressure, where clustering of the ablated species can occur in out-of-equilibrium conditions [39][40][41][42].…”
Section: Figure 3 Cross Sectional Sem Images Of Carbon Pld Films On mentioning
confidence: 99%
“…However, multidimensional numerical simulations of fl uid dynamics can bring yet unexplored insight into such complex physical phenomena. For example, shock-wave propagation after pulsed laser irradiation of Al targets under the atmospheric pressure conditions was studied by Harilal et al [8] employing unsteady solver of Navier-Stokes equations in a two-dimensional axially symmetric geometry.…”
Section: Introductionmentioning
confidence: 99%
“…The decrease of ambient gas density close to the target surface would lead to a decrease of laser shielding by the pre-plasma thereby determining an increase of the laser ablation and signal enhancement [10]. The shockwave front detaches from the plume front after few hundreds of ns and moves further, while the plume core gets stagnant at few mm from the plasma surface depending on the laser pulse energy [10,47]. At higher interpulse delays (>500 ns), optimal rarified regions are generated which lead to a signal enhancement mostly due to increased mass ablation.…”
Section: Accepted Manuscriptmentioning
confidence: 99%