2017
DOI: 10.1016/j.hedp.2017.09.002
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Measurement and simulation of the temperature evolution of a short pulse laser heated buried layer target

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Cited by 4 publications
(2 citation statements)
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“…Despite extensive research on isochoric heating of thin solid targets over the last two decades, there is no consensus on the dominant heating mechanism among resistive heating 16,17,18,19,20 , drag heating 21,22,23,24,25,26,27,28 , diffusion 1,3,29 , and both drag and resistive heating 30,31,32,33,34 . The current puzzle is that bulk electron temperatures (Te) estimated span a wide range from tens of eV to 5 keV 35 at similar laser and target conditions.…”
mentioning
confidence: 99%
“…Despite extensive research on isochoric heating of thin solid targets over the last two decades, there is no consensus on the dominant heating mechanism among resistive heating 16,17,18,19,20 , drag heating 21,22,23,24,25,26,27,28 , diffusion 1,3,29 , and both drag and resistive heating 30,31,32,33,34 . The current puzzle is that bulk electron temperatures (Te) estimated span a wide range from tens of eV to 5 keV 35 at similar laser and target conditions.…”
mentioning
confidence: 99%
“…Even with the short laser duration, the backlighter emission may last a few tens of ps. 11 The technique centers on changes to the K I edge or L II/III edge absorption features as a sample is heated to a high degree of ionization. A similar technique was demonstrated with Al heated directly by a 300 fs laser.…”
Section: B Motivation For a Short Pulse Low Z Backlightermentioning
confidence: 99%