2022
DOI: 10.48550/arxiv.2211.03090
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Laboratory observation of ion acceleration via reflection off laser-produced magnetized collisionless shocks

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(2 citation statements)
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“…The shock evolution in the simulation shows similar characteristics to our experimental results [31], including the shock Alfvén number (M 7 11 A = -in the experiment), the separation time between the shock and piston ( t 1 cp0 W ~), and the shock structure in figure 3 (obvious 'overshoot', 'ramp', 'foot', etc). Moreover, the energy spectrum of shock-accelerated ions in our simulation is also consistent with our experimental result, which shows a quasi-monoenergetic distribution at about twice the shock velocity [31]. The validity of our simulation is thus proven and we can discuss the details of ion dynamics in this kind of shock below.…”
Section: = -supporting
confidence: 76%
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“…The shock evolution in the simulation shows similar characteristics to our experimental results [31], including the shock Alfvén number (M 7 11 A = -in the experiment), the separation time between the shock and piston ( t 1 cp0 W ~), and the shock structure in figure 3 (obvious 'overshoot', 'ramp', 'foot', etc). Moreover, the energy spectrum of shock-accelerated ions in our simulation is also consistent with our experimental result, which shows a quasi-monoenergetic distribution at about twice the shock velocity [31]. The validity of our simulation is thus proven and we can discuss the details of ion dynamics in this kind of shock below.…”
Section: = -supporting
confidence: 76%
“…These parameters are similar to those applied in shocks produced by the Shengguang II laser facility [31].…”
mentioning
confidence: 74%