2014
DOI: 10.1017/hpl.2014.46
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Optimization of relativistic laser–ion acceleration

Abstract: Experiments have shown that the ion energy obtained by laser-ion acceleration can be optimized by choosing either the appropriate pulse duration or the appropriate target thickness. We demonstrate that this behavior can be described either by the target normal sheath acceleration model of Schreiber et al. or by the radiation pressure acceleration model of Bulanov and coworkers. The starting point of our considerations is that the essential property of a laser system for ion acceleration is its pulse energy and… Show more

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Cited by 13 publications
(5 citation statements)
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“…Due to the strong dependence of E max on both the intensity and focal spot size, it would be more appropriate to compare the data plotted in Figure 2 as a function of laser energy. 37 Except for three points, the short pulse data agree well with the simulations. Moreover, they follow a power dependence of the form E max $ e 3=5 , identical to that predicted by the PIC simulations.…”
Section: Maximum Proton Energy Versus Laser Energysupporting
confidence: 70%
“…Due to the strong dependence of E max on both the intensity and focal spot size, it would be more appropriate to compare the data plotted in Figure 2 as a function of laser energy. 37 Except for three points, the short pulse data agree well with the simulations. Moreover, they follow a power dependence of the form E max $ e 3=5 , identical to that predicted by the PIC simulations.…”
Section: Maximum Proton Energy Versus Laser Energysupporting
confidence: 70%
“…Significant progress has been made in this topic (Daido et al 2012;Macchi et al 2013). However, to realize real applications, more efforts are still required to improve the ion beam quality, e.g., enhancing the maximum energy, reducing the beam energy spread, increasing the stability and controllability (Schreiber et al 2014;Wagner et al 2014).…”
Section: Laser-driven Ion Acceleration and Applicationsmentioning
confidence: 99%
“…The interaction of relativistically intense laser pulses with solid targets has stimulated considerable interest because of its practical applications in laser-driven particle acceleration [1][2][3][4][5][6][7] , high-brightness ultrafast hard X-ray and K α source [8][9][10][11] , cancer treatment [12,13] , fast ignition in inertial confinement fusion [14] , etc. A crucial issue, in all these applications, is to produce high-quality forward hot electrons efficiently.…”
Section: Introductionmentioning
confidence: 99%