2016
DOI: 10.1038/srep22150
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Dense blocks of energetic ions driven by multi-petawatt lasers

Abstract: Laser-driven ion accelerators have the advantages of compact size, high density, and short bunch duration over conventional accelerators. Nevertheless, it is still challenging to simultaneously enhance the yield and quality of laser-driven ion beams for practical applications. Here we propose a scheme to address this challenge via the use of emerging multi-petawatt lasers and a density-modulated target. The density-modulated target permits its ions to be uniformly accelerated as a dense block by laser radiatio… Show more

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Cited by 28 publications
(20 citation statements)
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References 52 publications
(101 reference statements)
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“…It is worthwhile to notice that in the above 3D simulation the laser pulse already has a peak power of 10 PW, and this pulse has been converted into circularly polarized sub-pulses by a magnetized plasma on the centimeter scale (a waist of 0.68 cm). The resultant high-power circularly polarized pulses are particularly attractive to the laser-driven ion acceleration [26,27], the optical control of mesoscopic objects [28], and the ultrahigh acceleration of plasma blocks for fusion ignition [17][18][19]29].…”
Section: Discussionmentioning
confidence: 99%
“…It is worthwhile to notice that in the above 3D simulation the laser pulse already has a peak power of 10 PW, and this pulse has been converted into circularly polarized sub-pulses by a magnetized plasma on the centimeter scale (a waist of 0.68 cm). The resultant high-power circularly polarized pulses are particularly attractive to the laser-driven ion acceleration [26,27], the optical control of mesoscopic objects [28], and the ultrahigh acceleration of plasma blocks for fusion ignition [17][18][19]29].…”
Section: Discussionmentioning
confidence: 99%
“…The replenishment of cold electrons in the NCD plasma plays a crucial role for suppressing the plasma heating. In Figure 3a without the NCD plasma, the plasma temperature is as high as tens of m e c 2 , where the plasma temperature T e in PIC simulations is defined by the averaged kinetic energy of electrons in the center-of-momentum frame [46]. This considerable plasma heating causes the thermal expansion of the plasma and the decrease in the plasma density, which is indicated by the black and blue lines in Figure 3a.…”
Section: Particle-in-cell Simulation Resultsmentioning
confidence: 97%
“…A1D3V PIC simulation code 34 has been performed to verify the formation mechanism of the shocks. Two identical plasma flows are counter-propagating.…”
Section: Methodsmentioning
confidence: 99%