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首页> 外文期刊>Laser and Particle Beams >Collimated proton beams by ultra-short, ultra-intense laser pulse interaction with a foil-ramparts target
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Collimated proton beams by ultra-short, ultra-intense laser pulse interaction with a foil-ramparts target

机译:通过超短,超强激光脉冲与箔状撞击靶准直的质子束

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摘要

A foil-ramparts target interaction with an ultra-short, ultra-intense laser pulse (pulse duration between 10(-12) and 10(-15) s, intensity above 10(18) W cm(-2)) to produce proton beams with controlled divergence and concentrated energy density in target normal sheath acceleration regime is studied. Two-dimension-in-space and three-dimension-in-velocity particle-in-cell simulations show that the foil-ramparts target helps to reshape the sheath electric field and generate a transverse quasi-static electric field of similar to 6.7 TV m(-1) along the inner wall of the ramparts. The transverse electric field suppresses the transverse expansion of the proton beam effectively, as it tends to force the produced protons to focus inwards to the central axis, resulting in controlled divergence and concentrated energy density compared with that of a single plain target. The dependence of proton beam divergence on length of the rampart h is investigated in detail. A rough estimation of h ranges depending on dimensionless parameter a(0) of the incident laser is also given.
机译:箔-撞墙目标与超短,超强激光脉冲(脉冲持续时间在10(-12)和10(-15)s之间,强度在10(18)W cm(-2)以上)相互作用,从而产生质子研究了在目标法向护套加速状态下具有受控发散和集中能量密度的电子束。空间二维和速度三维颗粒模拟表明,箔状撞击靶有助于重塑鞘层电场并产生类似于6.7 TV m的横向准静态电场(-1)沿着城墙的内壁。横向电场有效地抑制了质子束的横向扩展,因为它倾向于迫使产生的质子向内聚焦到中心轴,与单个普通目标相比,可控制的发散和集中的能量密度。详细研究了质子束发散对城墙h长度的依赖性。还给出了取决于入射激光的无量纲参数a(0)的h范围的粗略估计。

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