Torrisi L, Giuffrida L, Cutroneo M, Cirrone P, Picciotto A, Krasa J, Margarone D, Velyhan A, Laska L, Ullschmied J, Wolowski J, Badziak J, Rosinski M
INFN-LNS Via S. Sofia 44, 95123 Catania, Italy.
Rev Sci Instrum. 2012 Feb;83(2):02B315. doi: 10.1063/1.3673506.
The iodine laser at PALS Laboratory in Prague, operating at 1315 nm fundamental harmonics and at 300 ps FWHM pulse length, is employed to irradiate thin hydrogenated targets placed in vacuum at intensities on the order of 10(16) W∕cm(2). The laser-generated plasma is investigated in terms of proton and ion emission in the forward and backward directions. The time-of-flight technique, using ion collectors and semiconductor detectors, is used to measure the ion currents and the corresponding velocities and energies. Thomson parabola spectrometer is employed to separate the contribution of the ion emission from single laser shots. A particular attention is given to the proton production in terms of the maximum energy, emission yield, and angular distribution as a function of the laser energy, focal position, target thickness, and composition. Metallic and polymeric targets allow to generate protons with large energy range and different yield, depending on the laser, target composition, and target geometry properties.
位于布拉格的高功率激光系统实验室的碘激光器,工作在1315纳米基波和谐波,脉冲长度为300皮秒半高宽,用于在真空中以约10(16)瓦/平方厘米的强度照射薄氢化靶。对激光产生的等离子体在向前和向后方向上的质子和离子发射进行了研究。采用飞行时间技术,利用离子收集器和半导体探测器来测量离子电流以及相应的速度和能量。汤姆逊抛物线光谱仪用于分离单次激光脉冲产生的离子发射贡献。特别关注了质子产生的最大能量、发射产额以及作为激光能量、焦点位置、靶厚度和成分函数的角分布。金属靶和聚合物靶能够根据激光、靶成分和靶几何特性产生能量范围大且产额不同的质子。