首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. B, Beam Interactions with Materials and Atoms >Analysis of the projectile track charging by H~+ secondary ion velocity distribution measurements
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Analysis of the projectile track charging by H~+ secondary ion velocity distribution measurements

机译:通过H〜+二次离子速度分布测量分析弹道电荷

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摘要

Secondary ions, emitted from LiF, Al (covered with layers of Al_2O_3) and Au bombarded by a MeV argon (25 keV/u) beam, are analyzed by a XY-TOF detection system. This new method allows, for each emitted ion, the simultaneous measurement of its time-of flight (TOF) and its impact coordinates (XY) on the detector surface, after acceleration by a homogenous electric field. Angular distributions and initial velocities for atomic H~+ secondary ions are determined as a function of the projectile impact angle θ_p (31° up to 78°, with respect to the surface normal) and the electrical surface target properties. Emission of low velocity H~+ ions (υ_0 < 30 km/s) occurs preferentially close to the line of incidence of the projectile. Their initial velocity distribution depends clearly on the target electrical conductivity. At constant θ_f, the maximum of the velocity distribution, υ_0~(max), is found to be 26.5, 27.9 and 32.5 km/s for Au, Al and LiF targets, respectively. For Au target, no clear dependence on the impact angle θ_p was found. However, increasing θ_p from 37° to 78° υ_0~(max) shifts from 27.9 to 30 km/s for Al and 32.5-35.5 km/s for LiF. This shift is explained by a transient positive charging up of the nuclear track and is an indication of the track potential decay. The dependence of υ_0 on θ_p is explained by the variation of the length of the track inside the insulator layer, once neutralization time is assumed to be dependent on the electron current inside the track of the insulator layers from a conducting substrate.
机译:由LiF,Al(被Al_2O_3覆盖)和被MeV氩气(25 keV / u)轰击的Au发射的二次离子通过XY-TOF检测系统进行分析。这种新方法允许在均匀电场加速后,对每个发射离子同时测量其飞行时间(TOF)和在检测器表面上的碰撞坐标(XY)。原子H〜+次级离子的角分布和初始速度取决于弹丸撞击角θ_p(相对于表面法线从31°到78°)和电子表面目标属性确定。低速H〜+离子(υ_0<30 km / s)的发射优先发生在弹丸的入射线附近。它们的初始速度分布显然取决于目标电导率。在常数θ_f下,发现Au,Al和LiF目标的速度分布最大值υ_0〜(max)分别为26.5、27.9和32.5 km / s。对于金靶,没有发现对冲击角θ_p的明显依赖。但是,将θ_p从37°增大到78°υ_0〜(max)对于Al来说是27.9到30 km / s,对于LiF是32.5-35.5 km / s。这种偏移可以通过核轨道的瞬时正充电来解释,并且是轨道电位衰减的指示。一旦假设中和时间取决于来自导电衬底的绝缘体层的迹线内部的电子电流,就可以通过绝缘体层内部的迹线长度的变化来解释υ_0对θ_p的依赖性。

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