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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Dynamic response of target electrons on elastic scattering cross sections for heavy-ion impact on a high-Z atom - art. no. 012718
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Dynamic response of target electrons on elastic scattering cross sections for heavy-ion impact on a high-Z atom - art. no. 012718

机译:目标电子在弹性散射截面上对重离子撞击高Z原子的动态响应-艺术没有。 012718

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Large-angle elastic scattering cross sections were measured for medium energy He+ and Ne+ ions impact on Ni, Sb, and Hf atoms and the results are compared with those calculated using screened interatomic potentials. As the screened Coulomb potential, we employed the Moliere, Ziegler-Biersack-Littmark (ZBL), and that calculated numerically by solving the Poisson equation applied to the Hartree-Fock (HF) atomic model. For He+ impact, the ZBL and HF (He2+ is assumed) potentials reproduced well the observed scattering cross sections but the Moliere potential underestimated them significantly. Surprisingly, however, for Ne+ impact on Sb and Hf, the observed scattering cross sections were much larger than those calculated from all the above screened interatomic potentials, although Ne10+ was assumed for the HF potential. In a large-angle collision, a projectile heavy ion attracts the target electrons to distort the electron cloud and as a result it changes the electric field upon the projectile. The observed scattering cross sections are reproduced well by assuming a simple model that the center of gravity of the target electrons slightly shifts toward the projectile by 0.09-0.12 Angstrom for Hf and 0.066-0.070 Angstrom for Sb from the nucleus. [References: 15]
机译:测量大角度弹性散射横截面的中等能量He +和Ne +离子对Ni,Sb和Hf原子的影响,并将结果与​​使用筛选的原子间电势计算的结果进行比较。作为筛选的库仑电势,我们采用了Moliere,Ziegler-Biersack-Littmark(ZBL),并通过求解应用于Hartree-Fock(HF)原子模型的泊松方程进行了数值计算。对于He +冲击,ZBL和HF(假定为He2 +)电势在观察到的散射截面上很好地再现,但Moliere电势显着低估了它们。然而,令人惊讶的是,对于Ne +对Sb和Hf的影响,观察到的散射截面远大于从所有上述筛选的原子间电势计算得出的散射截面,尽管假定HF势假定为Ne10 +。在大角度碰撞中,弹丸重离子吸引目标电子,使电子云变形,结果,它改变了弹丸上的电场。假设一个简单的模型,目标电子的重心从原子核向Hf的偏移为0.09-0.12埃,而从Sb向Sb的偏移为0.066-0.070埃,则可以通过简单的模型很好地再现观察到的散射截面。 [参考:15]

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