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Proton-induced secondary electron emission from elemental solids over the energy domain 1?keV–1000?MeV

机译:质子在能量范围1?keV–1000?MeV范围内由元素固体产生的二次电子发射

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We propose a new model to calculate the proton-induced secondary electron yield (SEY) from elemental solids. The model combines the stopping power formula generated by Lindhard dielectric response function and a modified version of Bethe formula for electron stopping. The former works well at low energies while the latter at high energies. The present work further modifies the Bethe formula to adapt it to the proton stopping to complement the stopping formula generated by the dielectric theory. The combination of the stopping power formulae of the dielectric and Bethe theories are connected with the SEY formula of Batrakin et al. [Sov. Phys. JETP 62(3) (1985) 633–634] to frame the present new model. The proposed model is applied to calculate the SEY values of 18 elements with atomic numbersZt?=?3–83 over a broad energy domain 1?keV–1000?MeV. The present results show a reasonable agreement with the available experimental data and other calculations. Universal curves of the normalized SEY values against the reduced energy is drawn to verify the validity of our calculations.
机译:我们提出了一个新的模型,可以从元素固体中计算质子诱导的二次电子产率(SEY)。该模型结合了Lindhard介电响应函数生成的停止功率公式和电子停止的Bethe公式的修改版本。前者在低能量下工作良好,而后者在高能量下工作。本工作进一步修改了贝特公式,使其适应质子停止,以补充介电理论生成的停止公式。电介质的停止功率公式和Bethe理论的组合与Batrakin等人的SEY公式有关。 [Sov。物理JETP 62(3)(1985)633–634]构成了目前的新模型。所提出的模型用于计算18个元素的SEY值,其原子序数Zt?=?3-83在宽1?keV–1000?MeV的能量范围内。目前的结果表明与可用的实验数据和其他计算有合理的一致性。绘制归一化的SEY值相对于降低的能量的通用曲线,以验证我们计算的有效性。

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