Energetic ²³²U, ^236,238Pu, ²⁴²Cm, ²⁴⁸Bk, ^250,252Cf and ²⁵²Es nuclei used in nuclear batteries were produced by using particle accelerators for proton, deuteron, triton, helium-3 and alpha-induced reaction processes on thin targets. The energy range used was E_particle = 100 → 1 MeV, including specific conditions such as irradiation time of 24 h with constant beam current of 1 μA. The impressive results were obtained in terms of charged-induced reaction processes, based on simulated activity and yield of product curves. In addition, the significance of these results was discussed for each reaction process so as to determine the appropriate reaction process in detail and add nuclear data to the literature. Also, obtaining these radioisotopes has loud economic cost and restrictions of target materials. Therefore, target materials in production processes were carried out in thin targets to provide convenience to experimenters.

^{核电池中使用的}高能²³² U，^{236 238} Pu，²⁴² Cm，²⁴⁸ Bk，^250,252 Cf和²⁵² Es核是通过使用质子，氘核，^ton核，氦3和α诱导的薄靶上的反应过程产生的。使用的能量范围是E_粒子 = 100→1 MeV，包括特定条件，例如24 h的照射时间和1μA的恒定束电流。基于模拟的活性和产物曲线的产率，在带电诱导的反应过程方面获得了令人印象深刻的结果。此外，讨论了这些结果对每个反应过程的意义，以便详细确定合适的反应过程并将核数据添加到文献中。而且，获得这些放射性同位素具有巨大的经济成本和靶材料的限制。因此，生产过程中的靶材是在薄靶材中进行的，以方便实验人员。