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本文描述的带电粒子(Z<4)分辨线路所实现的函数式为T/a=(E+△E+C)~b-(E+C)~b,式中E和△E分别为粒子在厚和薄探测器中的能量损耗,T为薄探测器厚度,C为在低能范围(<10MeV)内加入的校正项,b为常数(1.73左右,可调),a为与粒子本身有关的常数。本仪器对V_o=V_i~b的运算精度小于1.5%(V_i,V_o分别为输入和输出电压),温度稳定性小于0.15%/℃(20～45℃)。
The function of the realization of the charged particles (Z <4) described in this paper is T / a = (E + △ E + C) ~ b- (E + C) ~ b, where E and △ E are the particles in T is the thin detector thickness, C is the correction term added in the low energy range (<10 MeV), b is a constant (about 1.73, adjustable), a is the energy loss associated with the particle itself constant. The accuracy of V_o = V_i ~ b is less than 1.5% (V_i, V_o are input and output voltage respectively). The temperature stability is less than 0.15% / ℃ (20 ~ 45 ℃).