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Theoretical aspects of energy-range relations,stopping power and energy straggling of protons

机译:能量范围关系,质子的停止功率和能量散布的理论方面

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The Bragg-Kleeman rule R_(CSDA)=AE_0~p provides a connection between the initial energy E_0 of a proton and the range R_(CSDA)in a medium,if the continuous-slowing-down approximation(CSDA)is assumed.The rule results from a generalized(nonrelativistic)Langevin equation;its integration also yields information on the residual energy E{z)or dE{z)/dz of a proton at position z.A relativistic extension of the generalized Langevin equation leads to the formula R_(CSDA)=A(E_0+E_0~2/2Mc2)~p.Since the initial energy E_0 of therapeutic protons satisfies E_02MC2,relativistic contributions can be treated as correction terms.Besides this phenomenological aspect,a complete integration of Bethe-Bloch equation(BBE)is presented,which provides the determination of R_(CSDA),E(z),dE(z)/dz and works without any empirical parameters.The results of these different methods are compared with Monte Carlo calculations(GEANT4).Since the energy transfer from proton to the environmental atomic electrons regarded in the CSDA-framework has to account for local fluctuations,an analysis of the Gaussian convolution and the Landau-Vavilov distribution function is performed on the basis of quantum-statistical mechanics.The Landau tail can be described as a Hermite polynomial correction of a Gaussian convolution.
机译:如果假设连续减速近似(CSDA),则布拉格-克莱曼法则R_(CSDA)= AE_0〜p提供质子的初始能量E_0与介质中范围R_(CSDA)之间的联系。规则是由广义(非相对论)Langevin方程得出的;它的积分还可以得出位置z上质子的剩余能量E(z)或dE {z)/ dz的信息广义Langevin方程的相对论扩展导致公式R_( CSDA)= A(E_0 + E_0〜2 / 2Mc2)〜p。由于治疗性质子的初始能量E_0满足E_0 2MC2,因此相对论贡献可被视为校正项。提出了Bloch方程(BBE),该方程可确定R_(CSDA),E(z),dE(z)/ dz,并且无需任何经验参数即可工作。将这些不同方法的结果与Monte Carlo计算(GEANT4)进行了比较由于能量从质子转移到环境原子电子中CSDA框架必须考虑局部涨落,基于量子统计力学对高斯卷积和Landau-Vavilov分布函数进行了分析.Landau尾巴可以描述为高斯卷积的Hermite多项式校正。

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