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Quasi-elastic and elastic charge-exchange differential cross sections (critical review)

机译:准弹性和弹性电荷交换差分横截面(批评点评)

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More than 50 years ago the charge-exchange of one nucleon in the quasi-elastic nucleon deuteron scattering was proposed to determine the spin independent, or the spin dependent parts of the elastic backward neutron proton differential cross section. For this purpose two measurements are to be performed using unpolarized particles only. Such a suggestion was very attractive for experimentalists, since at that time polarized beams were rare and polarized targets were nonexistent. One experiment consists in the inclusive measurement of the charge-exchange quasi-elastic nucleon deuteron differential cross section. The energy of the fast outgoing nucleon is to be approximately the same as that of the incident nucleon. The intrinsic momenta of the remaining two identical nucleons should be small. The impulse approximation has been assumed, i.e. in the final state of the two nucleons their interaction can be neglected. The quasi-elastic result is to be compared with the elastic np differential cross section in the backward direction at the same energy. The theory related the ratio R (QE) (pi) of the quasi-elastic to the elastic np charge-exchange differential cross sections to the spin dependent part of the np backward elastic scattering amplitude. Several experiments in the nucleon kinetic energy interval below 1 GeV were carried out, where the R (QE) (pi) values were determined. Recently the energy interval was extended up to 2 GeV by successful experiments at the JINR VBLHE Nuclotron. The quasi-elastic results can be compared with the values of the analogous quantity R (np) (pi) for the np elastic scattering, calculated from the phase shift analyses below 1.3 GeV. The present paper is a critical review checking expressions for R (np) (pi) in different amplitude representations, listing numerical values of elastic np quantities and results of existing quasi-elastic experiments. Conclusions and statements of some authors and the validity of the relevant theory is discussed.
机译:超过50年前,提出了一种核仁在准弹性核心氘散射中的电荷交换,以确定旋转独立,或弹性向下中子质子差分横截面的自旋依赖性部分。为此目的,仅使用未偏振的颗粒进行两次测量。这种建议对于实验主义者来说非常有吸引力,因为当时偏振梁是罕见的并且极化的靶不存在。一个实验包括在电荷交换准弹性核子氘差横截面的包容性测量中。快速传出核的能量与入射核素的能量大致相同。剩下的两个相同核子的内在动量应该很小。已经假设了脉冲近似,即它们在其相互作用的两个核中的最终状态下可以忽略。在相同能量的向后方向上与弹性NP差剖视角沿着相同能量的弹性NP差分横截面进行比较。该理论相关的拟弹性与弹性NP电荷交换差分截面的比率R(QE)(Pi)(Qe)(Pi)与NP后向弹性散射幅度的自旋依赖性部分。进行了核心动能间隔的几个实验,进行了低于1 GEV,确定R(QE)(PI)值。最近,通过成功的实验,在Jinr vblhhe核心核查团的成功实验中,能量间隔延长至2个GEV。可以将准弹性结果与NP弹性散射的类似量R(PI)的值进行比较,从1.3 GEV的相移分析计算。本文是在不同幅度表示中的R(NP)(PI)的关键综述检查表达式,列出了弹性NP数量的数值和现有的准弹性实验结果。讨论了一些作者的结论和陈述和相关理论的有效性。

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