纯相对论系统的结构和电磁形式因素

V. Karmanov, J. Carbonell, H. Sazdjian
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引用次数: 3

摘要

通过标量无质量交换相互作用的两个大质量标量粒子的Bethe-Salpeter方程有两种类型的解,它们在非相对论极限下的行为不同:转化为库仑解的正常解和“异常”解。后者没有非相对论性的对应物,在非相对论性的极限中消失。我们研究了所有这些状态的组成。事实证明,即使在结合能很大的情况下,正常状态也是由两个大质量粒子主导的。然而,即使结合能很小,双体扇区对异常态的贡献也只有1%左右;它们被无数的无质量粒子所控制。计算了正常和异常状态下的弹性电磁形状因子,以及两者之间的过渡状态。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Structure and EM form factors of purely relativistic systems
The Bethe-Salpeter equation for two massive scalar particles interacting by scalar massless exchange has solutions of two types, which differ from each other by their behavior in the non-relativistic limit: the normal solutions which turn into the Coulomb ones and the "abnormal" solutions. The latter ones have no non-relativistic counterparts and disappear in the non-relativistic limit. We studied the composition of all these states. It turns out that the normal states, even for large binding energy, are dominated by two massive particles. Whereas, the contribution of the two-body sector into the abnormal states, even for small binding energy, is of the order of 1% only; they are dominated by an indefinite number of the massless particles. The elastic electromagnetic form factors for both normal and abnormal states, as well as the transition ones between them, are calculated.
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