高子康普顿散射的极化能力

Dominik Stamen, Jan Luca Dammann, Yannis Korte, Bastian Kubis
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引用次数: 0

摘要

轻质伪高子介子的极化率可以从临界附近康普顿散射的差分截面中提取出来。虽然利用普里马科夫反应已经完成了对带电质子的测量,但对高子的相应测量会受到距离阈值不远的$K^*(892)$共振的影响。我们提出了一种方法,利用色散理论从$K\pi$中间态独立地重建$K^*(892)$贡献模型,从而扩展了可用于此目的的能量范围。我们指出,与带电离子类似物不同,电偶极子极化率与磁偶极子极化率的和与差之间很可能不存在很强的层次关系;我们讨论了通过改进实验角度覆盖范围来分解二者的敏感性。
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Polarizabilities from kaon Compton scattering
The polarizabilities of light pseudoscalar mesons can be extracted from differential cross sections for Compton scattering near threshold. While this has been accomplished for charged pions employing Primakoff reactions, a corresponding measurement for kaons will be affected by the presence of the $K^*(892)$ resonance not too far from threshold. We propose a method to extend the energy range serviceable for this purpose by reconstructing the $K^*(892)$ contribution model-independently from its $K\pi$ intermediate state, using dispersion theory. We point out that, in contrast to the charged-pion analog, there is likely no strong hierarchy between sum and difference of electric and magnetic dipole polarizabilities; we discuss the sensitivity to disentangling both by improved experimental angular coverage.
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