The odderon: myths and reality

L. Jenkovszky, I. Szanyi, J. Turóci
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引用次数: 0

Abstract

In the framework of a Regge-pole model, we discussthe forward phase of the proton-proton elastic scattering amplitude (ρ(13 TeV) = 0.1 ± 0.01), recently measured at the LHC. Our model includesa dipole pomeron, odderon and secondary reggeon exchanges. It accommodetes forthe low- |t| «break» (departure from the exponential behavior of the diffraction cone), the accelerating rise with energy of the forward slope B(s, t = 0) and absence of secondary dips and bumps. Contrary to the majority of Regge-pole models, our approach is based on he use of a dipole (double pole) pomeron (DP). It has a number of advantages over the conventional simple pole pomeron: DP generates rising cross sections even at unit pomeron intercept and, what is even more important, it produces a single diffraction minimum and maximum in the differential cross section, in accord with the experimental data. Relative contributions from different components to the scattering amplitude are evaluated from the fitted model.
奇怪的是:神话和现实
在Regge-pole模型的框架下,我们讨论了最近在LHC上测量到的质子-质子弹性散射振幅(ρ(13 TeV) = 0.1±0.01)的前相。我们的模型包括偶极子、奇偶子和次级区域交换。它可以适应低- t -“断裂”(偏离衍射锥的指数行为),随着能量的加速上升,向前斜率B(s, t = 0),并且没有二次倾斜和颠簸。与大多数Regge-pole模型相反,我们的方法是基于偶极子(双极)pomeron (DP)的使用。与传统的简单极波美伦相比,它有许多优点:即使在单位波美伦截距处,DP也产生上升截面,更重要的是,它在微分截面上产生单个衍射最小值和最大值,与实验数据一致。根据拟合模型计算了不同分量对散射振幅的相对贡献。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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