在高能量下的深虚康普顿散射中探测质子的价夸克宽度

Wenchang Xiang, Dewen Cao, Dai-Cui 周代翠 Zhou
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引用次数: 0

摘要

我们利用改进的热点模型,在彩色玻璃冷凝物的框架内,研究质子在高能量下深度虚拟康普顿散射的价夸克形状。为了研究单个价夸克的形状,我们采用了一种新颖的价夸克宽度处理方法。我们首次使用不同的宽度($\mathrm{B_u}$ 和 $\mathrm{B_d}$)来计算上下夸克的轮廓密度分布,而不是使用文献中的相同宽度来计算相干和非相干深虚康普顿散射的截面。我们发现,在每种碰撞能量下,用$\mathrm{B_u \geq B_d}$计算的截面都是一致的,这与理论预期是一致的。而用$\mathrm{B_u < B_d}$计算的结果则有一些出入。这一结果意味着上夸克可能比下夸克发射出更多的胶子,导致高能量下的$\mathrm{B_u \geq B_d}$。我们估算了这一结果的能量影响。我们的结果表明,随着对撞能量的增加,上述差异不仅会显著扩大,而且会在未来的电子-离子对撞机(EIC)和大型强子电子对撞机(LHeC)能量下转移到相对较小的动量转移范围,这表明EIC和LHeC可以为获取质子价夸克的形状提供前所未有的机会。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probing valence quark width of the proton in deeply virtual Compton scattering at high energies
We use the refined hot spot model to study the valence quark shape of the proton with the deeply virtual Compton scattering at high energies in the framework of Color Glass Condensate. To investigate the individual valence quark shape, a novel treatment of the valence quark width is employed. We calculate the cross-sections for the coherent and incoherent deeply virtual Compton scattering, for the first time, by using different widths ($\mathrm{B_u}$ and $\mathrm{B_d}$) for the profile density distributions of the up and down quarks instead of using the same width as in the literature. We find that the cross-sections calculated with $\mathrm{B_u \geq B_d}$ at each collision energy are consistent with each other themselves, which is in agreement with the theoretical expectations. While the ones computed with $\mathrm{B_u < B_d}$ show some discrepancies. This outcome implies that the up quark might emit more gluons than the down quark leading to $\mathrm{B_u \geq B_d}$ at high energy. The energy impact of the outcome is estimated. Our results show that as the collision energy increases, the aforementioned discrepancies are not only significantly broadened, but also shift to relatively smaller momentum transfer range in the future Electron-Ion Collider (EIC) and Large Hadron Electron Collider (LHeC) energies, which indicates that the EIC and LHeC can provide unprecedented chance to access the shape of the valence quark of the proton.
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