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Stefanovitch R, Sziklai J, Taylor C, Tcherniaev E, Turini N, Urban O, Vacek V, Vavroch O, Welti J, Williams J, Zich J, Zielinski K
Yerevan Physics Institute, Yerevan, Armenia.
Institut für Hochenergiephysik, Vienna, Austria.
Eur Phys J C Part Fields. 2020;80(12):1164. doi: 10.1140/epjc/s10052-020-08562-y. Epub 2020 Dec 17.
Measurements are presented of the single-diffractive dijet cross section and the diffractive cross section as a function of the proton fractional momentum loss and the four-momentum transfer squared . Both processes and , i.e. with the proton scattering to either side of the interaction point, are measured, where includes at least two jets; the results of the two processes are averaged. The analyses are based on data collected simultaneously with the CMS and TOTEM detectors at the LHC in proton-proton collisions at during a dedicated run with at low instantaneous luminosity and correspond to an integrated luminosity of . The single-diffractive dijet cross section , in the kinematic region , , with at least two jets with transverse momentum , and pseudorapidity , is . The ratio of the single-diffractive to inclusive dijet yields, normalised per unit of , is presented as a function of , the longitudinal momentum fraction of the proton carried by the struck parton. The ratio in the kinematic region defined above, for values in the range , is , where and are the single-diffractive and inclusive dijet cross sections, respectively. The results are compared with predictions from models of diffractive and nondiffractive interactions. Monte Carlo predictions based on the HERA diffractive parton distribution functions agree well with the data when corrected for the effect of soft rescattering between the spectator partons.
给出了单衍射双喷注截面和衍射截面作为质子分数动量损失和四动量转移平方的函数的测量结果。测量了这两个过程，即质子散射到相互作用点两侧的过程 和 ，其中 包括至少两个喷注；对这两个过程的结果进行了平均。分析基于在大型强子对撞机（LHC）上，利用CMS和TOTEM探测器在质子 - 质子碰撞中，于低瞬时亮度下的一次专用运行期间，以 收集的数据，对应积分亮度为 。在运动学区域 、 ，至少有两个横向动量 的喷注且赝快度 的单衍射双喷注截面 为 。单衍射与包含性双喷注产额之比，按每单位 的归一化，作为被撞击部分子携带的质子纵向动量分数 的函数给出。在上述定义的运动学区域中，对于 范围内的 值，该比值为 ，其中 和 分别是单衍射和包含性双喷注截面。将结果与衍射和非衍射相互作用模型的预测进行了比较。基于HERA衍射部分子分布函数的蒙特卡罗预测，在对旁观者部分子之间的软再散射效应进行校正后，与数据吻合良好。
