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M, Delgado A, Dildick S, Eusebi R, Gilmore J, Huang T, Juska E, Kamon T, Krutelyov V, Mueller R, Pakhotin Y, Patel R, Perloff A, Perniè L, Rathjens D, Rose A, Safonov A, Tatarinov A, Ulmer K A, Akchurin N, Cowden C, Damgov J, Dragoiu C, Dudero P R, Faulkner J, Kunori S, Lamichhane K, Lee S W, Libeiro T, Undleeb S, Volobouev I, Wang Z, Delannoy A G, Greene S, Gurrola A, Janjam R, Johns W, Maguire C, Melo A, Ni H, Sheldon P, Tuo S, Velkovska J, Xu Q, Arenton M W, Barria P, Cox B, Goodell J, Hirosky R, Ledovskoy A, Li H, Neu C, Sinthuprasith T, Sun X, Wang Y, Wolfe E, Xia F, Clarke C, Harr R, Karchin P E, Lamichhane P, Sturdy J, Belknap D A, Dasu S, Dodd L, Duric S, Gomber B, Grothe M, Herndon M, Hervé A, Klabbers P, Lanaro A, Levine A, Long K, Loveless R, Ojalvo I, Perry T, Pierro G A, Polese G, Ruggles T, Savin A, Sharma A, Smith N, Smith W H, Taylor D, Verwilligen P, Woods N, Collaboration Authorinst The Cms
Yerevan Physics Institute, Yerevan, Armenia.
Institut für Hochenergiephysik der OeAW, Vienna, Austria.
Eur Phys J C Part Fields. 2016;76(8):451. doi: 10.1140/epjc/s10052-016-4286-3. Epub 2016 Aug 11.
A measurement of the double-differential inclusive jet cross section as a function of jet transverse momentum [Formula: see text] and absolute jet rapidity [Formula: see text] is presented. The analysis is based on proton-proton collisions collected by the CMS experiment at the LHC at a centre-of-mass energy of 13[Formula: see text]. The data samples correspond to integrated luminosities of 71 and 44[Formula: see text] for [Formula: see text] and [Formula: see text], respectively. Jets are reconstructed with the anti-[Formula: see text] clustering algorithm for two jet sizes, , of 0.7 and 0.4, in a phase space region covering jet [Formula: see text] up to 2[Formula: see text] and jet rapidity up to [Formula: see text] = 4.7. Predictions of perturbative quantum chromodynamics at next-to-leading order precision, complemented with electroweak and nonperturbative corrections, are used to compute the absolute scale and the shape of the inclusive jet cross section. The cross section difference in , when going to a smaller jet size of 0.4, is best described by Monte Carlo event generators with next-to-leading order predictions matched to parton showering, hadronisation, and multiparton interactions. In the phase space accessible with the new data, this measurement provides a first indication that jet physics is as well understood at [Formula: see text] as at smaller centre-of-mass energies.
本文给出了作为喷注横向动量[公式：见正文]和绝对喷注快度[公式：见正文]函数的双微分包含喷注截面的测量结果。该分析基于欧洲核子研究中心（CERN）大型强子对撞机（LHC）上的紧凑缪子线圈（CMS）实验收集的质子 - 质子碰撞数据，质心能量为13[公式：见正文]。数据样本分别对应于[公式：见正文]和[公式：见正文]时的积分亮度71和44[公式：见正文]。在一个覆盖喷注[公式：见正文]高达2[公式：见正文]且喷注快度高达[公式：见正文]=4.7的相空间区域内，使用反[公式：见正文]聚类算法对两种喷注尺寸，即0.7和0.4，进行喷注重建。采用次领头阶精度的微扰量子色动力学预测，并辅以电弱和非微扰修正，来计算包含喷注截面的绝对尺度和形状。当喷注尺寸减小到0.4时，[公式：见正文]中的截面差异最好由次领头阶预测与部分子淋浴、强子化和多部分子相互作用相匹配的蒙特卡罗事件发生器来描述。在新数据可及的相空间中，该测量首次表明，在[公式：见正文]时的喷注物理与在较小质心能量时一样易于理解。
