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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, Appelt E, Delannoy A G, Greene S, Gurrola A, Janjam R, Johns W, Maguire C, Mao Y, Melo A, Sheldon P, Snook B, Tuo S, Velkovska J, Xu Q, Arenton M W, Boutle S, Cox B, Francis B, Goodell J, Hirosky R, Ledovskoy A, Li H, Lin C, Neu C, Wolfe E, Wood J, Xia F, Clarke C, Harr R, Karchin P E, Kottachchi Kankanamge Don C, Lamichhane P, Sturdy J, Belknap D A, Carlsmith D, Cepeda M, Christian A, Dasu S, Dodd L, Duric S, Friis E, Gomber B, Grothe M, Hall-Wilton R, Herndon M, Hervé A, Klabbers P, Lanaro A, Levine A, Long K, Loveless R, Mohapatra A, Ojalvo I, Perry T, Pierro G A, Polese G, Ross I, Ruggles T, Sarangi T, Savin A, Sharma A, Smith N, Smith W H, Taylor D, 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;76:13. doi: 10.1140/epjc/s10052-015-3853-3. Epub 2016 Jan 11.
A measurement is presented of differential cross sections for Higgs boson (H) production in pp collisions at [Formula: see text][Formula: see text]. The analysis exploits the [Formula: see text] decay in data corresponding to an integrated luminosity of 19.7[Formula: see text] collected by the CMS experiment at the LHC. The cross section is measured as a function of the kinematic properties of the diphoton system and of the associated jets. Results corrected for detector effects are compared with predictions at next-to-leading order and next-to-next-to-leading order in perturbative quantum chromodynamics, as well as with predictions beyond the standard model. For isolated photons with pseudorapidities [Formula: see text], and with the photon of largest and next-to-largest transverse momentum ([Formula: see text]) divided by the diphoton mass [Formula: see text] satisfying the respective conditions of [Formula: see text] and [Formula: see text], the total fiducial cross section is [Formula: see text][Formula: see text].
给出了在[公式：见正文][公式：见正文]的质子-质子碰撞中希格斯玻色子（H）产生的微分截面测量结果。该分析利用了在大型强子对撞机（LHC）上CMS实验收集的对应于19.7[公式：见正文]积分亮度的数据中的[公式：见正文]衰变。截面作为双光子系统和相关喷注的运动学性质的函数进行测量。针对探测器效应校正后的结果与微扰量子色动力学中次领头阶和次次领头阶的预测以及超出标准模型的预测进行了比较。对于具有赝快度[公式：见正文]的孤立光子，且具有最大和次大横向动量（[公式：见正文]）的光子除以双光子质量[公式：见正文]满足各自的[公式：见正文]和[公式：见正文]条件时，总的基准截面为[公式：见正文][公式：见正文]。
