Faking ordinary photons by displaced dark photon decays

被引:4
|
作者
Tsai, Yuhsin [1 ]
Wang, Lian-Tao [2 ,3 ,4 ]
Zhao, Yue [5 ]
机构
[1] Univ Maryland, Maryland Ctr Fundamental Phys, Dept Phys, College Pk, MD 20742 USA
[2] Univ Chicago, Dept Phys, Chicago, IL 60637 USA
[3] Univ Chicago, Enrico Fermi Inst, Chicago, IL 60637 USA
[4] Univ Chicago, Kavli Inst Cosmol Phys, Chicago, IL 60637 USA
[5] Univ Michigan, Michigan Ctr Theoret Phys, Ann Arbor, MI 48109 USA
基金
美国国家科学基金会;
关键词
D O I
10.1103/PhysRevD.95.015027
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
A light metastable dark photon decaying into a collimated electron/positron pair can fake a photon, either converted or unconverted, at the LHC. The detailed object identification relies on the specifics of the detector and strategies for the reconstruction. We study the fake rate based on the ATLAS (CMS) detector geometry and show that it can be O(1) with a generic choice of parameters. Especially, the probability of being registered as a photon is angular dependent. Such detector effects can induce bias to measurements on certain properties of new physics. In this paper, we consider the scenario where dark photons in final states are from a heavy resonance decay. Consequently, the detector effects can dramatically affect the results when determining the spin of a resonance. Further, if the decay products from the heavy resonance are one photon and one dark photon, which has a large probability to fake a diphoton event, the resonance is allowed to be a vector. Because of the difference in detectors, the cross sections measured in ATLAS and CMS do not necessarily match. Furthermore, if the diphoton signal is given by the dark photons, the standard model Z. and ZZ final states do not necessarily come with the.. channel, which is a unique signature in our scenario. The issue studied here is relevant also for any future new physics searches with photon(s) in the final state. We discuss possible ways of distinguishing dark photon decay and a real photon in the future.
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页数:12
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