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Search for lepton flavour violating decays of heavy resonances and quantum black holes to an [equation] pair in proton–proton collisions at [equation]

机译:搜索在[等式]处质子-质子碰撞中违反重共振和量子黑洞衰减成[等式]对的轻子风味

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A search for narrow resonances decaying to an electron and a muon is presented. The (mathrm {e})({mu }) mass spectrum is also investigated for non-resonant contributions from the production of quantum black holes (QBHs). The analysis is performed using data corresponding to an integrated luminosity of 19.7(~ ext {fb}^ ext {-1}) collected in proton-proton collisions at a centre-of-mass energy of 8(~ ext {TeV}) with the CMS detector at the LHC. With no evidence for physics beyond the standard model in the invariant mass spectrum of selected (mathrm {e}mu ) pairs, upper limits are set at 95?(%) confidence level on the product of cross section and branching fraction for signals arising in theories with charged lepton flavour violation. In the search for narrow resonances, the resonant production of a (mathrm { au }) sneutrino in R-parity violating supersymmetry is considered. The (mathrm { au }) sneutrino is excluded for masses below 1.28(~ ext {TeV}) for couplings (lambda _{132}=lambda _{231}=lambda '_{311}=0.01), and below 2.30(~ ext {TeV}) for (lambda _{132}=lambda _{231}=0.07) and (lambda '_{311}=0.11). These are the most stringent limits to date from direct searches at high-energy colliders. In addition, the resonance searches are interpreted in terms of a model with heavy partners of the ({mathrm {Z}} ) boson and the photon. In a framework of TeV-scale quantum gravity based on a renormalization of Newton’s constant, the search for non-resonant contributions to the (mathrm {e})({mu }) mass spectrum excludes QBH production below a threshold mass (M_{mathrm {th}}) of 1.99(~ ext {TeV}). In models that invoke extra dimensions, the bounds range from 2.36(~ ext {TeV}) for one extra dimension to 3.63(~ ext {TeV}) for six extra dimensions. This is the first search for QBHs decaying into the (mathrm {e})({mu }) final state.
机译:提出了寻找衰减到电子和介子的窄共振的方法。还研究了(mathrm {e})({mu})质谱图,以了解量子黑洞(QBHs)产生的非共振贡献。使用与质子-质子碰撞中收集的积分光度19.7(〜ext {fb} ^ ext {-1})对应的数据在质心能量为8(〜ext {TeV})的情况下进行分析LHC上的CMS检测器。对于选定的(mathrm {e} mu)对的不变质谱,没有超出标准模型的物理证据,则将出现信号的横截面和分支分数乘积的上限设置为95?(%)置信度。在理论上带有违反轻子的味道。在寻找窄共振的过程中,考虑了(mathrm {au})中微子在R奇偶校验违反超对称性下的共振产生。对于小于1.28(〜ext {TeV})的质量(lambda _ {132} = lambda _ {231} = lambda'_ {311} = 0.01)和2.30(以下)的质量,排除(mathrm {au})中微子。 〜ext {TeV})表示(lambda _ {132} = lambda _ {231} = 0.07)和(lambda'_ {311} = 0.11)。这些是迄今为止在高能对撞机上进行直接搜索时最严格的限制。另外,根据具有({mathrm {Z}})玻色子和光子的重伙伴的模型来解释共振搜索。在基于牛顿常数的归一化的TeV尺度量子引力的框架中,对(mathrm {e})({mu})质谱的非共振贡献的搜索排除了阈值质量(M_ {mathrm {th}},该值是1.99(〜ext {TeV})。在调用额外维度的模型中,范围从一个额外维度的2.36(〜ext {TeV})到六个额外维度的3.63(〜ext {TeV})范围。这是对衰落到(mathrm {e})({mu})最终状态的QBH的首次搜索。

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