Diphotons at the Z-pole in models of the 750 GeV resonance decaying to axion-like particles

被引:0
作者
Alexandre Alves
Alex G. Dias
Kuver Sinha
机构
[1] Universidade Federal de São Paulo,Departamento de Ciências Exatas e da Terra
[2] Universidade Federal do ABC,Centro de Ciências Naturais e Humanas
[3] University of Utah,Department of Physics and Astronomy
来源
Journal of High Energy Physics | / 2016卷
关键词
Beyond Standard Model; Effective field theories; Extended Supersymmetry;
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摘要
Models in which the 750 GeV resonance (S) decays to two light axion-like particles (ALPs a), which in turn decay to collimated photons mimicking the observed signal, are motivated by Hidden Valley scenarios and could also provide a mechanism by which a S → γγ signal persists while S → Zγ, ZZ and W W remain subdued in the near future. We point out that these Hidden Valley like models invoking S → aa → 4γ must also contend with Z → a(→ γγ)γ constraints coming from CDF and ATLAS. Within an effective field theory framework, we work out the constraints on the couplings of S to a and gauge bosons coming from photonic Z decays and ensuring that the ALPs decay inside the electromagnetic calorimeter, in two regimes — where a decays primarily to photons, and where a also has hadronic branchings. The analysis is done for both when S has a large as well as a narrow width, and for different relative contributions to the signal coming from S → γγ and a → γγ. Results for the particular case where S and a belong to the same complex field are also presented. A γγ resonance at the Z-pole coming from Z → aγ is expected in this class of models. Taking benchmark ALP masses below around 0.4 GeV and, assuming reasonable values for the fake jet rate and the identification efficiency of the photon-jet, we find the prospects for the discovery of diphotons at the Z-pole.
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[1]  
Falkowski A(2016) 750 JHEP 02 152-undefined
[2]  
Slone O(2016)Rays of light from the LHC Phys. Rev. D 93 075020-undefined
[3]  
Volansky T(2016)Diphotons from Diaxions JHEP 05 077-undefined
[4]  
Knapen S(2016)Tricking Landau-Yang: How to obtain the diphoton excess from a vector resonance Phys. Lett. B 755 145-undefined
[5]  
Melia T(2016) 750 Phys. Rev. D 93 075013-undefined
[6]  
Papucci M(2016)Experimental Considerations Motivated by the Diphoton Excess at the LHC JHEP 06 082-undefined
[7]  
Zurek K(2016) 750 Phys. Rev. D 94 015012-undefined
[8]  
Aparicio L(2016) 750 Phys. Lett. B 760 228-undefined
[9]  
Azatov A(2016) 750 Eur. Phys. J. C 76 249-undefined
[10]  
Hardy E(2016) 750 JHEP 05 114-undefined