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Systematic study of diphoton resonance at 750 GeV from sgoldstino

Center for High-Energy Physics, Peking University, Beijing, 100871, P. R. China

State Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

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Li Huang

State Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

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Chuang Li

State Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

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Tianjun Li

State Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054, P. R. China

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Shabbar Raza

State Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

E-mail Address: shabbar@itp.ac.cn

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, and

Bin Zhu

Institute of Physics, Chinese Academy of Sciences, Beijing 100190, P. R. China

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https://doi.org/10.1142/S0217751X16501517Cited by:3 (Source: Crossref)

Abstract

The ATLAS and CMS Collaborations of the Large Hadron Collider (LHC) have reported an excess of events in diphoton channel with invariant mass of about 750 GeV. With low energy supersymmetry breaking, we systematically consider the sgoldstino scalar S as the new resonance, which is a linear combination of the CP-even scalar $s$ $s$ and CP-odd pseudoscalar $a$ $a$ . Because we show that $s$ $s$ and $a$ $a$ can be degenerated or have large mass splitting, we consider two cases for all the following three scenarios: (1) Single resonance, $s$ $s$ is the 750 GeV resonance decays to a pair of 1 GeV pseudoscalar $a$ $a$ with suitable decay length, these two $a$ $a$ decay into collimated pair of photons which cannot be distinguished at the LHC and may appear as diphotons instead of four photons. (2) Twin resonances, $m_{s} ≃ m_{a}$ $m_{s} ≃ m_{a}$ with a mass difference of about 40 GeV and both $s$ $s$ and $a$ $a$ decay into diphoton pairs. For productions, we consider three scenarios: (I) vector-boson fusion; (II) gluon–gluon fusion; (III) $q ˉ q$ $q \bar{q}$ pair production. In all these scenarios with two kinds of resonances, we find the parameter space that satisfies the diphoton production cross-section from 3 to 13 fb and all the other experimental constraints. And we address the decay width as well. In particular, in the third scenario, we observe that the production cross-section is small but the decay width of $s$ $s$ or $a$ $a$ can be from 40 to 60 GeV. Even if the 750 GeV diphoton excesses were not confirmed by the ATLAS and CMS experiments, we point out that our proposal can be used to explain the current and future diphoton excesses.

Keywords:

PACS: 12.60.Jv

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