Abstract
Motivated by the recent update on LHC searches for narrow and broad resonances decaying into diphotons we reconsider the possibility that the observed peak in the invariant mass spectrum at M_{\gamma \gamma} = 750 GeV originates from a closed string (possibly axionic) excitation \varphi (associated with low mass scale string theory) that has a coupling with gauge kinetic terms. We reevaluate the production of \varphi by photon fusion to accommodate recent developments on additional contributions to relativistic light-light scattering. We also study the production of \varphi via gluon fusion. We show that for both a narrow and a broad resonance these two initial topologies can accommodate the excess of events, spanning a wide range of string mass scales 7 \alt M_s/TeV \alt 30 that are consistent with the experimental lower bound: M_s > 7 TeV, at 95% CL. We demonstrate that for the two production processes the LHC13 data is compatible with the lack of a diphoton excess in LHC8 data within \sim 1\sigma. We also show that if the resonance production is dominated by gluon fusion the null results on dijet searches at LHC8 further constrain the coupling strengths of \varphi, but without altering the range of possible string mass scales.
Highlights
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Mγ γ = 750 GeV originates from a closed string excitation φ that has a coupling with gauge kinetic terms
We reevaluate the production of φ by photon fusion to accommodate recent developments on additional contributions to relativistic light
Summary
HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. Motivated by the recent update on LHC searches for narrow and broad resonances decaying into diphotons we reconsider the possibility that the observed peak in the invariant mass spectrum at The ATLAS [1] and CMS [2] Collaborations reported excesses of events over expectations from standard model (SM) processes in the diphoton mass distribution around 750 GeV, using (respectively) 3.2√fb−1 and 2.6 fb−1 of data recorded at a centerof-mass energy s = 13 TeV.
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