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      Astrophysical Constraints on Singlet Scalars at LHC

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          Abstract

          We consider the viability of new heavy gauge singlet scalar particles at the LHC. Our motivation for this study comes from the possibility of a new particle with mass ~ 750 GeV decaying significantly into two photons at LHC, but our analysis applies more broadly. We show that there are significant constraints from astrophysics and cosmology on the simplest UV complete models that incorporate such a particle and its associated collider signal. The simplest and most obvious UV complete model that incorporates the signal is that it arises from a new singlet scalar (or pseudo-scalar) coupled to a new electrically charged and colored heavy fermion. Here we show that these new fermions (and anti-fermions) would be produced in the early universe, then form new color singlet heavy mesons with light quarks, obtain a non-negligible freeze-out abundance, and remain in kinetic equilibrium until decoupling. These heavy mesons possess interesting phenomenology, dependent on their charge, including forming new bound states with electrons and protons. We show that a significant number of these heavy states would survive for the age of the universe and an appreciable number would eventually be contained within the earth and solar system. We show that this leads to detectable consequences, including the production of highly energetic events from annihilations on earth, new spectral lines, and, spectacularly, the destabilization of stars. The lack of detection of these consequences rules out such simple UV completions, putting pressure on the viability of such new particles at LHC. To incorporate such a scalar would require either much more complicated UV completions or even further new physics that provides a decay channel for the associated fermion.

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          The Minimal Model of a Diphoton Resonance: Production without Gluon Couplings

          , , (2015)
          We consider the phenomenology of a resonance that couples to photons but not gluons, and estimate its production rate at the LHC from photon-photon fusion in elastic pp scattering using the effective photon and narrow width approximations. The rate is sensitive only to the mass, the spin, the total width of the resonance, and its branching fraction to photons. Production cross sections of 5-10 fb at 13 TeV can be easily accommodated for a 750 GeV resonance with partial photon width of 15 GeV. This provides the minimal explanation of the reported diphoton anomaly in the early LHC Run II data.
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            Diphoton Signatures from Heavy Axion Decays at the CERN Large Hadron Collider

            (2016)
            Recently, the LHC collaborations, ATLAS and CMS, have announced an excess in the diphoton channel with local significance of about \(3\,\sigma\) around an invariant mass distribution of \(\sim 750\) GeV, after analyzing new data collected at centre-of-mass energies of \(\sqrt{s} = 13~{\rm TeV}\). We present a possible physical interpretation of such a signature, within the framework of a minimal UV-complete model with a massive singlet pseudo-scalar state \(a\) that couples to a new TeV-scale coloured vector-like fermion \(F\), whose hypercharge quantum number is a non-zero integer. The pseudo-scalar state \(a\) might be a heavy pseudo-Goldstone boson, such as a heavy axion, which decays into two photons and whose mass lies around the excess region. The mass of the CP-odd state \(a\) and its coupling to \(F\) may be due to non-perturbative effects, which can break the original Goldstone shift symmetry dynamically. The possible role that the heavy axion \(a\) can play in the radiative generation of a seesaw Majorana scale and in the solution to the so-called strong CP problem is briefly discussed.
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              Scattering Light by Light at 750 GeV at the LHC

              , , (2016)
              We consider the possibility that the diphoton excess at 750 GeV is caused by a new scalar resonance produced in photon fusion. This scenario is parametrised by only one relevant effective couplings and is thus minimal. We show that this setup can reproduce both the production rate and width of the resonance, and is not in conflict with the 8 TeV limits on the diphoton cross section. The scenario also predicts event rates for \(WW\), \(ZZ\), \(Z\gamma\) final states. We suggest to perform precision measurements by studying light-by-light scattering with intact protons detected in forward detectors. We construct a simple model that shows that the required couplings can be achieved with new vectorlike, uncolored fermions (with a strong Yukawa coupling to the resonance) which may also account for the required width.
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                Author and article information

                Journal
                2016-07-21
                2016-07-23
                Article
                1607.06445
                408c8814-364d-4749-9a81-0d8049b23523

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                17 pages, 3 figures. V2: small updates on charges
                hep-ph astro-ph.CO hep-th

                Cosmology & Extragalactic astrophysics,High energy & Particle physics
                Cosmology & Extragalactic astrophysics, High energy & Particle physics

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