arXiv:1404.3676v1 [hep-ph] 14 Apr 2014 3.5 keV X-ray Line Signal from Decay of Right-Handed Neutrino due to Transition Magnetic Moment Kamakshya Prasad Modak1,∗ 1Astroparticle Physics and Cosmology Division, Saha Institute of Nuclear Physics, Kolkata 700064, India We consider the dark matter model with radiative neutrino mass generation where the Standard Model is extended with three right-handed singlet neutrinos (N1,N2 andN3) and one additional SU(2)Ldoublet scalarη. One of the right-handed neutri- nos (N1), being lightest among them, is a leptophilic fermionic dark matter candidate whose stability is ensured by the imposedZ2symmetry on this model. The second lightest right-handed neutrino (N2) is assumed to be nearly degenerated with the lightest one enhancing the co-annihilation between them. The effective interaction term among the lightest, second lightest right-handed neutrinos and photon contain- ing transition magnetic moment is responsible for the decay of heavier right-handed neutrino to the lightest one and a photon (N2→N1+γ).This radiative decay of heavier right-handed neutrino with charged scalar and leptons in internal lines could explain the X-ray line signal∼3.5 keV recently claimed by XMM-Newton X-ray observatory from different galaxy clusters and Andromeda galaxy (M31). The value of the transition magnetic moment is computed and found to be several orders of magnitude below the current reach of various direct dark matter searches.The other parameter space in this framework in the light of the observed signal is further investigated. ∗kamakshya.modak@saha.ac.in
2 I.INTRODUCTION One of the enigmas of modern particle physics is dark matter (DM) which, according to the recent survey of PLANCK [1], consists of∼26.8% of the total energy content of the universe.Various astrophysical and cosmological observations [2–4] strongly suggest convincing hints of the existence of dark matter which is non-relativistic or cold in nature. The particle nature of dark matter is still unknown. The weakly interacting massive particles (WIMPs) are the most promising candidates for cold dark matter. The experimental techniques for the detection of dark matter for both direct and indirect cases are very challenging. In direct detection experiments, the recoil energy of the target nucleus scattered off by DM particle is measured whereas the signatures of the annihilations of decays of DM particles such as charged particles, photons and neutrinos etc. are aimed to detect in indirect searches. The monochromatic line feature of such decay or annihilation products of DM are particularly significant in predicting the nature of DM particles. A huge variety of DM models in the framework of WIMP scenario with masses of DM spanning from keV to TeVs has been addressed in several literatures and their direct and indirect detection prospects have been widely studied [5–17]. Recently an evidence of X-ray line of energy 3.55 keV with more than 3σCL has been reported from the analysis of X-ray data of 73 galaxy clusters from XMM-Newton obser- vatory [18].Another group has also claimed a similar line (3.52 keV X-ray line at 4.4σ CL) from the data of X-ray spectra of Andromeda galaxy (M31) and Perseus cluster [19]. The galaxy clusters are assumed to contain huge amount of DM. Thus the signal may have a possible origin related to DM. The observed line has been explained as decay of sterile neutrino dark matter (νs→ν+γ) with mass of the sterile neutrino 7.06±0.05 keV and mixing angle sin2(2θ) = (2.2−20)×10−11[19]. Recently many other interesting ideas have been proposed to explain this line signal to come from DM [20–41]. The neutrino oscillation data [42–45] provide strong evidences for neutrino mass.The non-zero neutrino masses and evidences of DM give hints to the physics beyond the Standard Model (SM). The two beyond SM phenomenon, namely the origin of neutrino masses and the existence of cold dark matter may have a connection. In this work we focus on the simplest framework which invokes this idea of connecting both sectors has been proposed by Ma [46]. In this model the neutrino masses are generated via radiative processes with only the DM
3 particles in the loop.The right-handed neutrino which can be a possible DM candidate interacts with lepton doublets and hence DM in this scenario is leptophilic in nature. The imposed discreetZ2symmetry on this model not only forbids the tree-level Dirac mass terms but also assure a stable cold DM candidate. Phenomenological prospects for DM in this model have been done in Refs. [47–53]. In this paper we consider the case where the lightest right-handed neutrino (N1) is the cold DM candidate and the second lightest right- handed neutrino (N2) is nearly degenerated with the cold DM candidate.This situation provides rich phenomenology in direct detection of such dark matter candidate [54]. Elastic scattering cross section for DM-nucleon interaction is suppressed in this case and inelastic scattering that occurs radiatively dominates.The transition fromN2toN1gives rise to monochromatic photon with energy equal to the mass difference between the lightest and second lightest right-handed neutrinos. If the mass difference betweenN2andN1 is of∼ keV, then the recent observation of X-ray line can be accommodated in this beyond SM scenario. The paper is organised as follows.In Sec.I the theoretical framework of the model is briefly discussed.Explanation of the observed X-ray line in this model framework and a study of the constrained parameter space are done in the next section. In Sec. IV a brief summery of this work and some conclusions are drawn. II.THE MODEL We consider the model proposed by Ma [46] which is the extension of Standard Model with three gauge singlet right-handed neutrinosN1,N2,N3and and extra SU(2)Ldoublet scalarη. The fields can be written as, N1,N2,N3,η= η+ η0 .(II.1) The doublet scalarηis assumed to obtain no vacuum expectation value and hence inert. An additional discreetZ2symmetry is imposed on the model. The stability of the cold dark matter candidate in this model is guaranteed by this symmetry. Not only that the tree-level Dirac masses of neutrinos are forbidden for this additionalZ2symmetry. SM gauge group andZ2charges of the particles are shown in Tab. I.
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