2012
DOI: 10.1007/jhep10(2012)123
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Extra U(1) as natural source of a monochromatic gamma ray line

Abstract: Extensions of the Standard Model with an extra U ′ (1) abelian group generically generate terms coming from loops of heavy fermions, leading to three gauge boson couplings, in particular Z ′ Zγ. We show that WMAP data constrains the gauge coupling of the group g D to values comparable with the electro-weak ones, rather independently of the mass of Z ′ . Moreover, the model predicts a monochromatic γ-ray line which can fit a 130 GeV signal at the FERMI telescope for natural values of the Chern-Simons terms and … Show more

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Cited by 70 publications
(57 citation statements)
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“…Radio telescopes might help to confirm or rule out the dark matter interpretation of the line soon [32]. While the origin of the γ-ray line from the galactic center still has to be clarified, a noticeable amount of theoretical interest has been triggered [33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49]. If interpreted in terms of dark matter, the γ-ray line requires a rather large annihilation cross section into photons, σv γγ ∼ 10 −27 cm 3 s −1 , if one assumes an Einasto profile [22].…”
Section: Jhep01(2013)124mentioning
confidence: 99%
“…Radio telescopes might help to confirm or rule out the dark matter interpretation of the line soon [32]. While the origin of the γ-ray line from the galactic center still has to be clarified, a noticeable amount of theoretical interest has been triggered [33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49]. If interpreted in terms of dark matter, the γ-ray line requires a rather large annihilation cross section into photons, σv γγ ∼ 10 −27 cm 3 s −1 , if one assumes an Einasto profile [22].…”
Section: Jhep01(2013)124mentioning
confidence: 99%
“…Such scenarios have already been studied in the context of Dark Matter (DM) model building [11,[48][49][50]. In such framework, dimension six operators are suppressed by a factor M 2 (M being the mass of heavy fermions integrated out) and the dark matter sector, charged under U(1) X , couples with the weak or coloured sector of the Standard Model.…”
Section: Introductionmentioning
confidence: 99%
“…In such framework, dimension six operators are suppressed by a factor M 2 (M being the mass of heavy fermions integrated out) and the dark matter sector, charged under U(1) X , couples with the weak or coloured sector of the Standard Model. An interaction with the weak SM sector was shown to have possible astrophysical signatures [48,49], while a coupling to the coloured SM sector was constrained [11] using mono-jets events at the LHC [52], as well as indirect detection constraints arising from astrophysical measurements. Such couplings had been studied, together with couplings to the top quarks in [53] but only in the context JHEP03(2016)006 Figure 1.…”
Section: Introductionmentioning
confidence: 99%
“…Beside this general class of models, there exist other ways along which DM could emit monochromatic photons. One possibility consists in assuming that the γ-ray line is due to a Z − Z − γ Chern-Simons interaction [7]. Another possibility, much less studied, would be to consider a photon directly emitted by the DM particle.…”
Section: Introductionmentioning
confidence: 99%