GALACTIC CENTER GEV GAMMA- RAY EXCESS FROM DARK MATTER WITH GAUGED LEPTON NUMBERS. Jongkuk Kim (SKKU) Based on Physics Letters B.

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GALACTIC CENTER GEV GAMMA- RAY EXCESS FROM DARK MATTER WITH GAUGED LEPTON NUMBERS Jongkuk Kim (SKKU) Based on Physics Letters B. 752 (2016) 59-65 In collaboration with Jong Chul Park, Seong Chan Park The 52nd workshop on Gravity & cosmology for APCTP FRP November 19, 2016 @ SKKU

OUTLINE Introduction Fermi-LAT: GeV gamma-rays from the Galactic center Leptophilic Dark Matter model Constraints Muon g-2, tau decay, neutrino trident production Direct detection Z search @ LHC Conclusion

INTRODUCTION FERMI-LAT GEV EXCESS GeV gamma ray excess is very well fit by 30~40GeV DM particles annihilating to b quark final states Required cross section is σv ~ 2*10-26 cm 3 /s Leptonic final state analysis Focus on prompt gamma ray emission Dan Hooper et al.(arxiv: 1402.6703) Annihilation of DM into pure lepton final states does not provide a good fit

INTRODUCTION FERMI-LAT GEV EXCESS Joseph Silk et al.(arxiv: 1403.1987) Omitting the photon emission originating from primary and secondary electrons Wrong conclusion : lepton final state! bad fit Including Inverse Compton Scattering and Bremsstrahlung contributions from electrons Annihilation of DM into pure leptons provide a good fit

INTRODUCTION FERMI-LAT GEV EXCESS Conduct the fit of the case of Best fit:

LEPTOPHILIC DM MODEL Cosmic ray detection experiments excess in positron fraction, but not in anti-proton AMS-02 Collaboration (PRL 113(2014) 221102) Possible to gauge one of the differences of two leptonflavor numbers L e -L μ, L μ -L τ, L τ L e : anomaly free Symmetries including L e are strongly constrained X. G. He, R. Volkas et al., PRD(1991) R. Foot, Mod. Phys. Lett. A(1991)

LEPTOPHILIC DM MODEL New gauge symmetry has influence on the 2 nd and 3 rd generations of leptons Dirac fermion plays a role of dark matter Charges under the gauged L μ -L τ symmetry Model set-up

RELIC ABUNDANCE Dominant annihilation channels of DM: DM annihilates into leptons through s-channel contribution DM annihilates into a Z pair through t-channel contribution kinematically allowed only when Relic density : Planck Collaboration (arxiv: 1502.01589)

FERMI-LAT GEV EXCESS DM annihilation into charged lepton final states The required dark matter mass : The preferred cross section : parameter plane (m Z,, g, ) Same range with thermal relic density The s-channel resonance effect around

Constraints

CONSTRAINTS MUON ANOMALOUS MAGNETIC MOMENT Experimental value: SM prediction : Particle Data Group 2014 Difference between them : A positive contribution to muon (g-2): E. Ma et al.(arxiv: 0110146)

CONSTRAINTS TAU DECAY Z boson makes new contributions to tau decay processes one-loop box diagram: M. Pospelov et al.(arxiv: 1403.1269) Experimental value is more than 2σ level above the SM prediction : with correction due to symmetry:

CONSTRAINTS NEUTRINO TRIDENT PRODUCTION Production of a muon pair from the scattering of a muon neutrino with heavy nuclei The leading order Z contribution: M.Pospelov et al.(arxiv: 1406.2332) Measurements stringently constrain a model with a new gauge boson that couples to both a muon and muon-neutrino

CONSTRAINTS DIRECT DETECTION FROM LUX Dominant direct detection process Cross section between DM and nucleon A : the mass number of the target Z : the charge number of the target reduced mass: LUX Collaboration (arxiv: 1310.8214) The most stringent result LUX experiment

CONSTRAINTS LHC PHENOMENOLOGY The lowest order Z production process at collider Produce a charged lepton pair through Drell-Yan process Z is radiated from one of leptons LHC Measures 4 leptons process at the Z boson resonance Interesting final state : 4 muons Dominant SM background :

CONSTRAINTS LHC PHENOMENOLOGY Perform Z production at LHC 8TeV & 14TeV using MadGraph Set g =0.1, ATLAS selection cut ATLAS selection cuts Candidate separation of Invariant mass of four leptons:

CONSTRAINTS parameter space (m Z,, g, ) Exclusion region from muon (g-2) & tau decay @ 2σ level from 4muon search at LHC @ 3 σ level from dark matter direct detection: LUX 90% confidence limit + 1 σ from neutrino trident production @ CCFR: 2 σ level

CONCLUSION DM with gauged L μ -L τ symmetry can explain Fermi-LAT GeV gamma ray excess near galactic center DM does not interact with SM quarks at tree level. However, DM couples to SM quarks in nucleus through the loop-suppressed interaction Leptophilic DM additionally contributes to muon (g-2), tau decay, neutrino trident production Parameter space is already partially constrained by 8TeV LHC for light Z and will be tested by 14TeV LHC Thank