TY - JOUR
T1 - Dark Matter interpretations of the e± excesses after FERMI
AU - Meade, Patrick
AU - Papucci, Michele
AU - Strumia, Alessandro
AU - Volansky, Tomer
N1 - Funding Information:
We thank Ronaldo Bellazzini, Marco Casolino, Marco Cirelli, Dario Grasso, David Morrissey, Igor Moskalenko, Pierre Salati, David Poland, Martti Raidal, and Neal Weiner for useful discussions. P.M. and T.V. are supported in part by DOE grant DE-FG02-90ER40542 . M.P. is supported in part by NSF grant PH0503584 . Research funds of A.S. have been in toto expropriated by his Department in financial difficulties.
PY - 2010/5/21
Y1 - 2010/5/21
N2 - The cosmic-ray excess observed by PAMELA in the positron fraction and by FERMI and HESS in e- + e+ can be interpreted in terms of DM annihilations or decays into leptonic final states. Final states into τ's or 4μ give the best-fit to the excess. However, in the annihilation scenario, they are incompatible with photon and neutrino constraints, unless DM has a quasi-constant density profile. Final states involving e's are less constrained but poorly fit the excess, unless hidden sector radiation makes their energy spectrum smoother, allowing a fit to all the data with a combination of leptonic modes. In general, DM lighter than about a TeV cannot fit the excesses, so PAMELA should find a greater positron fraction at higher energies. The DM interpretation can be tested by FERMI γ observations above 10 GeV: if the e± excess is everywhere in the DM halo, Inverse Compton scattering on ambient light produces a well-predicted γ excess that FERMI should soon detect.
AB - The cosmic-ray excess observed by PAMELA in the positron fraction and by FERMI and HESS in e- + e+ can be interpreted in terms of DM annihilations or decays into leptonic final states. Final states into τ's or 4μ give the best-fit to the excess. However, in the annihilation scenario, they are incompatible with photon and neutrino constraints, unless DM has a quasi-constant density profile. Final states involving e's are less constrained but poorly fit the excess, unless hidden sector radiation makes their energy spectrum smoother, allowing a fit to all the data with a combination of leptonic modes. In general, DM lighter than about a TeV cannot fit the excesses, so PAMELA should find a greater positron fraction at higher energies. The DM interpretation can be tested by FERMI γ observations above 10 GeV: if the e± excess is everywhere in the DM halo, Inverse Compton scattering on ambient light produces a well-predicted γ excess that FERMI should soon detect.
KW - Dark Matter
KW - FERMI
KW - PAMELA
UR - http://www.scopus.com/inward/record.url?scp=76749099675&partnerID=8YFLogxK
U2 - 10.1016/j.nuclphysb.2010.01.012
DO - 10.1016/j.nuclphysb.2010.01.012
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AN - SCOPUS:76749099675
SN - 0550-3213
VL - 831
SP - 178
EP - 203
JO - Nuclear Physics B
JF - Nuclear Physics B
IS - 1-2
ER -