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Constraints on the galactic halo dark matter from fermi-lat diffuse measurements

  • M. Ackermann
  • , M. Ajello
  • , W. B. Atwood
  • , L. Baldini
  • , G. Barbiellini
  • , D. Bastieri
  • , K. Bechtol
  • , R. Bellazzini
  • , R. D. Blandford
  • , E. D. Bloom
  • , E. Bonamente
  • , A. W. Borgland
  • , E. Bottacini
  • , T. J. Brandt
  • , J. Bregeon
  • , M. Brigida
  • , P. Bruel
  • , R. Buehler
  • , S. Buson
  • , G. A. Caliandro
  • R. A. Cameron, P. A. Caraveo, J. M. Casandjian, C. Cecchi, E. Charles, A. Chekhtman, J. Chiang, S. Ciprini, R. Claus, J. Cohen-Tanugi, J. Conrad, A. Cuoco, S. Cutini, F. D'Ammando, A. De Angelis, F. De Palma, C. D. Dermer, E. Do Couto E Silva, P. S. Drell, A. Drlica-Wagner, L. Falletti, C. Favuzzi, S. J. Fegan, W. B. Focke, Y. Fukazawa, S. Funk, P. Fusco, F. Gargano, D. Gasparrini, S. Germani, N. Giglietto, F. Giordano, M. Giroletti, T. Glanzman, G. Godfrey, I. A. Grenier, S. Guiriec, M. Gustafsson, D. Hadasch, M. Hayashida, D. Horan, R. E. Hughes, M. S. Jackson, T. Jogler, G. Jóhannesson, A. S. Johnson, T. Kamae, J. Knödlseder, M. Kuss, J. Lande, L. Latronico, A. M. Lionetto, M. Llena Garde, F. Longo, F. Loparco, B. Lott, M. N. Lovellette, P. Lubrano, M. N. Mazziotta, J. E. Mcenery, J. Mehault, P. F. Michelson, W. Mitthumsiri, T. Mizuno, A. A. Moiseev, C. Monte, M. E. Monzani, A. Morselli, I. V. Moskalenko, S. Murgia, M. Naumann-Godo, J. P. Norris, E. Nuss, T. Ohsugi, M. Orienti, E. Orlando, J. F. Ormes, D. Paneque, J. H. Panetta, M. Pesce-Rollins, M. Pierbattista, F. Piron, G. Pivato, H. Poon, S. Raino, R. Rando, M. Razzano, S. Razzaque, A. Reimer, O. Reimer, C. Romoli, C. Sbarra, J. D. Scargle, C. Sgrò, E. J. Siskind, G. Spandre, P. Spinelli, Łukasz Stawarz, A. W. Strong, D. J. Suson, H. Tajima, H. Takahashi, T. Tanaka, J. G. Thayer, J. B. Thayer, L. Tibaldo, M. Tinivella, G. Tosti, E. Troja, T. L. Usher, J. Vandenbroucke, V. Vasileiou, G. Vianello, V. Vitale, A. P. Waite, E. Wallace, K. S. Wood, M. Wood, Z. Yang, G. Zaharijas, S. Zimmer
  • German Electron Synchrotron
  • Kavli Institute for Particle Astrophysics and Cosmology
  • University of California at Berkeley
  • University of California at Santa Cruz
  • University of Pisa
  • National Institute for Nuclear Physics
  • University of Trieste
  • University of Padua
  • University of Perugia
  • NASA Goddard Space Flight Center
  • Polytechnic University of Bari
  • École polytechnique
  • CSIC
  • Istituto di Astrofisica Spaziale e Fisica Cosmica di Bologna
  • CEA-IRFU/CNRS/Université Paris Diderot
  • George Mason University
  • ASI Science Data Center
  • Université Montpellier 2
  • Stockholm University
  • Oskar Klein Centre
  • Italian Space Agency
  • National Institute for Astrophysics
  • University of Udine
  • Naval Research Laboratory
  • Hiroshima University
  • Kyoto University
  • Ohio State University
  • KTH Royal Institute of Technology
  • University of Iceland
  • IRAP
  • University of Rome Tor Vergata
  • Centre d'Etudes Nucléaires Bordeaux-Gradingnan (CENBG)
  • University of Maryland
  • Boise State University
  • University of Denver
  • Max Planck Institute for Physics (Werner Heisenberg Institute)
  • University of Innsbruck
  • NASA Ames Research Center
  • NYCB Real-Time Computing Inc.
  • JAXA Institute of Space and Astronautical Science
  • Jagiellonian University in Kraków
  • Max Planck Institute for Extraterrestrial Physics
  • Purdue University Northwest
  • Nagoya University
  • Consorzio Interuniversitario per la Fisica Spaziale (CIFS)
  • University of Washington
  • Service de Physique Théorique

Research output: Contribution to journalArticlepeer-review

224 Citations (Scopus)

Abstract

We have performed an analysis of the diffuse gamma-ray emission with the Fermi Large Area Telescope (LAT) in the Milky Way halo region, searching for a signal from dark matter annihilation or decay. In the absence of a robust dark matter signal, constraints are presented. We consider both gamma rays produced directly in the dark matter annihilation/decay and produced by inverse Compton scattering of the e+/e- produced in the annihilation/decay. Conservative limits are derived requiring that the dark matter signal does not exceed the observed diffuse gamma-ray emission. A second set of more stringent limits is derived based on modeling the foreground astrophysical diffuse emission using the GALPROP code. Uncertainties in the height of the diffusive cosmic-ray halo, the distribution of the cosmic-ray sources in the Galaxy, the index of the injection cosmic-ray electron spectrum, and the column density of the interstellar gas are taken into account using a profile likelihood formalism, while the parameters governing the cosmic-ray propagation have been derived from fits to local cosmic-ray data. The resulting limits impact the range of particle masses over which dark matter thermal production in the early universe is possible, and challenge the interpretation of the PAMELA/Fermi-LAT cosmic ray anomalies as the annihilation of dark matter.

Original languageEnglish
Article number91
JournalAstrophysical Journal
Volume761
Issue number2
DOIs
Publication statusPublished - 10 Dec 2012
Externally publishedYes

Keywords

  • Dark matter
  • Galaxy: Halo
  • Gamma rays: Diffuse background
  • Methods: Statistical

ASJC Scopus subject areas

  • Astronomy and Astrophysics
  • Space and Planetary Science

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