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Probing the gamma-ray emission from HESS J1834-087 using H.E.S.S. and Fermi LAT observations

  • A. Abramowski
  • , F. Aharonian
  • , F. Ait Benkhali
  • , A. G. Akhperjanian
  • , E. Angüner
  • , G. Anton
  • , M. Backes
  • , S. Balenderan
  • , A. Balzer
  • , A. Barnacka
  • , Y. Becherini
  • , J. Becker Tjus
  • , K. Bernlöhr
  • , E. Birsin
  • , E. Bissaldi
  • , J. Biteau
  • , M. Böttcher
  • , C. Boisson
  • , J. Bolmont
  • , P. Bordas
  • J. Brucker, F. Brun, P. Brun, T. Bulik, S. Carrigan, S. Casanova, P. M. Chadwick, R. Chalme-Calvet, R. C.G. Chaves, A. Cheesebrough, M. Chrétien, S. Colafrancesco, G. Cologna, J. Conrad, C. Couturier, Y. Cui, M. Dalton, M. K. Daniel, I. D. Davids, B. Degrange, C. Deil, P. DeWilt, H. J. Dickinson, A. Djannati-Ataï, W. Domainko, L. O.C. Drury, G. Dubus, K. Dutson, J. Dyks, M. Dyrda, T. Edwards, K. Egberts, P. Eger, P. Espigat, C. Farnier, S. Fegan, F. Feinstein, M. V. Fernandes, D. Fernandez, A. Fiasson, G. Fontaine, A. Förster, M. Füßling, M. Gajdus, Y. A. Gallant, T. Garrigoux, G. Giavitto, B. Giebels, J. F. Glicenstein, M. H. Grondin, M. Grudzińska, S. Häffner, J. Hahn, J. Harris, G. Heinzelmann, G. Henri, G. Hermann, O. Hervet, A. Hillert, J. A. Hinton, W. Hofmann, P. Hofverberg, M. Holler, D. Horns, A. Jacholkowska, C. Jahn, M. Jamrozy, M. Janiak, F. Jankowsky, I. Jung, M. A. Kastendieck, K. Katarzyński, U. Katz, S. Kaufmann, B. Khélifi, M. Kieffer, S. Klepser, D. Klochkov, W. Kluźniak, T. Kneiske, D. Kolitzus, Nu Komin, K. Kosack, S. Krakau, F. Krayzel, P. P. Krüger, H. Laffon, G. Lamanna, J. Lefaucheur, A. Lemière, M. Lemoine-Goumard, J. P. Lenain, T. Lohse, A. Lopatin, C. C. Lu, V. Marandon, A. Marcowith, R. Marx, G. Maurin, N. Maxted, M. Mayer, T. J.L. McComb, J. Méhault, P. J. Meintjes, U. Menzler, M. Meyer, R. Moderski, M. Mohamed, E. Moulin, T. Murach, C. L. Naumann, M. De Naurois, J. Niemiec, S. J. Nolan, L. Oakes, H. Odaka, S. Ohm, E. De Oña Wilhelmi, B. Opitz, M. Ostrowski, I. Oya, M. Panter, R. D. Parsons, M. Paz Arribas, N. W. Pekeur, G. Pelletier, J. Perez, P. O. Petrucci, B. Peyaud, S. Pita, H. Poon, G. Pühlhofer, M. Punch, A. Quirrenbach, S. Raab, M. Raue, I. Reichardt, A. Reimer, O. Reimer, M. Renaud, R. De Los Reyes, F. Rieger, L. Rob, C. Romoli, S. Rosier-Lees, G. Rowell, B. Rudak, C. B. Rulten, V. Sahakian, D. A. Sanchez, A. Santangelo, R. Schlickeiser, F. Schüssler, A. Schulz, U. Schwanke, S. Schwarzburg, S. Schwemmer, H. Sol, G. Spengler, F. Spies, Stawarz, R. Steenkamp, C. Stegmann, F. Stinzing, K. Stycz, I. Sushch, J. P. Tavernet, T. Tavernier, A. M. Taylor, R. Terrier, M. Tluczykont, C. Trichard, K. Valerius, C. Van Eldik, B. Van Soelen, G. Vasileiadis, C. Venter, A. Viana, P. Vincent, H. J Völk, F. Volpe, M. Vorster, T. Vuillaume, S. J. Wagner, P. Wagner, R. M Wagner, M. Ward, M. Weidinger, Q. Weitzel, R. White, A. Wierzcholska, P. Willmann, A. Wörnlein, D. Wouters, R. Yang, V. Zabalza, M. Zacharias, A. A Zdziarski, A. Zech, H. S. Zechlin, F. Acero, J. M. Casandjian, J. Cohen-Tanugi, F. Giordano, L. Guillemot, J. Lande, H. Pletsch, Y. Uchiyama
  • Universität Hamburg
  • Max-Planck-Institut für Kernphysik
  • Dublin Institute for Advanced Studies
  • National Academy of Sciences of Armenia
  • Yerevan Physics Institute
  • Humboldt-Universität zu Berlin
  • Friedrich-Alexander University (FAU) Erlangen-Nürnberg and Universitätsklinikum Erlangen
  • University of Namibia
  • Durham University
  • c/o DESY
  • University of Potsdam
  • Nicolaus Copernicus Astronomical Center of the Polish Academy of Sciences
  • Linnaeus University, Växjö
  • Ruhr-University Bochum
  • University of Innsbruck
  • Ip Paris
  • University of California at Santa Cruz
  • North-West University
  • LUTH - Laboratoire de l'Univers et de ses Theories
  • Sorbonne Université
  • University of Tübingen
  • Universite Paris-Saclay
  • University of Warsaw
  • University of the Witwatersrand, Johannesburg
  • Landessternwarte Heidelberg
  • Stockholm University
  • Wallenberg Academy Fellow
  • Univ. Bordeaux
  • European Community
  • University of Adelaide
  • Astroparticule and Cosmol APC
  • Université Grenoble Alpes
  • University of Leicester
  • Institute for Nuclear Physics
  • Laboratoire Univers et Particules de Montpellier
  • Université Savoie Mont Blanc
  • Jagiellonian University
  • Nicolaus Copernicus University
  • University of the Free State
  • Charles University
  • Politecnico di Bari
  • INFN Sezione di Bari
  • CNRS
  • CNRS
  • Stanford University
  • Max-Planck-Institut fuer Gravitationsphysik
  • Leibniz Universität Hannover
  • Rikkyo University

Résultats de recherche: Contribution à un journalArticleRevue par des pairs

Résumé

Aims. Previous observations with the High Energy Stereoscopic System (H.E.S.S.) have revealed an extended very-high-energy (VHE; E > 100 GeV) γ-ray source, HESS J1834-087, coincident with the supernova remnant (SNR)W41. The origin of the γ-ray emission was investigated in more detail with the H.E.S.S. array and the Large Area Telescope (LAT) onboard the Fermi Gamma-ray Space Telescope. Methods. The γ-ray data provided by 61 h of observations with H.E.S.S., and four years with the Fermi LAT were analyzed, covering over five decades in energy from 1.8 GeV up to 30 TeV. The morphology and spectrum of the TeV and GeV sources were studied and multiwavelength data were used to investigate the origin of the γ-ray emission toward W41. Results. The TeV source can be modeled with a sum of two components: one point-like and one significantly extended (σTeV = 0.17° ± 0. 01°), both centered on SNR W41 and exhibiting spectra described by a power law with index ΓTeV ≃ 2.6. The GeV source detected with Fermi LAT is extended (σGeV = 0.15° ± 0.03°) and morphologically matches the VHE emission. Its spectrum can be described by a power-law model with an index ΓGeV = 2.15 ± 0.12 and smoothly joins the spectrum of the whole TeV source. A break appears in the γ-ray spectra around 100 GeV. No pulsations were found in the GeV range. Conclusions. Two main scenarios are proposed to explain the observed emission: a pulsar wind nebula (PWN) or the interaction of SNRW41 with an associated molecular cloud. X-ray observations suggest the presence of a point-like source (a pulsar candidate) near the center of the remnant and nonthermal X-ray di ffuse emission that could arise from the possibly associated PWN. The PWN scenario is supported by the compatible positions of the TeV and GeV sources with the putative pulsar. However, the spectral energy distribution from radio to γ-rays is reproduced by a one-zone leptonic model only if an excess of low-energy electrons is injected following a Maxwellian distribution by a pulsar with a high spin-down power (>1037 ergs-1). This additional low-energy component is not needed if we consider that the point-like TeV source is unrelated to the extended GeV and TeV sources. The interacting SNR scenario is supported by the spatial coincidence between the γ-ray sources, the detection of OH (1720 MHz) maser lines, and the hadronic modeling.

langue originaleAnglais
Numéro d'articleA27
journalAstronomy and Astrophysics
Volume574
Les DOIs
étatPublié - 1 févr. 2015

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