TY - JOUR A1 - Steppa, Constantin A1 - Egberts, Kathrin T1 - Modelling the Galactic very-high-energy gamma-ray source population JF - Astronomy and astrophysics : an international weekly journal N2 - Context. The High Energy Stereoscopic System Galactic plane survey (HGPS) is to date the most comprehensive census of Galactic gamma -ray sources at very high energies (VHE; 100 GeV <= E <= 100 TeV). As a consequence of the limited sensitivity of this survey, the 78 detected gamma -ray sources comprise only a small and biased subsample of the overall population. The larger part consists of currently unresolved sources, which contribute to large-scale diffuse emission to a still uncertain amount.Aims. We study the VHE gamma -ray source population in the Milky Way. For this purpose population-synthesis models are derived based on the distributions of source positions, extents, and luminosities.Methods. Several azimuth-symmetric and spiral-arm models are compared for spatial source distribution. The luminosity and radius function of the population are derived from the source properties of the HGPS data set and are corrected for the sensitivity bias of the HGPS. Based on these models, VHE source populations are simulated and the subsets of sources detectable according to the HGPS are compared with HGPS sources.Results. The power-law indices of luminosity and radius functions are determined to range between -1.6 and -1.9 for luminosity and -1.1 and -1.6 for radius. A two-arm spiral structure with central bar is discarded as spatial distribution of VHE sources, while azimuth-symmetric distributions and a distribution following a four-arm spiral structure without bar describe the HGPS data reasonably well. The total number of Galactic VHE sources is predicted to be in the range from 800 to 7000 with a total luminosity and flux of (1.6-6.3) x 10(36) ph s(-1) and (3-15) x 10(-10) ph cm(-2) s(-1), respectively.Conclusions. Depending on the model, the HGPS sample accounts for (68-87)% of the emission of the population in the scanned region. This suggests that unresolved sources represent a critical component of the diffuse emission measurable in the HGPS. With the foreseen jump in sensitivity of the Cherenkov Telescope Array, the number of detectable sources is predicted to increase by a factor between 5 and 9. KW - astroparticle physics KW - gamma rays: general KW - gamma rays: diffuse KW - background KW - methods: observational KW - methods: numerical Y1 - 2020 U6 - https://doi.org/10.1051/0004-6361/202038172 SN - 0004-6361 SN - 1432-0746 VL - 643 PB - EDP Sciences CY - Les Ulis ER - TY - JOUR A1 - Abdalla, H. A1 - Adam, R. A1 - Aharonian, Felix A. A1 - Benkhali, F. Ait A1 - Angüner, Ekrem Oǧuzhan A1 - Arcaro, C. A1 - Armand, C. A1 - Armstrong, T. A1 - Ashkar, H. A1 - Backes, M. A1 - Baghmanyan, V. A1 - Martins, V. Barbosa A1 - Barnacka, A. A1 - Barnard, M. A1 - Becherini, Y. A1 - Berge, D. A1 - Bernlohr, K. A1 - Bi, B. A1 - Bottcher, M. A1 - Boisson, C. A1 - Bolmont, J. A1 - de Lavergne, M. de Bony A1 - Bordas, Pol A1 - Breuhaus, M. A1 - Brun, F. A1 - Brun, P. A1 - Bryan, M. A1 - Buchele, M. A1 - Bulik, T. A1 - Bylund, T. A1 - Caroff, S. A1 - Carosi, A. A1 - Casanova, Sabrina A1 - Chand, T. A1 - Chandra, S. A1 - Chen, A. A1 - Cotter, G. A1 - Curylo, M. A1 - Mbarubucyeye, J. Damascene A1 - Davids, I. D. A1 - Davies, J. A1 - Deil, C. A1 - Devin, J. A1 - deWilt, P. A1 - Dirson, L. A1 - Djannati-Atai, A. A1 - Dmytriiev, A. A1 - Donath, A. A1 - Doroshenko, V. A1 - Duffy, C. A1 - Dyks, J. A1 - Egberts, Kathrin A1 - Eichhorn, F. A1 - Einecke, S. A1 - Emery, G. A1 - Ernenwein, J. -P. A1 - Feijen, K. A1 - Fegan, S. A1 - Fiasson, A. A1 - de Clairfontaine, G. Fichet A1 - Fontaine, G. A1 - Funk, S. A1 - Fussling, Matthias A1 - Gabici, S. A1 - Gallant, Y. A. A1 - Giavitto, G. A1 - Giunti, L. A1 - Glawion, D. A1 - Glicenstein, J. F. A1 - Gottschall, D. A1 - Grondin, M. -H. A1 - Hahn, J. A1 - Haupt, M. A1 - Hermann, G. A1 - Hinton, J. A. A1 - Hofmann, W. A1 - Hoischen, Clemens A1 - Holch, T. L. A1 - Holler, M. A1 - Horbe, M. A1 - Horns, D. A1 - Huber, D. A1 - Jamrozy, M. A1 - Jankowsky, D. A1 - Jankowsky, F. A1 - Jardin-Blicq, A. A1 - Joshi, V. A1 - Jung-Richardt, I. A1 - Kasai, E. A1 - Kastendieck, M. A. A1 - Katarzynski, K. A1 - Katz, U. A1 - Khangulyan, D. A1 - Khelifi, B. A1 - Klepser, S. A1 - Kluzniak, W. A1 - Komin, Nu. A1 - Konno, R. A1 - Kosack, K. A1 - Kostunin, D. A1 - Kreter, M. A1 - Lamanna, G. A1 - Lemiere, A. A1 - Lemoine-Goumard, M. A1 - Lenain, J. -P. A1 - Levy, C. A1 - Lohse, T. A1 - Lypova, I. A1 - Mackey, J. A1 - Majumdar, J. A1 - Malyshev, D. A1 - Malyshev, D. A1 - Marandon, V. A1 - Marchegiani, P. A1 - Marcowith, Alexandre A1 - Mares, A. A1 - Marti-Devesa, G. A1 - Marx, R. A1 - Maurin, G. A1 - Meintjes, P. J. A1 - Meyer, M. A1 - Mitchell, A. A1 - Moderski, R. A1 - Mohamed, M. A1 - Mohrmann, L. A1 - Montanari, A. A1 - Moore, C. A1 - Morris, P. A1 - Moulin, Emmanuel A1 - Muller, J. A1 - Murach, T. A1 - Nakashima, K. A1 - Nayerhoda, A. A1 - de Naurois, M. A1 - Ndiyavala, H. A1 - Niederwanger, F. A1 - Niemiec, J. A1 - Oakes, L. A1 - O'Brien, Patrick A1 - Odaka, H. A1 - Ohm, S. A1 - Olivera-Nieto, L. A1 - Wilhelmi, E. de Ona A1 - Ostrowski, M. A1 - Oya, I. A1 - Panter, M. A1 - Panny, S. A1 - Parsons, R. D. A1 - Peron, G. A1 - Peyaud, B. A1 - Piel, Q. A1 - Pita, S. A1 - Poireau, V. A1 - Noel, A. Priyana A1 - Prokhorov, D. A. A1 - Prokoph, H. A1 - Puhlhofer, G. A1 - Punch, M. A1 - Quirrenbach, A. A1 - Raab, S. A1 - Rauth, R. A1 - Reichherzer, P. A1 - Reimer, A. A1 - Reimer, O. A1 - Remy, Q. A1 - Renaud, M. A1 - Rieger, F. A1 - Rinchiuso, L. A1 - Romoli, C. A1 - Rowell, G. A1 - Rudak, B. A1 - Ruiz-Velasco, E. A1 - Sahakian, V. A1 - Sailer, S. A1 - Sanchez, D. A. A1 - Santangelo, A. A1 - Sasaki, M. A1 - Scalici, M. A1 - Schussler, F. A1 - Schutte, H. M. A1 - Schwanke, U. A1 - Schwemmer, S. A1 - Seglar-Arroyo, M. A1 - Senniappan, M. A1 - Seyffert, A. S. A1 - Shafi, N. A1 - Shiningayamwe, K. A1 - Simoni, R. A1 - Sinha, A. A1 - Sol, H. A1 - Specovius, A. A1 - Spencer, S. A1 - Spir-Jacob, M. A1 - Stawarz, L. A1 - Sun, L. A1 - Steenkamp, R. A1 - Stegmann, C. A1 - Steinmassl, S. A1 - Steppa, C. A1 - Takahashi, T. A1 - Tavernier, T. A1 - Taylor, A. M. A1 - Terrier, R. A1 - Tiziani, D. A1 - Tluczykont, M. A1 - Tomankova, L. A1 - Trichard, C. A1 - Tsirou, M. A1 - Tuffs, R. A1 - Uchiyama, Y. A1 - van der Walt, D. J. A1 - van Eldik, C. A1 - van Rensburg, C. A1 - van Soelen, B. A1 - Vasileiadis, G. A1 - Veh, J. A1 - Venter, C. A1 - Vincent, P. A1 - Vink, J. A1 - Volk, H. J. A1 - Vuillaume, T. A1 - Wadiasingh, Z. A1 - Wagner, S. J. A1 - Watson, J. A1 - Werner, F. A1 - White, R. A1 - Wierzcholska, A. A1 - Wong, Yu Wun A1 - Yusafzai, A. A1 - Zacharias, M. A1 - Zanin, R. A1 - Zargaryan, D. A1 - Zdziarski, A. A. A1 - Zech, Alraune A1 - Zhu, S. J. A1 - Ziegler, A. A1 - Zorn, J. A1 - Zouari, S. A1 - Zywucka, N. T1 - An extreme particle accelerator in the Galactic plane BT - HESS J1826-130 JF - Astronomy and astrophysics : an international weekly journal N2 - The unidentified very-high-energy (VHE; E > 0.1 TeV) gamma -ray source, HESS J1826-130, was discovered with the High Energy Stereoscopic System (HESS) in the Galactic plane. The analysis of 215 h of HESS data has revealed a steady gamma -ray flux from HESS J1826-130, which appears extended with a half-width of 0.21 degrees +/- 0.02
(stat)degrees
stat degrees +/- 0.05
(sys)degrees sys degrees . The source spectrum is best fit with either a power-law function with a spectral index Gamma = 1.78 +/- 0.10(stat) +/- 0.20(sys) and an exponential cut-off at 15.2
(+5.5)(-3.2) -3.2+5.5 TeV, or a broken power-law with Gamma (1) = 1.96 +/- 0.06(stat) +/- 0.20(sys), Gamma (2) = 3.59 +/- 0.69(stat) +/- 0.20(sys) for energies below and above E-br = 11.2 +/- 2.7 TeV, respectively. The VHE flux from HESS J1826-130 is contaminated by the extended emission of the bright, nearby pulsar wind nebula, HESS J1825-137, particularly at the low end of the energy spectrum. Leptonic scenarios for the origin of HESS J1826-130 VHE emission related to PSR J1826-1256 are confronted by our spectral and morphological analysis. In a hadronic framework, taking into account the properties of dense gas regions surrounding HESS J1826-130, the source spectrum would imply an astrophysical object capable of accelerating the parent particle population up to greater than or similar to 200 TeV. Our results are also discussed in a multiwavelength context, accounting for both the presence of nearby supernova remnants, molecular clouds, and counterparts detected in radio, X-rays, and TeV energies. KW - ISM: supernova remnants KW - ISM: clouds KW - gamma rays: general KW - gamma rays: KW - ISM Y1 - 2020 U6 - https://doi.org/10.1051/0004-6361/202038851 SN - 0004-6361 SN - 1432-0746 VL - 644 PB - EDP Sciences CY - Les Ulis ER -