TY - JOUR A1 - Abdo, A. A. A1 - Ackermann, Margit A1 - Ajello, M. A1 - Allafort, A. J. A1 - Baldini, L. A1 - Ballet, J. A1 - Barbiellini, G. A1 - Baring, M. G. A1 - Bastieri, D. A1 - Bechtol, K. C. A1 - Bellazzini, R. A1 - Berenji, B. A1 - Blandford, R. D. A1 - Bloom, E. D. A1 - Bonamente, E. A1 - Borgland, A. W. A1 - Bouvier, A. A1 - Brandt, T. J. A1 - Bregeon, Johan A1 - Brez, A. A1 - Brigida, M. A1 - Bruel, P. A1 - Buehler, R. A1 - Buson, S. A1 - Caliandro, G. A. A1 - Cameron, R. A. A1 - Cannon, A. A1 - Caraveo, P. A. A1 - Carrigan, Svenja A1 - Casandjian, J. M. A1 - Cavazzuti, E. A1 - Cecchi, C. A1 - Celik, O. A1 - Charles, E. A1 - Chekhtman, A. A1 - Cheung, C. C. A1 - Chiang, J. A1 - Ciprini, S. A1 - Claus, R. A1 - Cohen-Tanugi, J. A1 - Conrad, Jan A1 - Cutini, S. A1 - Dermer, C. D. A1 - de Palma, F. A1 - do Couto e Silva, E. A1 - Drell, P. S. A1 - Dubois, R. A1 - Dumora, D. A1 - Favuzzi, C. A1 - Fegan, S. J. A1 - Ferrara, E. C. A1 - Focke, W. B. A1 - Fortin, P. A1 - Frailis, M. A1 - Fuhrmann, L. A1 - Fukazawa, Y. A1 - Funk, S. A1 - Fusco, P. A1 - Gargano, F. A1 - Gasparrini, D. A1 - Gehrels, N. A1 - Germani, S. A1 - Giglietto, N. A1 - Giordano, F. A1 - Giroletti, M. A1 - Glanzman, T. A1 - Godfrey, G. A1 - Grenier, I. A. A1 - Guillemot, L. A1 - Guiriec, S. A1 - Hayashida, M. A1 - Hays, E. A1 - Horan, D. A1 - Hughes, R. E. A1 - Johannesson, G. A1 - Johnson, A. S. A1 - Johnson, W. N. A1 - Kadler, M. A1 - Kamae, T. A1 - Katagiri, H. A1 - Kataoka, J. A1 - Knoedlseder, J. A1 - Kuss, M. A1 - Lande, J. A1 - Latronico, L. A1 - Lee, S. -H. A1 - Lemoine-Goumard, M. A1 - Longo, F. A1 - Loparco, F. A1 - Lott, B. A1 - Lovellette, M. N. A1 - Lubrano, P. A1 - Madejski, G. M. A1 - Makeev, A. A1 - Max-Moerbeck, W. A1 - Mazziotta, Mario Nicola A1 - McEnery, J. E. A1 - Mehault, J. A1 - Michelson, P. F. A1 - Mitthumsiri, W. A1 - Mizuno, T. A1 - Moiseev, A. A. A1 - Monte, C. A1 - Monzani, M. E. A1 - Morselli, A. A1 - Moskalenko, I. V. A1 - Murgia, S. A1 - Naumann-Godo, M. A1 - Nishino, S. A1 - Nolan, P. L. A1 - Norris, J. P. A1 - Nuss, E. A1 - Ohsugi, T. A1 - Okumura, A. A1 - Omodei, N. A1 - Orlando, E. A1 - Ormes, J. F. A1 - Paneque, D. A1 - Panetta, J. H. A1 - Parent, D. A1 - Pavlidou, V. A1 - Pearson, T. J. A1 - Pelassa, V. A1 - Pepe, M. A1 - Pesce-Rollins, M. A1 - Piron, F. A1 - Porter, T. A. A1 - Raino, S. A1 - Rando, R. A1 - Razzano, M. A1 - Readhead, A. A1 - Reimer, A. A1 - Reimer, O. A1 - Richards, J. L. A1 - Ripken, J. A1 - Ritz, S. A1 - Roth, M. A1 - Sadrozinski, H. F. -W. A1 - Sanchez, D. A1 - Sander, A. A1 - Scargle, J. D. A1 - Sgro, C. A1 - Siskind, E. J. A1 - Smith, P. D. A1 - Spandre, G. A1 - Spinelli, P. A1 - Stawarz, L. A1 - Stevenson, M. A1 - Strickman, M. S. A1 - Sokolovsky, K. V. A1 - Suson, D. J. A1 - Takahashi, H. A1 - Takahashi, T. A1 - Tanaka, T. A1 - Thayer, J. B. A1 - Thayer, J. G. A1 - Thompson, D. J. A1 - Tibaldo, L. A1 - Torres, F. A1 - Tosti, G. A1 - Tramacere, A. A1 - Uchiyama, Y. A1 - Usher, T. L. A1 - Vandenbroucke, J. A1 - Vasileiou, V. A1 - Vilchez, N. A1 - Vitale, V. A1 - Waite, A. P. A1 - Wang, P. A1 - Wehrle, A. E. A1 - Winer, B. L. A1 - Wood, K. S. A1 - Yang, Z. A1 - Ylinen, T. A1 - Zensus, J. A. A1 - Ziegler, M. A1 - Aleksic, J. A1 - Antonelli, L. A. A1 - Antoranz, P. A1 - Backes, Michael A1 - Barrio, J. A. A1 - Gonzalez, J. Becerra A1 - Bednarek, W. A1 - Berdyugin, A. A1 - Berger, K. A1 - Bernardini, E. A1 - Biland, A. A1 - Blanch Bigas, O. A1 - Bock, R. K. A1 - Boller, A. A1 - Bonnoli, G. A1 - Bordas, Pol A1 - Tridon, D. Borla A1 - Bosch-Ramon, Valentin A1 - Bose, D. A1 - Braun, I. A1 - Bretz, T. A1 - Camara, M. A1 - Carmona, E. A1 - Carosi, A. A1 - Colin, P. A1 - Colombo, E. A1 - Contreras, J. L. A1 - Cortina, J. A1 - Covino, S. A1 - Dazzi, F. A1 - de Angelis, A. A1 - del Pozo, E. De Cea A1 - De Lotto, B. A1 - De Maria, M. A1 - De Sabata, F. A1 - Mendez, C. Delgado A1 - Ortega, A. Diago A1 - Doert, M. A1 - Dominguez, A. A1 - Prester, Dijana Dominis A1 - Dorner, D. A1 - Doro, M. A1 - Elsaesser, D. A1 - Ferenc, D. A1 - Fonseca, M. V. A1 - Font, L. A1 - Lopen, R. J. Garcia A1 - Garczarczyk, M. A1 - Gaug, M. A1 - Giavitto, G. A1 - Godinovi, N. A1 - Hadasch, D. A1 - Herrero, A. A1 - Hildebrand, D. A1 - Hoehne-Moench, D. A1 - Hose, J. A1 - Hrupec, D. A1 - Jogler, T. A1 - Klepser, S. A1 - Kraehenbuehl, T. A1 - Kranich, D. A1 - Krause, J. A1 - La Barbera, A. A1 - Leonardo, E. A1 - Lindfors, E. A1 - Lombardi, S. A1 - Lopez, M. A1 - Lorenz, E. A1 - Majumdar, P. A1 - Makariev, E. A1 - Maneva, G. A1 - Mankuzhiyil, N. A1 - Mannheim, K. A1 - Maraschi, L. A1 - Mariotti, M. A1 - Martinez, M. A1 - Mazin, D. A1 - Meucci, M. A1 - Miranda, J. M. A1 - Mirzoyan, R. A1 - Miyamoto, H. A1 - Moldon, J. A1 - Moralejo, A. A1 - Nieto, D. A1 - Nilsson, K. A1 - Orito, R. A1 - Oya, I. A1 - Paoletti, R. A1 - Paredes, J. M. A1 - Partini, S. A1 - Pasanen, M. A1 - Pauss, F. A1 - Pegna, R. G. A1 - Perez-Torres, M. A. A1 - Persic, M. A1 - Peruzzo, J. A1 - Pochon, J. A1 - Moroni, P. G. Prada A1 - Prada, F. A1 - Prandini, E. A1 - Puchades, N. A1 - Puljak, I. A1 - Reichardt, T. A1 - Reinthal, R. A1 - Rhode, W. A1 - Ribo, M. A1 - Rico, J. A1 - Rissi, M. A1 - Ruegamer, S. A1 - Saggion, A. A1 - Saito, K. A1 - Saito, T. Y. A1 - Salvati, M. A1 - Sanchez-Conde, M. A1 - Satalecka, K. A1 - Scalzotto, V. A1 - Scapin, V. A1 - Schultz, C. A1 - Schweizer, T. A1 - Shayduk, M. A1 - Shore, S. N. A1 - Sierpowska-Bartosik, A. A1 - Sillanpaa, A. A1 - Sitarek, J. A1 - Sobczynska, D. A1 - Spanier, F. A1 - Spiro, S. A1 - Stamerra, A. A1 - Steinke, B. A1 - Storz, J. A1 - Strah, N. A1 - Struebig, J. C. A1 - Suric, T. A1 - Takalo, L. O. A1 - Tavecchio, F. A1 - Temnikov, P. A1 - Terzic, T. A1 - Tescaro, D. A1 - Teshima, M. A1 - Vankov, H. A1 - Wagner, R. M. A1 - Weitzel, Q. A1 - Zabalza, V. A1 - Zandanel, F. A1 - Zanin, R. A1 - Acciari, V. A. A1 - Arlen, T. A1 - Aune, T. A1 - Benbow, W. A1 - Boltuch, D. A1 - Bradbury, S. M. A1 - Buckley, J. H. A1 - Bugaev, V. A1 - Cannon, A. A1 - Cesarini, A. A1 - Ciupik, L. A1 - Cui, W. A1 - Dickherber, R. A1 - Errando, M. A1 - Falcone, A. A1 - Finley, J. P. A1 - Finnegan, G. A1 - Fortson, L. A1 - Furniss, A. A1 - Galante, N. A1 - Gall, D. A1 - Gillanders, G. H. A1 - Godambe, S. A1 - Grube, J. A1 - Guenette, R. A1 - Gyuk, G. A1 - Hanna, D. A1 - Holder, J. A1 - Huang, D. A1 - Hui, C. M. A1 - Humensky, T. B. A1 - Kaaret, P. A1 - Karlsson, N. A1 - Kertzman, M. A1 - Kieda, D. A1 - Konopelko, A. A1 - Krawczynski, H. A1 - Krennrich, F. A1 - Lang, M. J. A1 - Maier, G. A1 - McArthur, S. A1 - McCann, A. A1 - McCutcheon, M. A1 - Moriarty, P. A1 - Mukherjee, R. A1 - Ong, R. A1 - Otte, N. A1 - Pandel, D. A1 - Perkins, J. S. A1 - Pichel, A. A1 - Pohl, M. A1 - Quinn, J. A1 - Ragan, K. A1 - Reyes, L. C. A1 - Reynolds, P. T. A1 - Roache, E. A1 - Rose, H. J. A1 - Rovero, A. C. A1 - Schroedter, M. A1 - Sembroski, G. H. A1 - Senturk, G. D. A1 - Steele, D. A1 - Swordy, S. P. A1 - Tesic, G. A1 - Theiling, M. A1 - Thibadeau, S. A1 - Varlotta, A. A1 - Vincent, S. A1 - Wakely, S. P. A1 - Ward, J. E. A1 - Weekes, T. C. A1 - Weinstein, A. A1 - Weisgarber, T. A1 - Williams, D. A. A1 - Wood, M. A1 - Zitzer, B. A1 - Villata, M. A1 - Raiteri, C. M. A1 - Aller, H. D. A1 - Aller, M. F. A1 - Arkharov, A. A. A1 - Blinov, D. A. A1 - Calcidese, P. A1 - Chen, W. P. A1 - Efimova, N. V. A1 - Kimeridze, G. A1 - Konstantinova, T. S. A1 - Kopatskaya, E. N. A1 - Koptelova, E. A1 - Kurtanidze, O. M. A1 - Kurtanidze, S. O. A1 - Lahteenmaki, A. A1 - Larionov, V. M. A1 - Larionova, E. G. A1 - Larionova, L. V. A1 - Ligustri, R. A1 - Morozova, D. A. A1 - Nikolashvili, M. G. A1 - Sigua, L. A. A1 - Troitsky, I. S. A1 - Angelakis, E. A1 - Capalbi, M. A1 - Carraminana, A. A1 - Carrasco, L. A1 - Cassaro, P. A1 - de la Fuente, E. A1 - Gurwell, M. A. A1 - Kovalev, Y. Y. A1 - Kovalev, Yu. A. A1 - Krichbaum, T. P. A1 - Krimm, H. A. A1 - Leto, Paolo A1 - Lister, M. L. A1 - Maccaferri, G. A1 - Moody, J. W. A1 - Mori, Y. A1 - Nestoras, I. A1 - Orlati, A. A1 - Pagani, C. A1 - Pace, C. A1 - Pearson, R. A1 - Perri, M. A1 - Piner, B. G. A1 - Pushkarev, A. B. A1 - Ros, E. A1 - Sadun, A. C. A1 - Sakamoto, T. A1 - Tornikoski, M. A1 - Yatsu, Y. A1 - Zook, A. T1 - Insights into the high-energy gamma-Ray emission of markarian 501 fromextensive multifrequency observations in the fermi era JF - The astrophysical journal : an international review of spectroscopy and astronomical physics N2 - We report on the gamma-ray activity of the blazar Mrk 501 during the first 480 days of Fermi operation. We find that the average Large Area Telescope (LAT) gamma-ray spectrum of Mrk 501 can be well described by a single power-law function with a photon index of 1.78 +/- 0.03. While we observe relatively mild flux variations with the Fermi-LAT (within less than a factor of two), we detect remarkable spectral variability where the hardest observed spectral index within the LAT energy range is 1.52 +/- 0.14, and the softest one is 2.51 +/- 0.20. These unexpected spectral changes do not correlate with the measured flux variations above 0.3 GeV. In this paper, we also present the first results from the 4.5 month long multifrequency campaign (2009 March 15-August 1) on Mrk 501, which included the Very Long Baseline Array (VLBA), Swift, RXTE, MAGIC, and VERITAS, the F-GAMMA, GASP-WEBT, and other collaborations and instruments which provided excellent temporal and energy coverage of the source throughout the entire campaign. The extensive radio to TeV data set from this campaign provides us with the most detailed spectral energy distribution yet collected for this source during its relatively low activity. The average spectral energy distribution of Mrk 501 is well described by the standard one-zone synchrotron self-Compton (SSC) model. In the framework of this model, we find that the dominant emission region is characterized by a size less than or similar to 0.1 pc (comparable within a factor of few to the size of the partially resolved VLBA core at 15-43 GHz), and that the total jet power (similar or equal to 10(44) erg s(-1)) constitutes only a small fraction (similar to 10(-3)) of the Eddington luminosity. The energy distribution of the freshly accelerated radiating electrons required to fit the time-averaged data has a broken power-law form in the energy range 0.3 GeV-10 TeV, with spectral indices 2.2 and 2.7 below and above the break energy of 20 GeV. We argue that such a form is consistent with a scenario in which the bulk of the energy dissipation within the dominant emission zone of Mrk 501 is due to relativistic, proton-mediated shocks. We find that the ultrarelativistic electrons and mildly relativistic protons within the blazar zone, if comparable in number, are in approximate energy equipartition, with their energy dominating the jet magnetic field energy by about two orders of magnitude. KW - acceleration of particles KW - BL Lacertae objects: general KW - BL Lacertae objects: individual (Mrk 501) KW - galaxies: active KW - gamma rays: general KW - radiation mechanisms: non-thermal Y1 - 2011 U6 - https://doi.org/10.1088/0004-637X/727/2/129 SN - 0004-637X VL - 727 IS - 2 PB - IOP Publ. Ltd. CY - Bristol ER - TY - JOUR A1 - Hnatkova, Katarina A1 - Vessel, N. A1 - Voss, Andreas A1 - Kurths, Jürgen A1 - Sander, A. A1 - Schirdewan, Alexander A1 - Camm, A. J. A1 - Malik, Marek T1 - Multiparametric analysis of heart rate variability used for risk stratification among survivors of acute myocardial infarction Y1 - 1998 SN - 0895-2795 ER - TY - JOUR A1 - Oskinova, Lida A1 - Steinke, M. A1 - Hamann, Wolf-Rainer A1 - Sander, A. A1 - Todt, Helge Tobias A1 - Liermann, Adriane T1 - One of the most massive stars in the Galaxy may have formed in isolation JF - Monthly notices of the Royal Astronomical Society N2 - Very massive stars, 100 times heavier than the sun, are rare. It is not yet known whether such stars can form in isolation or only in star clusters. The answer to this question is of fundamental importance. The central region of our Galaxy is ideal for investigating very massive stars and clusters located in the same environment. We used archival infrared images to investigate the surroundings of apparently isolated massive stars presently known in the Galactic Centre (GC). We find that two such isolated massive stars display bow shocks and hence may be 'runaways' from their birthplace. Thus, some isolated massive stars in the GC region might have been born in star clusters known in this region. However, no bow shock is detected around the isolated star WR 102ka (Peony nebula star), which is one of the most massive and luminous stars in the Galaxy. This star is located at the centre of an associated circumstellar nebula. To study whether a star cluster may be 'hidden' in the surroundings of WR 102ka, to obtain new and better spectra of this star, and to measure its radial velocity, we obtained observations with the integral-field spectrograph SINFONI at the ESO's Very Large Telescope. Our observations confirm that WR 102ka is one of the most massive stars in the Galaxy and reveal that this star is not associated with a star cluster. We suggest that WR 102ka has been born in relative isolation, outside of any massive star cluster. KW - stars: individual: WR 102ka KW - Galaxy: centre KW - infrared: stars Y1 - 2013 U6 - https://doi.org/10.1093/mnras/stt1817 SN - 0035-8711 SN - 1365-2966 VL - 436 IS - 4 SP - 3357 EP - 3365 PB - Oxford Univ. Press CY - Oxford ER - TY - JOUR A1 - Sander, A. A1 - Hamann, Wolf-Rainer A1 - Todt, Helge Tobias T1 - The Galactic WC stars Stellar parameters from spectral analyses indicate a new evolutionary sequence JF - Astronomy and astrophysics : an international weekly journal N2 - Context. The life cycles of massive stars from the main sequence to their explosion as supernovae or gamma ray bursts are not yet fully clear, and the empirical results from spectral analyses are partly in conflict with current evolutionary models. The spectral analysis of Wolf-Rayet stars requires the detailed modeling of expanding stellar atmospheres in non-LTE. The Galactic WN stars have been comprehensively analyzed with such models of the latest stage of sophistication, while a similarly comprehensive study of the Galactic WC sample remains undone. Aims. We aim to establish the stellar parameters and mass-loss rates of the Galactic WC stars. These data provide the empirical basis of studies of (i) the role of WC stars in the evolution of massive stars, (ii) the wind-driving mechanisms, and (iii) the feedback of WC stars as input to models of the chemical and dynamical evolution of galaxies. Methods. We analyze the nearly complete sample of un-obscured Galactic WC stars, using optical spectra as well as ultraviolet spectra when available. The observations are fitted with theoretical spectra, using the Potsdam Wolf-Rayet (PoWR) model atmosphere code. A large grid of line-blanked models has been established for the range of WC subtypes WC4 - WC8, and smaller grids for the WC9 parameter domain. Both WO stars and WN/WC transit types are also analyzed using special models. Results. Stellar and atmospheric parameters are derived for more than 50 Galactic WC and two WO stars, covering almost the whole Galactic WC population as far as the stars are single, and un-obscured in the visual. In the Hertzsprung-Russell diagram, the WC stars reside between the hydrogen and the helium zero-age main sequences, having luminosities L from 10(4.9) to 10(5.6) L-circle dot. The mass-loss rates scale very tightly with L-0.8. The two WO stars in our sample turn out to be outstandingly hot (approximate to 200 kK) and do not fit into the WC scheme. Conclusions. By comparing the empirical WC positions in the Hertzsprung-Russell diagram with evolutionary models, and from recent supernova statistics, we conclude that WC stars have evolved from initial masses between 20 solar masses and 45 M-circle dot. In contrast to previous assumptions, it seems that WC stars in general do not descend from the most massive stars. Only the WO stars might stem from progenitors that have been initially more massive than 45 M-circle dot. KW - stars: massive KW - stars: mass-loss KW - stars: Wolf-Rayet KW - stars: evolution KW - stars: atmospheres KW - stars: winds, outflows Y1 - 2012 U6 - https://doi.org/10.1051/0004-6361/201117830 SN - 0004-6361 VL - 540 PB - EDP Sciences CY - Les Ulis ER -