Hiromi Seta, Naoki Isobe, Makoto S. Tashiro, Yuichi Yaji, Akira Arai, Masayuki Fukuhara, Kotaro Kohno, Kouichiro Nakanishi, Mahito Sasada, Yoshito Shimajiri, Tomoka Tosaki, Makoto Uemura, Hans Anderhub, Lucio Angelo Antonelli, Pedro Antoranz, Michael Backes, Carmen Baixeras, Silvia Balestra, Juan Abel Barrio, Denis Bastieri, Josefa Becerra Gonzalez, Julia K. Becker, Wlodzimierz Bednarek, Karsten Berger, Elisa Bernardini, Adrian Biland, Rudolf K. Bock, Giacomo Bonnoli, Pol Bordas, Daniela Borla Tridon, Valenti Bosch-Ramon, Debanjan Bose, Isabel Braun, Thomas Bretz, Ilia Britvitch, Miguel Camara, Emiliano Carmona, Sebastian Commichau, Jose Luis Contreras, Juan Cortina, Ma Teresa Costado Dios, Stefano Covino, Valentin Curtef, Francesco Dazzi, Alessandro De Angelis, Elsa De Cea del Pozo, Raquel de los Reyes, Barbara De Lotto, Michela De Maria, Francesco De Sabata, Carlos Delgado Mendez, Alberto Dominguez, Daniela Dorner, Michele Doro, Dominik Elsaesser, Manel Errando, Daniela Ferenc, Enrique Fernandez, Roger Firpo, Maria Victoria Fonseca, Lluis Font, Nicola Galante, Ramon J. Garcia Lopez, Markus Garczarczyk, Markus Gaug, Florian Goebel, Daniela Hadasch, Masaaki Hayashida, Artemio Herrero, Dorothee Hildebrand, Daniel Hoehne-Moench, Juergen Hose, Ching Cheng Hsu, Tobias Jogler, Daniel Kranich, Antonio La Barbera, Alvin Laille, Elvira Leonardo, Elina Lindfors, Saverio Lombardi, Francesco Longo, Donatella Lopez, Eckart Lorenz, Pratik Majumdar, Galina Maneva, Nijil Mankuzhiyil, Karl Mannheim, Laura Maraschi, Mose Mariotti, Manel Martinez, Daniel Mazin, Mario Meucci, Markus Meyer, Jose Miguel Miranda, Razmick Mirzoyan, Hiroko Miyamoto, Javier Moldon, Mariano Moles, Abelardo Moralejo, Daniel Nieto, Kari Nilsson, Jelena Ninkovic, Nepomuk Otte, Igor Oya, Riccardo Paoletti, Josep M. Paredes, Mikko Pasanen, Donatella Pascoli, Felicitas Pauss, Raffaello G. Pegna, Miguel A. Perez-Torres, Massimo Persic, Luigi Peruzzo, Francisco Prada, Elisa Prandini, Neus Puchades, Ignasi Reichardt, Wolfgang Rhode, Marc Ribo, Javier Rico, Michael Rissi, Arnau Robert, Stefan Ruegamer, Antonio Saggion, Takayuki Y. Saito, Marco Salvati, Miguel Sanchez-Conde, Konstancja Satalecka, Villi Scalzotto, Valeria Scapin, Thomas Schweizer, Maxim Shayduk, Steve N. Shore, Nuria Sidro, Agnieszka Sierpowska-Bartosik, Aimo Sillanpaa, Julian Sitarek, Dorota Sobczynska, Felix Spanier, Antonio Stamerra, Luisa Sabrina Stark Schneebeli, Leo Takalo, Fabrizio Tavecchio, Petar Temnikov, Diego Tescaro, Masahiro Teshima, Martin Tluczykont, Diego F. Torres, Nicola Turini, Hristofor Vankov, Robert M. Wagner, Wolfgang Wittek, Victor Zabalza, Fabio Zandanel, Roberta Zanin, Jordi Zapatero
PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN 61(5) 1011-1022 2009年10月 査読有り
Suzaku observations of the blazar OJ 287 were performed in 2007 April 10-13 and November 7-9. They correspond to a quiescent and a flaring state, respectively. The X-ray spectra of the source can be well-described with single power-law models in both exposures. The derived X-ray photon index and the flux density at 1 keV were found to be Gamma = 1.65 +/- 0.02 and S-1 (keV) = 215 +/- 5 nJy in the quiescent state. In the flaring state, the source exhibited a harder X-ray spectrum (Gamma = 1.50 +/- 0.01) with a nearly doubled X-ray flux density of S-1 keV = 404(-5)(+6) nJy Moreover, significant hard X-ray signals were detected up to similar to 27 keV. In cooperation with Suzaku, simultaneous radio, optical, and very-high-energy gamma-ray observations of OJ 287 were performed with the Nobeyama Millimeter Array, the KANATA telescope, and the MAGIC telescope, respectively. The radio and optical fluxes in the flaring state (3.04 +/- 0.46 Jy and 8.93 +/- 0.05 mJy at 86.75 Hz and in the V-band, respectively) were found to be higher by a factor of 2-3 than those in the quiescent state (1.73 +/- 0.26 Jy and 3.03 +/- 0.01 mJy at 86.75 Hz and in the V-band, respectively). No notable gamma-ray events were detected in either observation. The spectral energy distribution of OJ 287 indicated that the X-ray spectrum was dominated by inverse Compton radiation in both observations, while synchrotron radiation exhibited a spectral cutoff at around the optical frequency. Furthermore, no significant difference in the synchrotron cutoff frequency was found between the quiescent and flaring states. According to a simple synchrotron self-Compton model, the change of the spectral energy distribution is due to an increase in the energy density of electrons with small changes of both the magnetic field strength and the maximum Lorentz factor of electrons.