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Publication Open Access The 11 yr of low activity of the magnetar XTE J1810-197(2019); ; ; ;Turolla, Roberto; ;Rea, Nanda; In 2003, the magnetar XTE J1810-197 started an outburst that lasted until early 2007. In the following 11 yr, the source stayed in a quiescent/low-activity phase. XTE J1810-197 is one of the closest magnetars, hence its X-ray properties can be studied in detail even in quiescence and an extended monitoring has been carried out to study its long-term timing and spectral evolution. Here, we report the results of new X-ray observations, taken between 2017 September and 2018 April, with XMM-Newton, Chandra, and NICER. We derived a phase-connected timing solution yielding a frequency derivative of -9.26(6) × 10-14 Hz s-1. This value is consistent with that measured between 2009 and 2011, indicating that the pulsar spin-down rate remained quite stable during the long quiescent period. A spectral analysis of all the X-ray observations taken between 2009 and 2018 does not reveal significant spectral and/or flux variability. The spectrum of XTE J1810-197 can be described by the sum of two thermal components with temperatures of 0.15 and 0.3 keV, plus a power-law component with photon index 0.6. We also found evidence for an absorption line at ∼1.2 keV and width of 0.1 keV. Due to the long exposure time of the summed XMM-Newton observations, we could also carry out a phase-resolved spectral analysis for this source in quiescence. This showed that the flux modulation can be mainly ascribed to the warmer of the two thermal components, whose flux varies by ∼45 per cent along the pulse phase.Scopus© Citations 14 170 38 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The 2009 multiwavelength campaign on Mrk 421: Variability and correlation studies(2015) ;Aleksić, J. ;Ansoldi, S.; ;Antoranz, P. ;Babic, A. ;Bangale, P. ;Barres de Almeida, U. ;Barrio, J. A. ;Becerra González, J. ;Bednarek, W. ;Berger, K.; ;Palatiello, M. ;Paneque, D. ;Paoletti, R. ;Paredes, J. M. ;Paredes-Fortuny, X. ;Partini, S.; ;Prada, F. ;Prada Moroni, P. G. ;Bernardini, E.; ;Preziuso, S. ;Puljak, I. ;Reinthal, R. ;Rhode, W. ;Ribó, M. ;Rico, J. ;RodriguezGarcia, J. ;Rügamer, S. ;Saggion, A. ;Biland, A. ;Saito, K. ;Salvati, M. ;Satalecka, K. ;Scalzotto, V. ;Scapin, V. ;Schultz, C. ;Schweizer, T. ;Shore, S. N. ;Sillanpää, A. ;Sitarek, J. ;Blanch, O. ;Snidaric, I. ;Sobczynska, D. ;Spanier, F. ;Stamatescu, V.; ;Steinbring, T. ;Storz, J. ;Sun, S. ;Surić, T. ;Takalo, L. ;Bock, R. K.; ;Temnikov, P. ;Terzić, T. ;Tescaro, D. ;Teshima, M. ;Thaele, J. ;Tibolla, O. ;Torres, D. F. ;Toyama, T. ;Treves, A. ;Bonnefoy, S. ;Uellenbeck, M. ;Vogler, P. ;Wagner, R. M. ;Zandanel, F. ;Zanin, R. ;MAGIC Collaboration ;Archambault, S. ;Behera, B. ;Beilicke, M. ;Benbow, W.; ;Bird, R. ;Buckley, J. H. ;Bugaev, V. ;Cerruti, M. ;Chen, X. ;Ciupik, L. ;Collins-Hughes, E. ;Cui, W. ;Dumm, J. ;Eisch, J. D. ;Borracci, F. ;Falcone, A. ;Federici, S. ;Feng, Q. ;Finley, J. P. ;Fleischhack, H. ;Fortin, P. ;Fortson, L. ;Furniss, A. ;Griffin, S. ;Griffiths, S. T. ;Bretz, T. ;Grube, J. ;Gyuk, G. ;Hanna, D. ;Holder, J. ;Hughes, G. ;Humensky, T. B. ;Johnson, C. A. ;Kaaret, P. ;Kertzman, M. ;Khassen, Y. ;Carmona, E. ;Kieda, D. ;Krawczynski, H. ;Krennrich, F. ;Kumar, S. ;Lang, M. J. ;Maier, G. ;McArthur, S. ;Meagher, K. ;Moriarty, P. ;Mukherjee, R.; ;Ong, R. A. ;Otte, A. N. ;Park, N. ;Pichel, A. ;Pohl, M. ;Popkow, A. ;Prokoph, H. ;Quinn, J. ;Ragan, K. ;Rajotte, J. ;Carreto Fidalgo, D. ;Reynolds, P. T. ;Richards, G. T. ;Roache, E. ;Rovero, A. C. ;Sembroski, G. H. ;Shahinyan, K. ;Staszak, D. ;Telezhinsky, I. ;Theiling, M. ;Tucci, J. V. ;Colin, P. ;Tyler, J. ;Varlotta, A. ;Wakely, S. P. ;Weekes, T. C. ;Weinstein, A. ;Welsing, R. ;Wilhelm, A. ;Williams, D. A. ;Zitzer, B. ;VERITAS Collaboration ;Colombo, E.; ; ;Aller, H. D. ;Aller, M. F. ;Chen, W. P. ;Jordan, B. ;Koptelova, E. ;Kurtanidze, O. M. ;Lähteenmäki, A. ;McBreen, B. ;Contreras, J. L. ;Larionov, V. M. ;Lin, C. S. ;Nikolashvili, M. G. ;Angelakis, E.; ;Carramiñana, A. ;Carrasco, L.; ;Cesarini, A. ;Fuhrmann, L. ;Cortina, J.; ;Hovatta, T. ;Krichbaum, T. P. ;Krimm, H. A. ;Max-Moerbeck, W. ;Moody, J. W.; ;Mori, Y. ;Nestoras, I.; ; ;Pace, C. ;Pearson, R.; ;Readhead, A. C. S. ;Richards, J. L. ;Sadun, A. C. ;Sakamoto, T. ;Tammi, J. ;Tornikoski, M. ;Yatsu, Y. ;Da Vela, P. ;Zook, A.; ;De Angelis, A. ;De Caneva, G. ;De Lotto, B. ;Delgado Mendez, C. ;Doert, M. ;Domínguez, A. ;Dominis Prester, D. ;Dorner, D. ;Doro, M. ;Einecke, S. ;Eisenacher, D. ;Elsaesser, D. ;Farina, E. ;Ferenc, D. ;Fonseca, M. V. ;Font, L. ;Frantzen, K. ;Fruck, C. ;García López, R. J. ;Garczarczyk, M. ;Garrido Terrats, D. ;Gaug, M. ;Giavitto, G. ;Godinović, N. ;González Muñoz, A. ;Gozzini, S. R. ;Hadamek, A. ;Hadasch, D. ;Herrero, A. ;Hildebrand, D. ;Hose, J. ;Hrupec, D. ;Idec, W. ;Kadenius, V. ;Kellermann, H. ;Knoetig, M. L. ;Krause, J. ;Kushida, J.; ;Lelas, D. ;Lewandowska, N. ;Lindfors, E. ;Longo, F.; ;López, M. ;López-Coto, R. ;López-Oramas, A. ;Lorenz, E. ;Lozano, I. ;Makariev, M. ;Mallot, K. ;Maneva, G. ;Mankuzhiyil, N. ;Mannheim, K. ;Maraschi, L. ;Marcote, B. ;Mariotti, M. ;Martínez, M. ;Mazin, D. ;Menzel, U. ;Meucci, M. ;Miranda, J. M. ;Mirzoyan, R. ;Moralejo, A. ;Munar-Adrover, P. ;Nakajima, D. ;Niedzwiecki, A. ;Nilsson, K. ;Nowak, N. ;Orito, R.Overkemping, A.
Aims: We perform an extensive characterization of the broadband emission of Mrk 421, as well as its temporal evolution, during the non-flaring (low) state. The high brightness and nearby location (z = 0.031) of Mrk 421 make it an excellent laboratory to study blazar emission. The goal is to learn about the physical processes responsible for the typical emission of Mrk 421, which might also be extended to other blazars that are located farther away and hence are more difficult to study.
Methods: We performed a 4.5-month multi-instrument campaign on Mrk 421 between January 2009 and June 2009, which included VLBA, F-GAMMA, GASP-WEBT, Swift, RXTE, Fermi-LAT, MAGIC, and Whipple, among other instruments and collaborations. This extensive radio to very-high-energy (VHE; E> 100 GeV) γ-ray dataset provides excellent temporal and energy coverage, which allows detailed studies of the evolution of the broadband spectral energy distribution.
Results: Mrk421 was found in its typical (non-flaring) activity state, with a VHE flux of about half that of the Crab Nebula, yet the light curves show significant variability at all wavelengths, the highest variability being in the X-rays. We determined the power spectral densities (PSD) at most wavelengths and found that all PSDs can be described by power-laws without a break, and with indices consistent with pink/red-noise behavior. We observed a harder-when-brighter behavior in the X-ray spectra and measured a positive correlation between VHE and X-ray fluxes with zero time lag. Such characteristics have been reported many times during flaring activity, but here they are reported for the first time in the non-flaring state. We also observed an overall anti-correlation between optical/UV and X-rays extending over the duration of the campaign.
Conclusions: The harder-when-brighter behavior in the X-ray spectra and the measured positive X-ray/VHE correlation during the 2009 multi-wavelength campaign suggests that the physical processes dominating the emission during non-flaring states have similarities with those occurring during flaring activity. In particular, this observation supports leptonic scenarios as being responsible for the emission of Mrk 421 during non-flaring activity. Such a temporally extended X-ray/VHE correlation is not driven by any single flaring event, and hence is difficult to explain within the standard hadronic scenarios. The highest variability is observed in the X-ray band, which, within the one-zone synchrotron self-Compton scenario, indicates that the electron energy distribution is most variable at the highest energies.Appendix A is available in electronic form at http://www.aanda.orgThe complete data set shown in Fig. 1 is only available at the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr (ftp://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/576/A126
Scopus© Citations 102 292 59 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 3HSP J095507.9+355101: a flaring extreme blazar coincident in space and time with IceCube-200107A(2020) ;Giommi, P. ;Padovani, P. ;Oikonomou, F. ;Glauch, T.; Resconi, E.The uncertainty region of the highly energetic neutrino IceCube200107A includes 3HSP J095507.9+355101 ($z$~=~0.557), an extreme blazar, which was detected in a high, very hard, and variable X-ray state shortly after the neutrino arrival. Following a detailed multi-wavelength investigation, we confirm that the source is a genuine BL Lac, contrary to TXS 0506+056, the first source so far associated with IceCube neutrinos, which is a "masquerading" BL Lac. As in the case of TXS0506+056, 3HSP J095507.9+355101 is also way off the so-called "blazar sequence". We consider 3HSP J095507.9+355101 a possible counterpart to the IceCube neutrino. Finally, we discuss some theoretical implications in terms of neutrino production.Scopus© Citations 46 58 9 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A detailed study of the very high-energy Crab pulsar emission with the LST-1(2024) ;Abe, K. ;Abe, S. ;Abhishek, A. ;Acero, F. ;Aguasca-Cabot, A. ;Agudo, I. ;Alvarez Crespo, N.; ;Aramo, C. ;Arbet-Engels, A. ;Arcaro, C. ;Takeishi, R. ;Tam, P. H. T. ;Tanaka, S. J. ;Tateishi, D. ;Tavernier, T. ;Bhattacharjee, P. ;Temnikov, P. ;Terada, Y. ;Terauchi, K. ;Hassan, T. ;Morcuende, D. ;Terzic, T. ;Teshima, M. ;Tluczykont, M. ;Tokanai, F. ;Torres, D. F. ;Travnicek, P. ;Truzzi, S.; ; ;Vacula, M. ;Morselli, A. ;Hayashi, K.; ;van Scherpenberg, J. ;Vázquez Acosta, M. ;Verna, G. ;Viale, I. ;Vigliano, A. ;Vigorito, C. F. ;Visentin, E. ;Bissaldi, E. ;Moya, V. ;Vitale, V. ;Artero, M. ;Voitsekhovskyi, V. ;Voutsinas, G. ;Vovk, I. ;Vuillaume, T. ;Walter, R. ;Wan, L. ;Will, M. ;Yamamoto, T. ;Muraishi, H. ;Yamazaki, R. ;Blanch, O. ;Heckmann, L. ;Yeung, P. K. H. ;Yoshida, T. ;Yoshikoshi, T. ;Zhang, W. ;Zywucka, N.; ;Bordas, P. ;Nagataki, S. ;Brunelli, G.; ;Burelli, I. ;Heller, M. ;Burmistrov, L. ;Buscemi, M.; ;Caroff, S.; ;Carrasco, M. S. ;Nakamori, T. ;Cassol, F. ;Castrejón, N. ;Cauz, D. ;Cerasole, D. ;Herrera Llorente, J. ;Ceribella, G. ;Chai, Y. ;Cheng, K. ;Chiavassa, A. ;Chikawa, M. ;Neronov, A. ;Chon, G. ;Chytka, L. ;Cicciari, G. M. ;Cifuentes, A. ;Contreras, J. L. ;Hirotani, K. ;Cortina, J. ;Costantini, H. ;Da Vela, P. ;Dalchenko, M. ;Nickel, L.; ;De Angelis, A. ;de Bony de Lavergne, M. ;De Lotto, B. ;de Menezes, R. ;Del Peral, L. ;Hoffmann, D. ;Delgado, C. ;Delgado Mengual, J. ;della Volpe, D. ;Nievas Rosillo, M. ;Dellaiera, M. ;Di Piano, A. ;Di Pierro, F. ;Di Tria, R. ;Di Venere, L. ;Díaz, C. ;Dominik, R. M. ;Horns, D. ;Dominis Prester, D. ;Donini, A. ;Barrio, J. A. ;Dorner, D. ;Doro, M. ;Eisenberger, L. ;Elsässer, D. ;Emery, G. ;Escudero, J. ;Fallah Ramazani, V. ;Ferrarotto, F. ;Houles, J. ;Fiasson, A. ;Grau, R. ;Foffano, L. ;Freixas Coromina, L. ;Fröse, S. ;Fukazawa, Y. ;Garcia López, R. ;Gasbarra, C. ;Gasparrini, D. ;Gavira, L. ;Geyer, D. ;Hrabovsky, M. ;Nikolic, L. ;Giesbrecht Paiva, J. ;Giglietto, N. ;Giordano, F. ;Gliwny, P. ;Godinovic, N. ;Hrupec, D. ;Hui, D. ;Asano, K. ;Iarlori, M. ;Imazawa, R. ;Nishijima, K. ;Inada, T. ;Inome, Y. ;Ioka, K. ;Iori, M. ;Jimenez Martinez, I. ;Jiménez Quiles, J. ;Jurysek, J. ;Kagaya, M. ;Aubert, P. ;Karas, V. ;Noda, K. ;Katagiri, H. ;Kataoka, J. ;Kerszberg, D. ;Kobayashi, Y. ;Kohri, K. ;Kong, A. ;Kubo, H. ;Kushida, J. ;Lainez, M. ;Baktash, A. ;Nosek, D. ;Lamanna, G.; ;Lemoigne, L. ;Linhoff, M. ;Longo, F. ;López-Coto, R. ;López-Moya, M. ;López-Oramas, A. ;Loporchio, S. ;Lorini, A. ;Novotny, V. ;Bamba, A. ;Lozano Bahilo, J. ;Luque-Escamilla, P. L. ;Majumdar, P. ;Makariev, M. ;Mallamaci, M. ;Mandat, D. ;Manganaro, M. ;Manicò, G. ;Mannheim, K. ;Nozaki, S.; ;Baquero Larriva, A. ;Mariotti, M. ;Marquez, P. ;Marsella, G. ;Martí, J. ;Martinez, O. ;Martínez, G. ;Martínez, M. ;Mas-Aguilar, A. ;Ohishi, M. ;Maurin, G. ;Mazin, D.; ;Mestre Guillen, E. ;Micanovic, S. ;Miceli, D. ;Miener, T. ;Miranda, J. M. ;Mirzoyan, R. ;Mizuno, T. ;Ohtani, Y. ;Molero Gonzalez, M. ;Molina, E. ;Montaruli, T. ;Barres de Almeida, U. ;Moralejo, A. ;Oka, T. ;Okumura, A. ;Green, D. ;Batkovic, I. ;Orito, R. ;Otero-Santos, J. ;Ottanelli, P. ;Owen, E. ;Palatiello, M. ;Paneque, D. ;Pantaleo, F. R. ;Paoletti, R. ;Paredes, J. M.; ;Pech, M. ;Baxter, J. ;Pecimotika, M. ;Peresano, M. ;Pfeiffle, F. ;Pietropaolo, E. ;Pihet, M. ;Pirola, G. ;Plard, C. ;Podobnik, F. ;Gunji, S. ;Pons, E.; ;Becerra Gonzáilez, J. ;Priyadarshi, C. ;Prouza, M. ;Rando, R. ;Rhode, W. ;Ribó, M.; ;Rizi, V. ;Günther, P. ;Rodriguez Fernandez, G. ;Rodríguez Frías, M. D. ;Saito, T. ;Bernardini, E. ;Sakurai, S. ;Sanchez, D. A. ;Sano, H. ;Šarić, T. ;Sato, Y.; ;Hackfeld, J. ;Savchenko, V.; ;Schleicher, B. ;Schmuckermaier, F. ;Bernete Medrano, J. ;Schubert, J. L. ;Schussler, F. ;Schweizer, T. ;Seglar Arroyo, M. ;Siegert, T. ;Hadasch, D. ;Silvia, R. ;Sitarek, J. ;Sliusar, V. ;Strišković, J. ;Strzys, M. ;Berti, A. ;Suda, Y. ;Tajima, H. ;Takahashi, H. ;Takahashi, M. ;Hahn, A.Takata, J.Context. To date, three pulsars have been firmly detected by imaging atmospheric Cherenkov telescopes (IACTs). Two of them reached the TeV energy range, challenging models of very high-energy (VHE) emission in pulsars. More precise observations are needed to better characterize pulsar emission at these energies. The LST-1 is the prototype of the large-sized telescopes, which will be part of the Cherenkov Telescope Array Observatory (CTAO). Its improved performance over previous IACTs makes it well suited for studying pulsars. Aims. In this work we study the Crab pulsar emission with the LST-1, improving upon and complementing the results from other telescopes. Crab pulsar observations can also be used to characterize the potential of the LST-1 to study other pulsars and detect new ones. Methods. We analyzed a total of ∼103 hours of gamma-ray observations of the Crab pulsar conducted with the LST-1 in the period from September 2020 to January 2023. The observations were carried out at zenith angles of less than 50 degrees. To characterize the Crab pulsar emission over a broader energy range, a new analysis of the Fermi/LAT data, including ∼14 years of observations, was also performed. Results. The Crab pulsar phaseogram, long-term light curve, and phase-resolved spectra are reconstructed with the LST-1 from 20 GeV to 450 GeV for the first peak and up to 700 GeV for the second peak The pulsed emission is detected with a significance level of 15.2σ. The two characteristic emission peaks of the Crab pulsar are clearly detected (> 10σ), as is the so-called bridge emission between them (5.7σ). We find that both peaks are described well by power laws, with spectral indices of ∼3.44 and ∼3.03, respectively. The joint analysis of Fermi/LAT and LST-1 data shows a good agreement between the two instruments in their overlapping energy range. The detailed results obtained from the first observations of the Crab pulsar with the LST-1 show the potential that CTAO will have to study this type of source.Scopus© Citations 1 99 19 - Some of the metrics are blocked by yourconsent settings
Publication Open Access A Swift view on IGR J19149+1036IGR J19149+1036 is a high-mass X-ray binary detected by INTEGRAL in 2011 in the hard X-ray domain. We have analysed the Burst Alert Telescope (BAT) survey data of the first 103 months of the Swift mission detecting this source at a significance level of ̃30 standard deviations. The timing analysis on the long-term BAT light curve reveals the presence of a strong sinusoidal intensity modulation of 22.25 ± 0.05 d, that we interpret as the orbital period of this binary system. A broad-band (0.3-150 keV) spectral analysis was performed combining the BAT spectrum and the X-Ray Telescope (XRT) spectra from the pointed follow-up observations. The spectrum is adequately modelled with an absorbed power law with a high-energy cutoff at ̃24 keV and an absorption cyclotron feature at ̃31 keV. Correcting for the gravitational redshift, the inferred magnetic field at the neutron star surface is Bsurf ̃ 3.6 × 1012 G.Scopus© Citations 5 143 71 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The absolute calibration strategy of the ASTRI SST-2M telescope proposed for the Cherenkov Telescope Array and its external ground-based illumination system(2016); ; ; ;Biondo, B.; ; ; ; ; ; ASTRI is the end-to-end prototype for the CTA small-size class of telescopes in a dual-mirror configuration (SST-2M) proposed by the Italian National Institute of Astrophysics (INAF) in the framework of the Cherenkov Telescope Array. ASTRI SST-2M has been installed at the Serra La Nave Astrophysical Observatory on Mount Etna (Sicily) and its Performance Verification Phase will start in autumn 2016. For the relative pixel calibration and gain monitoring, the ASTRI SST-2M camera is equipped with an internal illumination device, while an external, portable, illumination system, placed at a few km distance from the telescope, will be used for the absolute end-to-end calibration of the telescope spectral response. Moreover analysis of signals induced in the camera pixels by the night sky background (diffuse emission and reference stars) will be used to monitor the long term evolution of the telescope calibration. We present an overview of the ASTRI SST-2M absolute calibration strategy and the external illuminating device that will be used for its spectral calibrationScopus© Citations 12 155 67 - Some of the metrics are blocked by yourconsent settings
Publication Restricted An accreting pulsar with extreme properties drives an ultraluminous x-ray source in NGC 5907(2017); ;Belfiore, Andrea; ; ; ; ; ; ; ;Puccetti, Simonetta; ;Salvetti, David; ; ;D'Agostino, Daniele ;Greiner, Jochen ;Haberl, Frank ;Novara, Giovanni; ;Turolla, Roberto ;Watson, Mike ;Wilms, JoernUltraluminous x-ray sources (ULXs) in nearby galaxies shine brighter than any x-ray source in our Galaxy. ULXs are usually modeled as stellar-mass black holes (BHs) accreting at very high rates or intermediate-mass BHs. We present observations showing that NGC 5907 ULX is instead an x-ray accreting neutron star (NS) with a spin period evolving from 1.43 seconds in 2003 to 1.13 seconds in 2014. It has an isotropic peak luminosity of ~1000 times the Eddington limit for a NS at 17.1 megaparsec. Standard accretion models fail to explain its luminosity, even assuming beamed emission, but a strong multipolar magnetic field can describe its properties. These findings suggest that other extreme ULXs (x-ray luminosity ≥ 1041 erg second-1) might harbor NSs.Scopus© Citations 368 155 58 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Accretion in Stellar-Mass Black Holes at High X-ray Spectral Resolution(2019) ;Miller, Jon ;Barret, Didier ;Cackett, Edward ;Diaz Trigo, Maria ;Done, Christine ;Gallo, Elena ;Kaastra, Jelle ;Motch, Christian; ; ;Webb, NatalieZoghbi, AbderahmenAccretion disks around stellar-mass black holes are optimal regimes in which to make observational tests of seminal theory that applies across the mass scale. High X-ray spectral resolution will enable the most incisive tests. This white paper briefly reviews the key ideas and examines three case studies.132 26 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Accretion in strong field gravity with eXTP(2019); ;Uttley, Phil ;Gou, LiJun ;Liu, Yuan ;Bambi, Cosimo ;Barret, Didier; ;Berti, Emanuele ;BIANCHI, STEFANO ;Caiazzo, Ilaria; ;Yuan, Feng ;in't Zand, Jean J. M. ;Zdziarski, Andrzej A. ;Zhou, XinLin; ;Ferrari, Valeria ;Gualtieri, Leonardo ;Heyl, Jeremy ;Ingram, Adam ;Karas, Vladimir ;Lu, FangJun ;Luo, Bin; ; ;Neilsen, Joseph ;Pani, Paolo ;Santangelo, Andrea ;Shu, XinWen ;Wang, JunFeng ;Wang, Jian-Min ;Xue, YongQuan ;Xu, YuPeng ;Yuan, WeiMin ;Yuan, YeFei ;Zhang, Shuang-Nan ;Zhang, Shu ;Agudo, Ivan; ;Andersson, Nils ;Baglio, Cristina ;Bakala, Pavel ;Baykal, Altan ;Bhattacharyya, Sudip ;Bombaci, Ignazio; ; ; ;Cui, Wei K.; ;Dauser, Thomas; ;De Marco, Barbara; ;Done, Chris ;Dovčiak, Michal ;Fabian, Andrew C. ;Falanga, Maurizio ;Gambino, Angelo Francesco ;Gendre, Bruce ;Grinberg, Victoria ;Heger, Alexander ;Homan, Jeroen; ;Jiang, JiaChen ;Jin, ChiChuan ;Koerding, Elmar ;Linares, Manu ;Liu, Zhu ;Maccarone, Thomas J. ;Malzac, Julien ;Manousakis, Antonios ;Marin, Frédéric ;Marinucci, Andrea ;Mehdipour, Missagh ;Méndez, Mariano ;Migliari, Simone ;Miller, Cole ;Miniutti, Giovanni; ;O'Brien, Paul T. ;Osborne, Julian P. ;Petrucci, Pierre Olivier; ; ;Rodriguez, Jerome; ;Shao, LiJing ;Sobolewska, Malgosia ;Sramkova, Eva ;Stevens, Abigail L. ;Stiele, Holger; ;Stuchlik, Zdenek ;Svoboda, Jiri ;Tamburini, Fabrizio ;Tauris, Thomas M.; ;Torok, Gabriel ;Urbanec, Martin ;Vincent, FredericWu, QingWenIn this paper we describe the potential of the enhanced X-ray Timing and Polarimetry (eXTP) mission for studies related to accretion flows in the strong field gravity regime around both stellar-mass and supermassive black-holes. eXTP has the unique capability of using advanced "spectral-timing-polarimetry" techniques to analyze the rapid variations with three orthogonal diagnostics of the flow and its geometry, yielding unprecedented insight into the inner accreting regions, the effects of strong field gravity on the material within them and the powerful outflows which are driven by the accretion process. X-spinmeasurementsScopus© Citations 40 140 47 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Addendum al Documento Valutazione dei Rischi dedicato al rischio biologico derivante da Sars-CoV-2, protocollo di sicurezza anti-contagio misure di prevenzione e protezione formazione e informazione(IASF Palermo, 2020); ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; Number: 59Documento da allegare al Documento di Valutazione dei Rischi di ogni Struttura di Ricerca INAF - Istituto Nazionale di Astrofisica. Documento approvato con nota Circolare del 15 maggio 2020, numero 2482.350 149 - Some of the metrics are blocked by yourconsent settings
Publication Restricted Advances in Multi-Pixel Photon Counter technology: First characterization results(2016); ; ; ; ; ;Timpanaro, M. C.; ; ; ; Due to the recent advances in silicon photomultiplier technology, new types of Silicon Photomultiplier (SiPM), also named Multi-Pixel Photon Counter (MPPC) detectors have become recently available, demonstrating superior performance in terms of their most important electrical and optical parameters. This paper presents the latest characterization results of the novel Low Cross-Talk (LCT) MPPC families from Hamamatsu, where a noticeable fill-factor enhancement and cross-talk reduction is achieved. In addition, the newly adopted resin coating has been proven to yield improved photon detection capabilities in the 280-320 nm spectral range, making the new LCT MPPCs particularly suitable for emerging applications like Cherenkov Telescope Array, and Astroparticle Physics.Scopus© Citations 18 145 6 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Anatomy of the AGN in NGC 5548. II. The spatial, temporal, and physical nature of the outflow from HST/COS Observations(2015) ;Arav, N. ;Chamberlain, C. ;Kriss, G. A. ;Kaastra, J. S.; ;Mehdipour, M. ;Petrucci, P. -O. ;Steenbrugge, K. C. ;Behar, E. ;Bianchi, S. ;Boissay, R. ;Branduardi-Raymont, G. ;Costantini, E. ;Ely, J. C. ;Ebrero, J. ;di Gesu, L. ;Harrison, F. A. ;Kaspi, S. ;Malzac, J. ;De Marco, B. ;Matt, G. ;Nandra, K. P. ;Paltani, S. ;Peterson, B. M.; ; ;Pozo Nuñez, F.; ;Seta, H.; ;de Vries, C. P. ;Walton, D. J.Whewell, M.Context. AGN outflows are thought to influence the evolution of their host galaxies and of super massive black holes. Our deep multiwavelength campaign on NGC 5548 has revealed a new, unusually strong X-ray obscuration, accompanied by broad UV absorption troughs observed for the first time in this object. The X-ray obscuration caused a dramatic decrease in the incident ionizing flux on the outflow that produces the long-studied narrow UV absorption lines in this AGN. The resulting data allowed us to construct a comprehensive physical, spatial, and temporal picture for this enduring AGN wind.
Aims: We aim to determine the distance of the narrow UV outflow components from the central source, their total column-density, and the mechanism responsible for their observed absorption variability.
Methods: We study the UV spectra acquired during the campaign, as well as from four previous epochs (1998-2011). Our main analysis tools are ionic column-density extraction techniques, photoionization models based on the code CLOUDY, and collisional excitation simulations.
Results: A simple model based on a fixed total column-density absorber, reacting to changes in ionizing illumination, matches the very different ionization states seen in five spectroscopic epochs spanning 16 years. The main component of the enduring outflow is situated at 3.5 ± 1.1 pc from the central source, and its distance and number density are similar to those of the narrow-emitting-line region in this object. Three other components are situated between 5-70 pc and two are farther than 100 pc. The wealth of observational constraints and the anti-correlation between the observed X-ray and UV flux in the 2002 and 2013 epochs make our physical model a leading contender for interpreting trough variability data of quasar outflows.
Conclusions: This campaign, in combination with prior UV and X-ray data, yields the first simple model that can explain the physical characteristics and the substantial variability observed in an AGN outflow.Appendix A is available in electronic form at http://www.aanda.org
Scopus© Citations 82 150 32 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Anatomy of the AGN in NGC 5548. IV. The short-term variability of the outflows(2015) ;Di Gesu, L. ;Costantini, E. ;Ebrero, J. ;Mehdipour, M. ;Kaastra, J. S.; ;Petrucci, P. O.; ;Kriss, G. A. ;Bianchi, S. ;Branduardi-Raymont, G. ;De Marco, B.; ;Kaspi, S. ;Paltani, S.; ; ;Steenbrugge, K. C.Whewell, M.During an extensive multiwavelength campaign that we performed in 2013-2014, we found the prototypical Seyfert 1 galaxy NGC 5548 in an unusual condition of heavy and persistent obscuration. The newly discovered "obscurer" absorbs most of the soft X-ray continuum along our line of sight and lowers the ionizing luminosity received by the classical warm absorber. We present the analysis of the high resolution X-ray spectra collected with XMM-Newton and Chandra throughout the campaign, which are suitable to investigate the variability of both the obscurer and classical warm absorber. The time separation between these X-ray observations range from two days to eight months. On these timescales the obscurer is variable both in column density and in covering fraction. This is consistent with the picture of a patchy wind. The most significant variation occurred in September 2013 when the source brightened for two weeks. A higher and steeper intrinsic continuum and a lower obscurer covering fraction are both required to explain the spectral shape during the flare. We suggest that a geometrical change of the soft X-ray source behind the obscurer causes the observed drop in the covering fraction. Because of the higher soft X-ray continuum level, the September 2013 Chandra spectrum is the only X ray spectrum of the campaign in which individual features of the warm absorber could be detected. The spectrum shows absorption from Fe-UTA, O iv, and O v, consistent with belonging to the lower-ionization counterpart of the historical NGC 5548 warm absorber. Hence, we confirm that the warm absorber has responded to the drop in the ionizing luminosity caused by the obscurer.Scopus© Citations 28 163 28 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Anatomy of the AGN in NGC 5548. V. A clear view of the X-ray narrow emission lines(2015) ;Whewell, M. ;Branduardi-Raymont, G. ;Kaastra, J. S. ;Mehdipour, M. ;Steenbrugge, K. C. ;Bianchi, S. ;Behar, E. ;Ebrero, J.; ;Costantini, E. ;De Marco, B. ;Di Gesu, L. ;Kriss, G. A. ;Paltani, S. ;Peterson, B. M. ;Petrucci, P. -O.; Context. Our consortium performed an extensive multi-wavelength campaign of the nearby Seyfert 1 galaxy NGC 5548 in 2013-14. The source appeared unusually heavily absorbed in the soft X-rays, and signatures of outflowing absorption were also present in the UV. He-like triplets of neon, oxygen and nitrogen, and radiative recombination continuum (RRC) features were found to dominate the soft X-ray spectrum due to the low continuum flux.
Aims: Here we focus on characterising these narrow emission features using data obtained from the XMM-Newton RGS (770 ks stacked spectrum).
Methods: We use spex for our initial analysis of these features. Self-consistent photoionisation models from Cloudy are then compared with the data to characterise the physical conditions of the emitting region.
Results: Outflow velocity discrepancies within the O VII triplet lines can be explained if the X-ray narrow-line region (NLR) in NGC 5548 is absorbed by at least one of the six warm absorber components found by previous analyses. The RRCs allow us to directly calculate a temperature of the emitting gas of a few eV (~104 K), favouring photoionised conditions. We fit the data with a Cloudy model of log ξ = 1.45 ± 0.05 erg cm s-1, log NH = 22.9 ± 0.4 cm-2 and log vturb = 2.25 ± 0.5 km s-1 for the emitting gas; this is the first time the X-ray NLR gas in this source has been modelled so comprehensively. This allows us to estimate the distance from the central source to the illuminated face of the emitting clouds as 13.9 ± 0.6 pc, consistent with previous work.Scopus© Citations 19 138 24 - Some of the metrics are blocked by yourconsent settings
Publication Open Access 86 18 - Some of the metrics are blocked by yourconsent settings
Patent Open Access Apparatus and method for non-invasive inspection of solid bodies by muon imagingThe present invention has application in the technical field of measuring instruments and it relates to an apparatus for non-invasive inspection of solid bodies by muon imaging usable in civil engineering, archeology, volcanology, tectonics and everywhere a radiographic and/or tomographic non-destructive inspection of geological and/or engineering structures, even of large dimensions, is necessary The invention further relates to a method for non-invasive inspection by muon imaging implementable by said apparatus.267 127 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Are jet ubiquitous in ULXs?(2015); ; ;Costamante, L.A jet model represents well different X-ray states of the bright ULX IC342 X-1.166 40 - Some of the metrics are blocked by yourconsent settings
Publication Open Access The Array Data Acquisition System software architecture of the ASTRI Mini-Array project(SPIE, The International Society for Optical Engineering, 2022); ; ; ; ; ; ; ; ; ; ; ; ; ; ; The ASTRI (Astrofisica con Specchi a Tecnologia Replicante Italiana) Project was born as a collaborative international effort led by the Italian National Institute for Astrophysics (INAF) to design and realize an end-to-end prototype of the Small-Sized Telescope (SST) of the Cherenkov Telescope Array (CTA) in a dual-mirror configuration (2M). The prototype, named ASTRI-Horn, has been operational since 2014 at the INAF observing station located on Mt. Etna (Italy). The ASTRI Project is now building the ASTRI Mini-Array consisting of nine ASTRI-Horn-like telescopes to be installed and operated at the Teide Observatory (Spain). The ASTRI software is aimed at supporting the Assembly Integration and Verification (AIV), and the operations of the ASTRI Mini-Array. The Array Data Acquisition System (ADAS) includes all hardware, software and communication infrastructure required to gather the bulk data of the Cherenkov Cameras and the Intensity Interferometers installed on the telescopes, and make these data available to the Online Observation Quality System (OOQS) for the on-site quick look, and to the Data Processing System (DPS) for the off-site scientific pipeline. This contribution presents the ADAS software architecture according to the use cases and requirement specifications, with particular emphasis on the interfaces with the Back End Electronics (BEE) of the instruments, the array central control, the OOQS, and the DPS.Scopus© Citations 5 57 18 - Some of the metrics are blocked by yourconsent settings
Publication Open Access Arrival Directions of Cosmic Rays above 32 EeV from Phase One of the Pierre Auger Observatory(2022) ;Abreu, P.; ;Albury, J. M. ;Allekotte, I. ;Almeida Cheminant, K. ;Almela, A. ;Alvarez-Muñiz, J. ;Alves Batista, R. ;Ammerman Yebra, J. ;Anastasi, G. A. ;Anchordoqui, L. ;Andrada, B. ;Andringa, S. ;Aramo, C. ;Araújo Ferreira, P. R. ;Arnone, E. ;Arteaga Velázquez, J. C. ;Asorey, H. ;Assis, P. ;Avila, G. ;Avocone, E. ;Badescu, A. M. ;Bakalova, A. ;Balaceanu, A. ;Barbato, F. ;Bellido, J. A. ;Berat, C. ;Bertaina, M. E. ;Bhatta, G. ;Biermann, P. L. ;Binet, V. ;Bismark, K. ;Bister, T. ;Biteau, J. ;Blazek, J. ;Bleve, C. ;Blümer, J. ;Boháčová, M. ;Boncioli, D. ;Bonifazi, C. ;Bonneau Arbeletche, L. ;Borodai, N. ;Botti, A. M. ;Brack, J. ;Bretz, T. ;Brichetto Orchera, P. G. ;Briechle, F. L. ;Buchholz, P. ;Bueno, A. ;Buitink, S. ;Buscemi, M. ;Büsken, M. ;Caballero-Mora, K. S. ;Caccianiga, L. ;Canfora, F. ;Caracas, I. ;Caruso, R.; ;Catalani, F. ;Cataldi, G. ;Cazon, L. ;Cerda, M. ;Chinellato, J. A. ;Chudoba, J. ;Chytka, L. ;Clay, R. W. ;Cobos Cerutti, A. C. ;Colalillo, R. ;Coleman, A. ;Coluccia, M. R. ;Conceição, R. ;Condorelli, A. ;Consolati, G. ;Contreras, F. ;Convenga, F. ;Correia dos Santos, D. ;Covault, C. E. ;Dasso, S. ;Daumiller, K. ;Dawson, B. R. ;Day, J. A. ;de Almeida, R. M. ;de Jesús, J. ;de Jong, S. J. ;de Mello Neto, J. R. T. ;De Mitri, I. ;de Oliveira, J. ;de Oliveira Franco, D. ;de Palma, F. ;de Souza, V. ;De Vito, E. ;Del Popolo, A. ;del Río, M. ;Deligny, O. ;Deval, L. ;di Matteo, A. ;Dobre, M. ;Dobrigkeit, C. ;D'Olivo, J. C. ;Domingues Mendes, L. M. ;dos Anjos, R. C. ;Dova, M. T. ;Ebr, J. ;Engel, R. ;Epicoco, I. ;Erdmann, M. ;Escobar, C. O. ;Etchegoyen, A. ;Falcke, H. ;Farmer, J. ;Farrar, G. ;Fauth, A. C. ;Fazzini, N. ;Feldbusch, F. ;Fenu, F. ;Fick, B. ;Figueira, J. M. ;Filipčič, A. ;Fitoussi, T. ;Fodran, T. ;Fujii, T. ;Fuster, A. ;Galea, C. ;Galelli, C. ;García, B. ;Gemmeke, H. ;Gesualdi, F. ;Gherghel-Lascu, A. ;Ghia, P. L. ;Giaccari, U. ;Giammarchi, M. ;Glombitza, J. ;Gobbi, F. ;Gollan, F. ;Golup, G. ;Gómez Berisso, M. ;Gómez Vitale, P. F. ;Gongora, J. P. ;González, J. M. ;González, N. ;Goos, I. ;Góra, D.; ;Gottowik, M. ;Grubb, T. D. ;Guarino, F. ;Guedes, G. P. ;Guido, E. ;Hahn, S. ;Hamal, P. ;Hampel, M. R. ;Hansen, P. ;Harari, D. ;Harvey, V. M. ;Haungs, A. ;Hebbeker, T. ;Heck, D. ;Hill, G. C. ;Hojvat, C. ;Hörandel, J. R. ;Horvath, P. ;Hrabovský, M. ;Huege, T. ;Insolia, A. ;Isar, P. G. ;Janecek, P. ;Johnsen, J. A. ;Jurysek, J. ;Kääpä, A. ;Kampert, K. H. ;Keilhauer, B. ;Khakurdikar, A. ;Kizakke Covilakam, V. V. ;Klages, H. O. ;Kleifges, M. ;Kleinfeller, J. ;Knapp, F. ;Kunka, N. ;Lago, B. L. ;Langner, N. ;Leigui de Oliveira, M. A. ;Lenok, V. ;Letessier-Selvon, A. ;Lhenry-Yvon, I. ;Lo Presti, D. ;Lopes, L. ;López, R. ;Lu, L. ;Luce, Q. ;Lundquist, J. P. ;Machado Payeras, A. ;Mancarella, G. ;Mandat, D. ;Manning, B. C. ;Manshanden, J. ;Mantsch, P. ;Marafico, S. ;Mariani, F. M. ;Mariazzi, A. G. ;Mariş, I. C. ;Marsella, G. ;Martello, D. ;Martinelli, S. ;Martínez Bravo, O. ;Mastrodicasa, M. ;Mathes, H. J. ;Matthews, J. ;Matthiae, G. ;Mayotte, E. ;Mayotte, S. ;Mazur, P. O. ;Medina-Tanco, G. ;Melo, D. ;Menshikov, A. ;Michal, S. ;Micheletti, M. I. ;Miramonti, L. ;Mollerach, S. ;Montanet, F. ;Morejon, L. ;Morello, C. ;Mostafá, M. ;Müller, A. L. ;Muller, M. A. ;Mulrey, K. ;Mussa, R. ;Muzio, M. ;Namasaka, W. M. ;Nasr-Esfahani, A. ;Nellen, L. ;Nicora, G. ;Niculescu-Oglinzanu, M. ;Niechciol, M. ;Nitz, D. ;Norwood, I. ;Nosek, D. ;Novotny, V. ;Nožka, L. ;Nucita, A. ;Núñez, L. A. ;Oliveira, C. ;Palatka, M. ;Pallotta, J. ;Papenbreer, P. ;Parente, G. ;Parra, A. ;Pawlowsky, J. ;Pech, M. ;Pȩkala, J. ;Pelayo, R. ;Peña-Rodriguez, J. ;Pereira Martins, E. E. ;Perez Armand, J. ;Pérez Bertolli, C. ;Perrone, L. ;Petrera, S. ;Petrucci, C. ;Pierog, T. ;Pimenta, M. ;Pirronello, V. ;Platino, M. ;Pont, B. ;Pothast, M. ;Privitera, P. ;Prouza, M. ;Puyleart, A. ;Querchfeld, S. ;Rautenberg, J. ;Ravignani, D. ;Reininghaus, M. ;Ridky, J. ;Riehn, F. ;Risse, M. ;Rizi, V. ;Rodrigues de Carvalho, W. ;Rodriguez Rojo, J. ;Roncoroni, M. J. ;Rossoni, S. ;Roth, M. ;Roulet, E. ;Rovero, A. C. ;Ruehl, P. ;Saftoiu, A. ;Saharan, M. ;Salamida, F. ;Salazar, H. ;Salina, G. ;Sanabria Gomez, J. D. ;Sánchez, F. ;Santos, E. M. ;Santos, E. ;Sarazin, F. ;Sarmento, R. ;Sato, R. ;Savina, P. ;Schäfer, C. M. ;Scherini, V. ;Schieler, H. ;Schimassek, M. ;Schimp, M. ;Schlüter, F. ;Schmidt, D. ;Scholten, O. ;Schoorlemmer, H. ;Schovánek, P. ;Schröder, F. G. ;Schulte, J. ;Schulz, T. ;Sciutto, S. J. ;Scornavacche, M.; ;Sehgal, S. ;Shellard, R. C. ;Sigl, G. ;Silli, G. ;Sima, O. ;Smau, R. ;Šmída, R. ;Sommers, P. ;Soriano, J. F. ;Squartini, R. ;Stadelmaier, M. ;Stanca, D. ;Stanič, S. ;Stasielak, J. ;Stassi, P. ;Straub, M. ;Streich, A. ;Suárez-Durán, M. ;Sudholz, T. ;Suomijärvi, T. ;Supanitsky, A. D. ;Szadkowski, Z. ;Tapia, A. ;Taricco, C. ;Timmermans, C. ;Tkachenko, O. ;Tobiska, P. ;Todero Peixoto, C. J. ;Tomé, B. ;Torrès, Z. ;Travaini, A. ;Travnicek, P. ;Trimarelli, C. ;Tueros, M. ;Ulrich, R. ;Unger, M. ;Vaclavek, L. ;Vacula, M. ;Valdés Galicia, J. F. ;Valore, L. ;Varela, E. ;Vásquez-Ramírez, A. ;Veberič, D. ;Ventura, C. ;Vergara Quispe, I. D. ;Verzi, V. ;Vicha, J. ;Vink, J. ;Vorobiov, S. ;Wahlberg, H. ;Watanabe, C. ;Watson, A. A. ;Weindl, A. ;Wiencke, L. ;Wilczyński, H. ;Wittkowski, D. ;Wundheiler, B. ;Yushkov, A. ;Zapparrata, O. ;Zas, E. ;Zavrtanik, D. ;Zavrtanik, M. ;Zehrer, L.Pierre Auger CollaborationA promising energy range to look for angular correlations between cosmic rays of extragalactic origin and their sources is at the highest energies, above a few tens of EeV (1 EeV ≡ 1018 eV). Despite the flux of these particles being extremely low, the area of ~3000 km2 covered at the Pierre Auger Observatory, and the 17 yr data-taking period of the Phase 1 of its operations, have enabled us to measure the arrival directions of more than 2600 ultra-high-energy cosmic rays above 32 EeV. We publish this data set, the largest available at such energies from an integrated exposure of 122,000 km2 sr yr, and search it for anisotropies over the 3.4π steradians covered with the Observatory. Evidence for a deviation in excess of isotropy at intermediate angular scales, with ~15° Gaussian spread or ~25° top-hat radius, is obtained at the 4σ significance level for cosmic-ray energies above ~40 EeV.Scopus© Citations 64 46 23 - Some of the metrics are blocked by yourconsent settings
Publication Open Access An ASIC front-end for fluorescence and Cherenkov light detection with SiPM for space and ground applications(2020); ; ; ; ; ;OSTERIA, Giuseppe ;SCOTTI, Valentina ;MIYAMOTO, Hiroko ;VIGORITO, Carlo ;CASOLINO, MarcoDE DONATO, CinziaAstroparticle and High Energy Astrophysics space missions measuring extensive air showers produced by cosmic rays and neutrinos in atmosphere require detection of very faint and intense ultraviolet and visible light. Characteristics of the new generation of SiPM (Silicon PhotoMultiplier) are potentially right for this purpose. The capability to operate SiPM contemporarily in photon counting and in charge integration is strictly dependent indeed by the design of the front-end electronics (FEE). In this context, the challenge is to find the right balance and a feasible solution for managing SiPM with a FEE to be able to work, contemporarily and efficiently, in photon counting and charge integration. In this manuscript we present a new ASIC, named RADIOROC, that is an improvement of the CITIROC and that is at the end of its design phase: this chip will be able to work contemporarily in both the named modes. The RADIOROC characteristics and the first simulations carried out on the chip design will be presented.Scopus© Citations 10 144 161