TY - JOUR A1 - Adrián-Martínez, S. A1 - Ageron, M. A1 - Aharonian, F. A1 - Aiello, S. A1 - Albert, A. A1 - Ameli, F. A1 - Annasontzis, E. A1 - Andre, M. A1 - Androulakis, G. A1 - Anghinolfi, M. A1 - Anton, G. A1 - Ardid, M. A1 - Avgitas, T. A1 - Barbarino, G. A1 - Baret, B. A1 - Barrios-Martí, J. A1 - Belhorma, B. A1 - Belias, A. A1 - Berbee, A. A1 - van den Berg, A. A1 - Bertin, V. A1 - Beurthey, S. A1 - van Beeveren, V. A1 - Beverini, N. A1 - Biagi, S. A1 - Biagioni, A. A1 - Billault, M. A1 - Bondì, M. A1 - Bormuth, R. A1 - Bouhadef, B. A1 - Bourlis, G. A1 - Bourret, S. A1 - Boutonnet, C. A1 - Bouwhuis, M. A1 - Bozza, C. A1 - Bruijn, R. A1 - Brunner, J. A1 - Buis, E. A1 - Busto, J. A1 - Cacopardo, G. A1 - Caillat, L. A1 - Calmai, M. A1 - Calvo, D. A1 - Capone, A. A1 - Caramete, L. A1 - Cecchini, S. A1 - Celli, S. A1 - Champion, C. A1 - Cherkaoui El Moursli, R. A1 - Cherubini, S. A1 - Chiarusi, T. A1 - Circella, M. A1 - Classen, L. A1 - Cocimano, R. A1 - Coelho, J. A. B. A1 - Coleiro, A. A1 - Colonges, S. A1 - Coniglione, R. A1 - Cordelli, M. A1 - Cosquer, A. A1 - Coyle, P. A1 - Creusot, A. A1 - Cuttone, G. A1 - D'Amico, A. A1 - De Bonis, G. A1 - De Rosa, G. A1 - De Sio, C. A1 - Di Capua, F. A1 - Di Palma, I. A1 - Díaz García, A. F. A1 - Distefano, C. A1 - Donzaud, C. A1 - Dornic, D. A1 - Dorosti-Hasankiadeh, Q. A1 - Drakopoulou, E. A1 - Drouhin, D. A1 - Drury, L. A1 - Durocher, M. A1 - Eberl, T. A1 - Eichie, S. A1 - van Eijk, D. A1 - El Bojaddaini, I. A1 - El Khayati, N. A1 - Elsaesser, D. A1 - Enzenhöfer, A. A1 - Fassi, F. A1 - Favali, P. A1 - Fermani, P. A1 - Ferrara, G. A1 - Filippidis, C. A1 - Frascadore, G. A1 - Fusco, L. A. A1 - Gal, T. A1 - Galatà, S. A1 - Garufi, F. A1 - Gay, P. A1 - Gebyehu, M. A1 - Giordano, V. A1 - Gizani, N. A1 - Gracia, R. A1 - Graf, K. A1 - Grégoire, T. A1 - Grella, G. A1 - Habel, R. A1 - Hallmann, S. A1 - van Haren, H. A1 - Harissopulos, S. A1 - Heid, T. A1 - Heijboer, A. A1 - Heine, E. A1 - Henry, S. A1 - Hernández-Rey, J. J. A1 - Hevinga, M. A1 - Hofestädt, J. A1 - Hugon, C. M. F. A1 - Illuminati, G. A1 - James, C. W. A1 - Jansweijer, P. A1 - Jongen, M. A1 - de Jong, M. A1 - Kadler, M. A1 - Kalekin, O. A1 - Kappes, A. A1 - Katz, U. F. A1 - Keller, P. A1 - Kieft, G. A1 - Kießling, D. A1 - Koffeman, E. N. A1 - Kooijman, P. A1 - Kouchner, A. A1 - Kulikovskiy, V. A1 - Lahmann, R. A1 - Lamare, P. A1 - Leisos, A. A1 - Leonora, E. A1 - Lindsey Clark, M. A1 - Liolios, A. A1 - Llorenz Alvarez, C. D. A1 - Lo Presti, D. A1 - Löhner, H. A1 - Lonardo, A. A1 - Lotze, M. A1 - Loucatos, S. A1 - Maccioni, E. A1 - Mannheim, K. A1 - Margiotta, A. A1 - Marinelli, A. A1 - Mariş, O. A1 - Markou, C. A1 - Martínez-Mora, J. A. A1 - Martini, A. A1 - Mele, R. A1 - Melis, K. W. A1 - Michael, T. A1 - Migliozzi, P. A1 - Migneco, E. A1 - Mijakowski, P. A1 - Miraglia, A. A1 - Mollo, C. M. A1 - Mongelli, M. A1 - Morganti, M. A1 - Moussa, A. A1 - Musico, P. A1 - Musumeci, M. A1 - Navas, S. A1 - Nicoleau, C. A. A1 - Olcina, I. A1 - Olivetto, C. A1 - Orlando, A. A1 - Papaikonomou, A. A1 - Papaleo, R. A1 - Păvălaş, G. E. A1 - Peek, H. A1 - Pellegrino, C. A1 - Perrina, C. A1 - Pfutzner, M. A1 - Piattelli, P. A1 - Pikounis, K. A1 - Poma, G. E. A1 - Popa, V. A1 - Pradier, T. A1 - Pratolongo, F. A1 - Pühlhofer, G. A1 - Pulvirenti, S. A1 - Quinn, L. A1 - Racca, C. A1 - Raffaelli, F. A1 - Randazzo, N. A1 - Rapidis, P. A1 - Razis, P. A1 - Real, D. A1 - Resvanis, L. A1 - Reubelt, J. A1 - Riccobene, G. A1 - Rossi, C. A1 - Rovelli, A. A1 - Saldaña, M. A1 - Salvadori, I. A1 - Samtleben, D. F. E. A1 - Sánchez García, A. A1 - Sánchez Losa, A. A1 - Sanguineti, M. A1 - Santangelo, A. A1 - Santonocito, D. A1 - Sapienza, P. A1 - Schimmel, F. A1 - Schmelling, J. A1 - Sciacca, V. A1 - Sedita, M. A1 - Seitz, T. A1 - Sgura, I. A1 - Simeone, F. A1 - Siotis, I. A1 - Sipala, V. A1 - Spisso, B. A1 - Spurio, M. A1 - Stavropoulos, G. A1 - Steijger, J. A1 - Stellacci, S. M. A1 - Stransky, D. A1 - Taiuti, M. A1 - Tayalati, Y. A1 - Tézier, D. A1 - Theraube, S. A1 - Thompson, L. A1 - Timmer, P. A1 - Tönnis, C. A1 - Trasatti, L. A1 - Trovato, A. A1 - Tsirigotis, A. A1 - Tzamarias, S. A1 - Tzamariudaki, E. A1 - Vallage, B. A1 - Van Elewyk, V. A1 - Vermeulen, J. A1 - Vicini, P. A1 - Viola, S. A1 - Vivolo, D. A1 - Volkert, M. A1 - Voulgaris, G. A1 - Wiggers, L. A1 - Wilms, J. A1 - de Wolf, E. A1 - Zachariadou, K. A1 - Zornoza, J. D. A1 - Zúñiga, J. T1 - Letter of intent for KM3NeT 2.0 JF - Journal of Physics G-Nuclear and Particle Physics N2 - The main objectives of the KM3NeT Collaboration are (i) the discovery and subsequent observation of high-energy neutrino sources in the Universe and (ii) the determination of the mass hierarchy of neutrinos. These objectives are strongly motivated by two recent important discoveries, namely: (1) the high-energy astrophysical neutrino signal reported by IceCube and (2) the sizable contribution of electron neutrinos to the third neutrino mass eigenstate as reported by Daya Bay, Reno and others. To meet these objectives, the KM3NeT Collaboration plans to build a new Research Infrastructure consisting of a network of deep-sea neutrino telescopes in the Mediterranean Sea. A phased and distributed implementation is pursued which maximises the access to regional funds, the availability of human resources and the synergistic opportunities for the Earth and sea sciences community. Three suitable deep-sea sites are selected, namely off-shore Toulon (France), Capo Passero (Sicily, Italy) and Pylos (Peloponnese, Greece). The infrastructure will consist of three so-called building blocks. A building block comprises 115 strings, each string comprises 18 optical modules and each optical module comprises 31 photo-multiplier tubes. Each building block thus constitutes a three-dimensional array of photo sensors that can be used to detect the Cherenkov light produced by relativistic particles emerging from neutrino interactions. Two building blocks will be sparsely configured to fully explore the IceCube signal with similar instrumented volume, different methodology, improved resolution and KW - neutrino astronomy KW - eutrino physics KW - deep sea neutrino telescope KW - neutrino mass hierarchy Y1 - 2016 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-188050 VL - 43 IS - 8 ER - TY - JOUR A1 - Adrián-Martínez, S. A1 - Albert, A. A1 - André, M. A1 - Anton, G. A1 - Ardid, M. A1 - Aubert, J.-J. A1 - Avgitas, T. A1 - Baret, B. A1 - Barrios-Martí, J. A1 - Basa, S. A1 - Bertin, V. A1 - Biagi, S. A1 - Bormuth, R. A1 - Bou-Cabo, M. A1 - Bouwhuis, M.C. A1 - Bruijn, R. A1 - Brunner, J. A1 - Busto, J. A1 - Capone, A. A1 - Caramete, L. A1 - Carr, J. A1 - Celli, S. A1 - Chiarusi, T. A1 - Circella, M. A1 - Coleiro, A. A1 - Coniglione, R. A1 - Costantini, H. A1 - Coyle, P. A1 - Creusot, A. A1 - Deschamps, A. A1 - De Bonis, G. A1 - Distefano, C. A1 - Donzaud, C. A1 - Dornic, D. A1 - Drouhin, D. A1 - Eberl, T. A1 - El Bojaddaini, I. A1 - Elsässer, D. A1 - Enzenhöfer, A. A1 - Fehn, K. A1 - Felis, I. A1 - Fusco, L.A. A1 - Galatà, S. A1 - Gay, P. A1 - Geißelsöder, S. A1 - Geyer, K. A1 - Giordano, V. A1 - Gleixner, A. A1 - Glotin, H. A1 - Gracia-Ruiz, R. A1 - Graf, K. A1 - Hallmann, S. A1 - van Haren, H. A1 - Heijboer, A.J. A1 - Hello, Y. A1 - Hernández-Rey, J.-J. A1 - Hößl, J. A1 - Hofestädt, J. A1 - Hugon, C. A1 - Illuminati, G. A1 - James, C.W. A1 - de Jong, M. A1 - Kadler, M. A1 - Kalekin, O. A1 - Katz, U. A1 - Kießling, D. A1 - Kouchner, A. A1 - Kreter, M. A1 - Kreykenbohm, I. A1 - Kulikovskiy, V. A1 - Lachaud, C. A1 - Lahmann, R. A1 - Lefèvre, D. A1 - Leonora, E. A1 - Loucatos, S. A1 - Marcelin, M. A1 - Margiotta, A. A1 - Marinelli, A. A1 - Martínez-Mora, J.A. A1 - Mathieu, A. A1 - Michael, T. A1 - Migliozzi, P. A1 - Moussa, A. A1 - Mueller, C. A1 - Nezri, E. A1 - Păvălaș, G.E. A1 - Pellegrino, C. A1 - Perrina, C. A1 - Piattelli, P. A1 - Popa, V. A1 - Pradier, T. A1 - Racca, C. A1 - Riccobene, G. A1 - Roensch, K. A1 - Saldaña, M. A1 - Samtleben, D.F.E. A1 - Sanguineti, M. A1 - Sapienza, P. A1 - Schnabel, J. A1 - Schüssler, F. A1 - Seitz, T. A1 - Sieger, C. A1 - Spurio, M. A1 - Stolarczyk, Th. A1 - Sánchez-Losa, A. A1 - Taiuti, M. A1 - Trovato, A. A1 - Tselengidou, M. A1 - Turpin, D. A1 - Tönnis, C. A1 - Vallage, B. A1 - Vallée, C. A1 - Van Elewyck, V. A1 - Vivolo, D. A1 - Wagner, S. A1 - Wilms, J. A1 - Zornoza, J.D. A1 - Zúñiga, J. T1 - A search for Secluded Dark Matter in the Sun with the ANTARES neutrino telescope JF - Journal of Cosmology and Astroparticle Physics N2 - A search for Secluded Dark Matter annihilation in the Sun using 2007-2012 data of the ANTARES neutrino telescope is presented. Three different cases are considered: a) detection of dimuons that result from the decay of the mediator, or neutrino detection from: b) mediator that decays into a dimuon and, in turn, into neutrinos, and c) mediator that decays directly into neutrinos. As no significant excess over background is observed, constraints are derived on the dark matter mass and the lifetime of the mediator. KW - dark matter experiments KW - neutrino detectors KW - dark matter detectors KW - neutrino astronomy Y1 - 2016 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-189035 VL - 2016 IS - 5 ER - TY - JOUR A1 - Adrián-Martínez, S. A1 - Albert, A. A1 - André, M. A1 - Anton, G. A1 - Ardid, M. A1 - Aubert, J.-J. A1 - Avgitas, T. A1 - Baret, B. A1 - Barrios-Martí, J. A1 - Basa, S. A1 - Bertin, V. A1 - Biagi, S. A1 - Bormuth, R. A1 - Bouwhuis, M.C. A1 - Bruijn, R. A1 - Brunner, J. A1 - Busto, J. A1 - Capone, A. A1 - Caramete, L. A1 - Carr, J. A1 - Celli, S. A1 - Chiarusi, T. A1 - Circella, M. A1 - Coleiro, A. A1 - Coniglione, R. A1 - Costantini, H. A1 - Coyle, P. A1 - Creusot, A. A1 - Deschamps, A. A1 - De Bonis, G. A1 - Distefano, C. A1 - Donzaud, C. A1 - Dornic, D. A1 - Drouhin, D. A1 - Eberl, T. A1 - El Bojaddaini, I. A1 - Elsässer, D. A1 - Enzenhöfer, A. A1 - Fehn, K. A1 - Felis, I. A1 - Fusco, L.A. A1 - Galatà, S. A1 - Gay, P. A1 - Geißelsöder, S. A1 - Geyer, K. A1 - Giordano, V. A1 - Gleixner, A. A1 - Glotin, H. A1 - Gracia-Ruiz, R. A1 - Graf, K. A1 - Hallmann, S. A1 - van Haren, H. A1 - Heijboer, A.J. A1 - Hello, Y. A1 - Hernández-Rey, J.J. A1 - Hößl, J. A1 - Hofestädt, J. A1 - Hugon, C. A1 - Illuminati, G. A1 - James, C.W. A1 - de Jong, M. A1 - Jongen, M. A1 - Kadler, M. A1 - Kalekin, O. A1 - Katz, U. A1 - Kießling, D. A1 - Kouchner, A. A1 - Kreter, M. A1 - Kreykenbohm, I. A1 - Kulikovskiy, V. A1 - Lachaud, C. A1 - Lahmann, R. A1 - Lefèvre, D. A1 - Leonora, E. A1 - Loucatos, S. A1 - Marcelin, M. A1 - Margiotta, A. A1 - Marinelli, A. A1 - Martínez-Mora, J.A. A1 - Mathieu, A. A1 - Melis, K. A1 - Michael, T. A1 - Migliozzi, P. A1 - Moussa, A. A1 - Mueller, C. A1 - Nezri, E. A1 - Pavalas, G.E. A1 - Pellegrino, C. A1 - Perrina, C. A1 - Piattelli, P. A1 - Popa, V. A1 - Pradier, T. A1 - Racca, C. A1 - Riccobene, G. A1 - Roensch, K. A1 - Saldaña, M. A1 - Samtleben, D.F.E. A1 - Sánchez-Losa, A. A1 - Sanguineti, M. A1 - Sapienza, P. A1 - Schnabel, J. A1 - Schüssler, F. A1 - Seitz, T. A1 - Sieger, C. A1 - Spurio, M. A1 - Stolarczyk, Th. A1 - Taiuti, M. A1 - Tönnis, C. A1 - Trovato, A. A1 - Tselengidou, M. A1 - Turpin, D. A1 - Vallage, B. A1 - Vallée, C. A1 - Van Elewyck, V. A1 - Vivolo, D. A1 - Wagner, S. A1 - Wilms, J. A1 - Zornoza, J.D. A1 - Zúñiga, J. T1 - Limits on dark matter annihilation in the sun using the ANTARES neutrino telescope JF - Physics Letters B N2 - A search for muon neutrinos originating from dark matter annihilations in the Sun is performed using the data recorded by the ANTARES neutrino telescope from 2007 to 2012. In order to obtain the best possible sensitivities to dark matter signals, an optimisation of the event selection criteria is performed taking into account the background of atmospheric muons, atmospheric neutrinos and the energy spectra of the expected neutrino signals. No significant excess over the background is observed and 90% C.L. upper limits on the neutrino flux, the spin-dependent and spin-independent WIMP-nucleon cross-sections are derived for WIMP masses ranging from 50 GeV to 5 TeV for the annihilation channels WIMP + WIMP→ b\(\overline{b}\), W\(^{+}\)W\(^{−}\) and τ\(^{+}\)τ\(^{−}\). KW - dark matter KW - WIMP KW - neutralino KW - indirect detection KW - neutrino telescope KW - sun Y1 - 2016 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-166642 VL - 759 ER - TY - JOUR A1 - Adrián-Martínez, S. A1 - Albert, A. A1 - André, M. A1 - Anghinolfi, M. A1 - Anton, G. A1 - Ardid, M. A1 - Aubert, J.-J. A1 - Avgitas, T. A1 - Baret, B. A1 - Barrios-Martí, J. A1 - Basa, S. A1 - Bertin, V. A1 - Biagi, S. A1 - Bormuth, R. A1 - Bouwhuis, M.C. A1 - Bruijn, R. A1 - Brunner, J. A1 - Busto, J. A1 - Capone, A. A1 - Caramete, L. A1 - Carr, J. A1 - Celli, S. A1 - Chiarusi, T. A1 - Circella, M. A1 - Coleiro, A. A1 - Coniglione, R. A1 - Constantini, H. A1 - Coyle, P. A1 - Creusot, A. A1 - Deschamps, A. A1 - De Bonis, G. A1 - Distefano, C. A1 - Donzaud, C. A1 - Dornic, D. A1 - Drouhin, D. A1 - Eberl, T. A1 - El Bojaddaini, I. A1 - Elsässer, D. A1 - Enzenhöfer, A. A1 - Fehn, K. A1 - Felis, I. A1 - Fusco, L.A. A1 - Galatà, S. A1 - Gay, P. A1 - Geißelsöder, S. A1 - Geyer, K. A1 - Giordano, V. A1 - Gleixner, A. A1 - Glotin, H. A1 - Gracia-Ruiz, R. A1 - Graf, K. A1 - Hallmann, S. A1 - van Haren, H. A1 - Heijboer, A.J. A1 - Hello, Y. A1 - Hernández-Rey, J.J. A1 - Hößl, J. A1 - Hofestädt, J. A1 - Hugon, C. A1 - Illuminati, G. A1 - James, C.W. A1 - de Jong, M. A1 - Kadler, M. A1 - Kalekin, O. A1 - Katz, U. A1 - Kießling, D. A1 - Kouchner, A. A1 - Kreter, M. A1 - Kreykenbohm, I. A1 - Kulikovskiy, V. A1 - Lachaud, C. A1 - Lahmann, R. A1 - Lefèvre, D. A1 - Leonora, E. A1 - Loucatos, S. A1 - Marcelin, M. A1 - Margiotta, A. A1 - Marinelli, A. A1 - Martínez-Mora, J.A. A1 - Mathieu, A. A1 - Michael, T. A1 - Migliozzi, P. A1 - Moussa, A. A1 - Mueller, C. A1 - Nezri, E. A1 - Pavalas, G.E. A1 - Pellegrino, C. A1 - Perrina, C. A1 - Piattelli, P. A1 - Popa, V. A1 - Pradier, T. A1 - Racca, C. A1 - Riccobene, G. A1 - Roensch, K. A1 - Saldaña, M. A1 - Samtleben, D.F.E. A1 - Sánchez-Losa, A. A1 - Sanguineti, M. A1 - Sapienza, P. A1 - Schnabel, J. A1 - Schüssler, F. A1 - Seitz, T. A1 - Sieger, C. A1 - Spurio, M. A1 - Stolarczyk, Th. A1 - Taiuti, M. A1 - Trovato, A. A1 - Tselengidou, M. A1 - Turpin, D. A1 - Tönnis, C. A1 - Vallage, B. A1 - Vallée, C. A1 - Van Elewyck, V. A1 - Visser, E. A1 - Vivolo, D. A1 - Wagner, S. A1 - Wilms, J. A1 - Zornoza, J.D. A1 - Zúñiga, J. T1 - Constraints on the neutrino emission from the Galactic Ridge with the ANTARES telescope JF - Physics Letters B N2 - A highly significant excess of high-energy astrophysical neutrinos has been reported by the IceCube Collaboration. Some features of the energy and declination distributions of IceCube events hint at a North/South asymmetry of the neutrino flux. This could be due to the presence of the bulk of our Galaxy in the Southern hemisphere. The ANTARES neutrino telescope, located in the Mediterranean Sea, has been taking data since 2007. It offers the best sensitivity to muon neutrinos produced by galactic cosmic ray interactions in this region of the sky. In this letter a search for an extended neutrino flux from the Galactic Ridge region is presented. Different models of neutrino production by cosmic ray propagation are tested. No excess of events is observed and upper limits for different neutrino flux spectral indices Γ are set. For Γ=2.4 the 90% confidence level flux upper limit at 100 TeV for one neutrino flavour corresponds to Φ\(^{1f}_{0}\) (100 TeV) = 2.0 · 10\(^{−17}\) GeV\(^{−1}\) cm\(^{−2}\)s\(^{−1}\)sr\(^{−1}\). Under this assumption, at most two events of the IceCube cosmic candidates can originate from the Galactic Ridge. A simple power-law extrapolation of the Fermi-LAT flux to account for IceCube High Energy Starting Events is excluded at 90% confidence level. KW - neutrino emission KW - Galactic Ridge KW - ANTARES telescope Y1 - 2016 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-166608 VL - 760 ER - TY - JOUR A1 - Albert, A. A1 - André, M. A1 - Anghinolfi, M. A1 - Anton, G. A1 - Ardid, M. A1 - Aubert, J.-J. A1 - Aublin, J. A1 - Avgitas, T. A1 - Baret, B. A1 - Barrios-Martít, J. A1 - Basa, S. A1 - Belhorma, B. A1 - Bertin, V. A1 - Biagi, S. A1 - Bormuth, R. A1 - Boumaaza, J A1 - Bourret, S. A1 - Bouwhuis, M. C. A1 - Brânzas, H. A1 - Bruijn, R. A1 - Brunner, J. A1 - Busto, J. A1 - Capone, A. A1 - Caramete, L. A1 - Carr, J. A1 - Celli, S. A1 - Chabab, M. A1 - Cherkaoui El Moursli, R. A1 - Chiarusi, T. A1 - Circella, M. A1 - Coelho, J. A. B. A1 - Coleiro, A. A1 - Colomer, M A1 - Coniglione, R. A1 - Costantini, H. A1 - Coyle, P. A1 - Creusot, A. A1 - Díaz, A. F. A1 - Deschamps, A. A1 - Distefano, C. A1 - Di Palma, I. A1 - Domi, A. A1 - Donzaud, C. A1 - Dornic, D. A1 - Drouhin, D. A1 - Eberl, T. A1 - El Bojaddaini, I. A1 - El Khayati, N. A1 - Elsässer, D. A1 - Enzenhöfer, A. A1 - Ettahiri, A. A1 - Fassi, F. A1 - Felis, I. A1 - Fermani, P. A1 - Ferrara, G. A1 - Fusco, L. A. A1 - Gay, P. A1 - Glotin, H. A1 - Grégoire, T. A1 - Gracia Ruiz, R. A1 - Graf, K. A1 - Hallmann, S. A1 - van Haren, H. A1 - Heijboer, A. J. A1 - Hello, Y. A1 - Hernández-Rey, J. J. A1 - Hößl, J. A1 - Hofestädt, J. A1 - Illuminati, G. A1 - de Jong, M. A1 - Jongen, M. A1 - Kadler, M. A1 - Kalekin, O. A1 - Katz, U. A1 - Khan-Chowdhury, N. R. A1 - Kouchner, A. A1 - Kreter, M. A1 - Kreykenbohm, I. A1 - Kulikovskiy, V. A1 - Lachaud, C. A1 - Lahmann, R. A1 - Lefèvre, D. A1 - Leonora, E. A1 - Levi, G. A1 - Lotze, M. A1 - Loucatos, S. A1 - Marcelin, M. A1 - Margiotta, A. A1 - Marinelli, A. A1 - Martínez-Mora, J. A. A1 - Mele, R. A1 - Melis, K. A1 - Migliozzi, P. A1 - Moussa, A. A1 - Navas, S. A1 - Nezri, E. A1 - Nuñez, A. A1 - Organokov, M. A1 - Pavalas, G. E. A1 - Pellegrino, C. A1 - Piattelli, P. A1 - Popa, V. A1 - Pradier, T. A1 - Quinn, L. A1 - Racca, C. A1 - Randazzo, N. A1 - Riccobene, G. A1 - Sánchez-Losa, A. A1 - Saldaña, M. A1 - Salvadori, I. A1 - Samtleben, D. F. E. A1 - Sanguineti, M. A1 - Sapienza, P. A1 - Schüssler, F. A1 - Spurio, M. A1 - Stolarczyk, Th. A1 - Taiuti, M. A1 - Tayalati, Y. A1 - Trovato, A. A1 - Vallage, B. A1 - Van Elewyck, V. A1 - Versari, F. A1 - Vivolo, D. A1 - Wilms, J. A1 - Zaborov, D. A1 - Zornoza, J. D. A1 - Zúñiga, J. T1 - The cosmic ray shadow of the Moon observed with the ANTARES neutrino telescope JF - European Physical Journal C N2 - One of the main objectives of the ANTARES telescope is the search for point- like neutrino sources. Both the pointing accuracy and the angular resolution of the detector are important in this context and a reliableway to evaluate this performance is needed. In order to measure the pointing accuracy of the detector, one possibility is to study the shadow of the Moon, i. e. the deficit of the atmospheric muon flux from the direction of the Moon induced by the absorption of cosmic rays. Analysing the data taken between 2007 and 2016, theMoon shadow is observed with 3.5s statistical significance. The detector angular resolution for downwardgoing muons is 0.73. +/- 0.14.. The resulting pointing performance is consistent with the expectations. An independent check of the telescope pointing accuracy is realised with the data collected by a shower array detector onboard of a ship temporarily moving around the ANTARES location. KW - Atmospheric muons Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-227802 VL - 78 ER - TY - JOUR A1 - Andratschke, N. A1 - Alheid, H. A1 - Allgäuer, M. A1 - Becker, G. A1 - Blanck, O. A1 - Boda-Heggemann, J. A1 - Brunner, T. A1 - Duma, M. A1 - Gerum, S. A1 - Guckenberger, M. A1 - Hildebrandt, G. A1 - Klement, R. J. A1 - Lewitzki, V. A1 - Ostheimer, C. A1 - Papachristofilou, A. A1 - Petersen, C. A1 - Schneider, T. A1 - Semrau, R. A1 - Wachter, S. A1 - Habermehl, D. T1 - The SBRT database initiative of the German Society for Radiation Oncology (DEGRO): patterns of care and outcome analysis of stereotactic body radiotherapy (SBRT) for liver oligometastases in 474 patients with 623 metastases JF - BMC Cancer N2 - Background The intent of this pooled analysis as part of the German society for radiation oncology (DEGRO) stereotactic body radiotherapy (SBRT) initiative was to analyze the patterns of care of SBRT for liver oligometastases and to derive factors influencing treated metastases control and overall survival in a large patient cohort. Methods From 17 German and Swiss centers, data on all patients treated for liver oligometastases with SBRT since its introduction in 1997 has been collected and entered into a centralized database. In addition to patient and tumor characteristics, data on immobilization, image guidance and motion management as well as dose prescription and fractionation has been gathered. Besides dose response and survival statistics, time trends of the aforementioned variables have been investigated. Results In total, 474 patients with 623 liver oligometastases (median 1 lesion/patient; range 1–4) have been collected from 1997 until 2015. Predominant histologies were colorectal cancer (n = 213 pts.; 300 lesions) and breast cancer (n = 57; 81 lesions). All centers employed an SBRT specific setup. Initially, stereotactic coordinates and CT simulation were used for treatment set-up (55%), but eventually were replaced by CBCT guidance (28%) or more recently robotic tracking (17%). High variance in fraction (fx) number (median 1 fx; range 1–13) and dose per fraction (median: 18.5 Gy; range 3–37.5 Gy) was observed, although median BED remained consistently high after an initial learning curve. Median follow-up time was 15 months; median overall survival after SBRT was 24 months. One- and 2-year treated metastases control rate of treated lesions was 77% and 64%; if maximum isocenter biological equivalent dose (BED) was greater than 150 Gy EQD2Gy, it increased to 83% and 70%, respectively. Besides radiation dose colorectal and breast histology and motion management methods were associated with improved treated metastases control. Conclusion After an initial learning curve with regards to total cumulative doses, consistently high biologically effective doses have been employed translating into high local tumor control at 1 and 2 years. The true impact of histology and motion management method on treated metastases control deserve deeper analysis. Overall survival is mainly influenced by histology and metastatic tumor burden. KW - stereotactic body radiotherapy KW - liver oligometastases KW - outcome KW - treated metastases control KW - oligometastases KW - oligo-recurrence KW - sync-oligometastases Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-221116 VL - 18 ER - TY - JOUR A1 - Klement, Rainer J. A1 - Abbasi-Senger, N. A1 - Adebahr, S. A1 - Alheid, H. A1 - Allgaeuer, M. A1 - Becker, G. A1 - Blanck, O. A1 - Boda-Heggemann, J. A1 - Brunner, T. A1 - Duma, M. A1 - Eble, M. J. A1 - Ernst, I. A1 - Gerum, S. A1 - Habermehl, D. A1 - Hass, P. A1 - Henkenberens, C. A1 - Hildebrandt, G. A1 - Imhoff, D. A1 - Kahl, H. A1 - Klass, N. D. A1 - Krempien, R. A1 - Lewitzki, V. A1 - Lohaus, F. A1 - Ostheimer, C. A1 - Papachristofilou, A. A1 - Petersen, C. A1 - Rieber, J. A1 - Schneider, T. A1 - Schrade, E. A1 - Semrau, R. A1 - Wachter, S. A1 - Wittig, A. A1 - Guckenberger, M. A1 - Andratschke, N. T1 - The impact of local control on overall survival after stereotactic body radiotherapy for liver and lung metastases from colorectal cancer: a combined analysis of 388 patients with 500 metastases JF - BMC Cancer N2 - Background The aim of this analysis was to model the effect of local control (LC) on overall survival (OS) in patients treated with stereotactic body radiotherapy (SBRT) for liver or lung metastases from colorectal cancer. Methods The analysis is based on pooled data from two retrospective SBRT databases for pulmonary and hepatic metastases from 27 centers from Germany and Switzerland. Only patients with metastases from colorectal cancer were considered to avoid histology as a confounding factor. An illness-death model was employed to model the relationship between LC and OS. Results Three hundred eighty-eight patients with 500 metastatic lesions (lung n = 209, liver n = 291) were included and analyzed. Median follow-up time for local recurrence assessment was 12.1 months. Ninety-nine patients with 112 lesions experienced local failure. Seventy-one of these patients died after local failure. Median survival time was 27.9 months in all patients and 25.4 months versus 30.6 months in patients with and without local failure after SBRT. The baseline risk of death after local failure exceeds the baseline risk of death without local failure at 10 months indicating better survival with LC. Conclusion In CRC patients with lung or liver metastases, our findings suggest improved long-term OS by achieving metastatic disease control using SBRT in patients with a projected OS estimate of > 12 months. KW - colorectal cancer KW - illness-death model KW - liver metastases KW - lung metastases KW - tumor control probability KW - stereotactic body radiation therapy Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-325877 VL - 19 ER - TY - JOUR A1 - Adrián-Martínez, S. A1 - Albert, A. A1 - André, M. A1 - Anghinolfi, M. A1 - Anton, G. A1 - Ardid, M. A1 - Aubert, J.-J. A1 - Baret, B. A1 - Barrios-Marti, J. A1 - Basa, S. A1 - Bertin, V. A1 - Biagi, S. A1 - Bormuth, R. A1 - Bouwhuis, M.C. A1 - Bruijn, R. A1 - Brunner, J. A1 - Buto, J. A1 - Capone, A. A1 - Caramete, L. A1 - Carr, J. A1 - Chiarusi, T. A1 - Circella, M. A1 - Coniglione, R. A1 - Costantini, H. A1 - Coyle, P. A1 - Creusot, A. A1 - Dekeyser, I. A1 - Deschamps, A. A1 - De Bonis, G. A1 - Distefano, C. T1 - Stacked search for time shifted high energy neutrinos from gamma ray bursts with the ANTARES neutrino telescope JF - European Physical Journal C N2 - A search for high-energy neutrino emission correlated with gamma-ray bursts outside the electromagnetic prompt-emission time window is presented. Using a stacking approach of the time delays between reported gamma-ray burst alerts and spatially coincident muon-neutrino signatures, data from the Antares neutrino telescope recorded between 2007 and 2012 are analysed. One year of public data from the IceCube detector between 2008 and 2009 have been also investigated. The respective timing profiles are scanned for statistically significant accumulations within 40 days of the Gamma Ray Burst, as expected from Lorentz Invariance Violation effects and some astrophysical models. No significant excess over the expected accidental coincidence rate could be found in either of the two data sets. The average strength of the neutrino signal is found to be fainter than one detectable neutrino signal per hundred gamma-ray bursts in the Antares data at 90% confidence level. KW - Search window KW - Neutrino data KW - Neutrino telescope KW - Neutrino emission KW - Accidental coincidence KW - Gamma-ray bursts Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-181251 VL - 77 IS - 1 ER -