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
T1  - Search for dark matter in events with heavy quarks and missing transverse momentum in pp collisions with the ATLAS detector
JF  - European Physical Journal C: Particles and Fields
N2  - This article reports on a search for dark matter pair production in association with bottom or top quarks in 20.3 fb\(^{−1}\) of pp collisions collected at \(\sqrt {s}\) = 8 TeV by the ATLAS detector at the LHC. Events with large missing transverse momentum are selected when produced in association with high-momentum jets of which one or more are identified as jets containing b-quarks. Final states with top quarks are selected by requiring a high jet multiplicity and in some cases a single lepton. The data are found to be consistent with the Standard Model expectations and limits are set on the mass scale of effective field theories that describe scalar and tensor interactions between dark matter and Standard Model particles. Limits on the dark-matter–nucleon cross-section for spin-independent and spin-dependent interactions are also provided. These limits are particularly strong for low-mass dark matter. Using a simplified model, constraints are set on the mass of dark matter and of a coloured mediator suitable to explain a possible signal of annihilating dark matter.
KW  - dark matter
KW  - proton-proton collision
KW  - ATLAS detector
Y1  - 2015
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-150089
VL  - 75
IS  - 2
ER  -