Precision muon reconstruction in Double Chooz

Y. Abe , J.C. dos Anjos , J.C. Barriere (1) , E. Baussan (2) , I. Bekman , M. Bergevin , T.J.C. Bezerra , L. Bezrukov , E. Blucher , C. Buck , J. Busenitz , A. Cabrera (3) , E. Caden , L. Camilleri , R. Carr , M. Cerrada , P.-J. Chang , E. Chauveau , P. Chimenti , A.P. Collin (4) , E. Conover , J.M. Conrad , J.I. Crespo-Anadón , K. Crum , A. Cucoanes (5) , E. Damon , J.V. Dawson (3) , J. Dhooghe , D. Dietrich , Z. Djurcic , M. Dracos (2) , M. Elnimr , A. Etenko , Muriel Fallot (5) , F. von Feilitzsch , J. Felde , S.M. Fernandes , V. Fischer (6) , D. Franco (3) , M. Franke , H. Furuta , I. Gil-Botella , Lydie Giot (5) , M. Göger-Neff , L.F.G. Gonzalez , L. Goodenough , M.C. Goodman , C. Grant , N. Haag , T. Hara , J. Haser , M. Hofmann , G.A. Horton-Smith , A. Hourlier (3) , M. Ishitsuka , J. Jochum , C. Jollet (2) , F. Kaether , L.N. Kalousis , Y. Kamyshkov , D.M. Kaplan , T. Kawasaki , E. Kemp , H. de Kerret (3) , D. Kryn (3) , M. Kuze , T. Lachenmaier , C.E. Lane , T. Lasserre (6, 3) , A. Letourneau (7) , D. Lhuillier (7) , H.P. Lima , M. Lindner , J.M. López-Castaño , J.M. Losecco , B. Lubsandorzhiev , S. Lucht , J. Maeda , C. Mariani , J. Maricic , J. Martino (8) , T. Matsubara , G. Mention (6) , A. Meregaglia (2) , T. Miletic , R. Milincic , A. Minotti (2) , Y. Nagasaka , Y. Nikitenko , P. Novella (3) , L. Oberauer , M. Obolensky (3) , A. Onillon (5) , A. Osborn , C. Palomares , I.M. Pepe , S. Perasso (3) , P. Pfahler , Amanda Porta (5) , G. Pronost (5) , J. Reichenbacher , B. Reinhold , M. Röhling , R. Roncin (3) , S. Roth , B. Rybolt , Y. Sakamoto , R. Santorelli , A.C. Schilithz , S. Schönert , S. Schoppmann , M.H. Shaevitz , R. Sharankova , S. Shimojima , D. Shrestha , V. Sibille (7) , V. Sinev , M. Skorokhvatov , E. Smith , J. Spitz , A. Stahl , I. Stancu , L.F.F. Stokes , M. Strait , A. Stüken , F. Suekane , S. Sukhotin , T. Sumiyoshi , Y. Sun , R. Svoboda , K. Terao , A. Tonazzo (3) , H.H. Trinh Thi , G. Valdiviesso , N. Vassilopoulos (2) , C. Veyssiere (1) , M. Vivier (6) , S. Wagner , N. Walsh , H. Watanabe , C. Wiebusch , L. Winslow , M. Wurm , G. Yang , F. Yermia (5) , V. Zimmer

1 DIS - Département d'Ingénierie des Systèmes (ex SIS)
2 IPHC - Institut Pluridisciplinaire Hubert Curien
3 APC (UMR_7164) - AstroParticule et Cosmologie
4 Max-Planck-Institut
5 SUBATECH - Laboratoire SUBATECH Nantes
6 DPhP - Département de Physique des Particules (ex SPP)
7 DPHN - Département de Physique Nucléaire (ex SPhN)
8 IAS - Institut d'astrophysique spatiale

We describe a muon track reconstruction algorithm for the reactor anti-neutrino experiment Double Chooz. The Double Chooz detector consists of two optically isolated volumes of the liquid scintillator viewed by PMTs, and an Outer Veto above these made of crossed scintillator strips. Muons are reconstructed by their Outer Veto hit positions along with timing information from the other two detector volumes. All muons are fit under the hypothesis that they are through-going and ultrarelativistic. If the energy depositions suggest that the muon may have stopped, the reconstruction fits also for this hypothesis and chooses between the two via the relative goodness-of-fit. In the ideal case of a through-going muon intersecting the center of the detector, the resolution is View the MathML source~40mm in each transverse dimension. High quality muon reconstruction is an important tool for reducing the impact of the cosmogenic isotope background in Double Chooz.

Mots clés: Neutrino detector; Double Chooz; Muon reconstruction

Domaines: Physique des Hautes Energies - Expérience [hep-ex]; Instrumentations et Détecteurs [physics.ins-det]

Y. Abe, J.C. dos Anjos, J.C. Barriere, E. Baussan, I. Bekman, et al.. Precision muon reconstruction in Double Chooz. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2014, 764, pp.330-339. ⟨10.1016/j.nima.2014.07.058⟩. ⟨hal-01076545⟩