Publications [#248759] of Christopher Walter

Papers Published
  1. Abe, K; Abgrall, N; Aihara, H; Ajima, Y; Albert, JB; Allan, D; Amaudruz, P-A; Andreopoulos, C; Andrieu, B; Anerella, MD; Angelsen, C; Aoki, S; Araoka, O; Argyriades, J; Ariga, A; Ariga, T; Assylbekov, S; André, JPAMD; Autiero, D; Badertscher, A; Ballester, O; Barbi, M; Barker, GJ; Baron, P; Barr, G; Bartoszek, L; Batkiewicz, M; Bay, F; Bentham, S; Berardi, V; Berger, BE; Berns, H; Bertram, I; Besnier, M; Beucher, J; Beznosko, D; Bhadra, S; Birney, P; Bishop, D; Blackmore, E; Blaszczyk, FDM et al., The T2K experiment, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, vol. 659 no. 1 (2011), pp. 106-135 [pdf], [doi] .

    Abstract:
    The T2K experiment is a long baseline neutrino oscillation experiment. Its main goal is to measure the last unknown lepton sector mixing angle θ13 by observing νe appearance in a νμ beam. It also aims to make a precision measurement of the known oscillation parameters, Δ232+ and sin22θ23, via νμ disappearance studies. Other goals of the experiment include various neutrino cross-section measurements and sterile neutrino searches. The experiment uses an intense proton beam generated by the J-PARC accelerator in Tokai, Japan, and is composed of a neutrino beamline, a near detector complex (ND280), and a far detector (Super-Kamiokande) located 295 km away from J-PARC. This paper provides a comprehensive review of the instrumentation aspect of the T2K experiment and a summary of the vital information for each subsystem. © 2011 Elsevier B.V. All rights reserved.