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Archive | 2012

nuSTORM - Neutrinos from STORed Muons: Letter of Intent to the Fermilab Physics Advisory Committee

P. Kyberd; J. Pasternak; M. Popovic; L. Coney; David R. Smith; Y. Kuno; Sanjib Kumar Agarwalla; N. Mokhov; S. A. Bogacz; E. Noah; J. M. Link; J. H. Cobb; V. Blackmore; Walter Winter; Atsushi Sato; Patrick Huber; P. Rubinov; C. M. Ankenbrandt; H. Cease; S. Striganov; A. Dobbs; J. Morfin; S. J. Brice; A. Blondel; S. Pascoli; A. Bross; M. O. Wascko; K. R. Long; Joachim Kopp; A. de Gouvea

The idea of using a muon storage ring to produce a high-energy ({approx_equal} 50 GeV) neutrino beam for experiments was first discussed by Koshkarev in 1974. A detailed description of a muon storage ring for neutrino oscillation experiments was first produced by Neuffer in 1980. In his paper, Neuffer studied muon decay rings with E{sub {mu}} of 8, 4.5 and 1.5 GeV. With his 4.5 GeV ring design, he achieved a figure of merit of {approx_equal} 6 x 10{sup 9} useful neutrinos per 3 x 10{sup 13} protons on target. The facility we describe here ({nu}STORM) is essentially the same facility proposed in 1980 and would utilize a 3-4 GeV/c muon storage ring to study eV-scale oscillation physics and, in addition, could add significantly to our understanding of {nu}{sub e} and {nu}{sub {mu}} cross sections. In particular the facility can: (1) address the large {Delta}m{sup 2} oscillation regime and make a major contribution to the study of sterile neutrinos, (2) make precision {nu}{sub e} and {bar {nu}}{sub e} cross-section measurements, (3) provide a technology ({mu} decay ring) test demonstration and {mu} beam diagnostics test bed, and (4) provide a precisely understood {nu} beam for detector studies. The facility is the simplest implementation of the Neutrino Factory concept. In our case, 60 GeV/c protons are used to produce pions off a conventional solid target. The pions are collected with a focusing device (horn or lithium lens) and are then transported to, and injected into, a storage ring. The pions that decay in the first straight of the ring can yield a muon that is captured in the ring. The circulating muons then subsequently decay into electrons and neutrinos. We are starting with a storage ring design that is optimized for 3.8 GeV/c muon momentum. This momentum was selected to maximize the physics reach for both oscillation and the cross section physics. See Fig. 1 for a schematic of the facility.


arXiv: Instrumentation and Detectors | 2014

Proposal for SPS beam time for the baby MIND and TASD neutrino detector prototypes

R. Asfandiyarov; I. Karpikov; M. Bogomilov; N. Yershov; A. Rubbia; E. Noah; P. Soler; M. Khabibulin; G. Vankova-Kirilova; F. Cadoux; Y. Musienko; R. Matev; O. Mineev; M. Nessi; A. Khotyantsev; A. Izmaylov; A. Shaykiev; A. Cervera; A. Blondel; R. Tsenov; A. Bross; Y. Kudenko; Y. Karadzhov; A. Kopylov; R. Bayes


arXiv: Instrumentation and Detectors | 2016

TITUS: the Tokai Intermediate Tank for the Unoscillated Spectrum

C. Andreopoulos; F.C.T. Barbato; G. J. Barker; G. Barr; P. Beltrame; Berardi; T. Berry; A. Blondel; S. Boyd; A. Bravar; F. Cafagna; S. Cartwright; M. G. Catanesi; C. Checchia; A. Cole; G. Collazuol; G. Cowan; T. Davenne; T. Dealtry; C. Densham; G. Rosa; Fd Lodovico; E.L. Drakopoulou; P. Dunne; A.J. Finch; M. Fitton; D. R. Hadley; K. Hayrapetyan; R. A. Intonti; P. Jonsson

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A. Dobbs

Imperial College London

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C. Andreopoulos

Rutherford Appleton Laboratory

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C. Densham

Rutherford Appleton Laboratory

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G. Barr

University of Oxford

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