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Featured researches published by A. Dobbs.


Journal of Instrumentation | 2013

The design, construction and performance of the MICE target

C.N. Booth; P. Hodgson; L. Howlett; R. Nicholson; E. Overton; M. Robinson; P.J. Smith; M. Apollonio; G. Barber; A. Dobbs; J. Leaver; Kenneth Long; B. Shepherd; D. Adams; E Capocci; E McCarron; J. Tarrant

The pion-production target that serves the MICE Muon Beam consists of a titanium cylinder that is dipped into the halo of the ISIS proton beam. The design and construction of the MICE target system are described along with the quality-assurance procedures, electromagnetic drive and control systems, the readout electronics, and the data-acquisition system. The performance of the target is presented together with the particle rates delivered to the MICE Muon Beam. Finally, the beam loss in ISIS generated by the operation of the target is evaluated as a function of the particle rate, and the operating parameters of the target are derived.


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.


Journal of Physics: Conference Series | 2014

The Reconstruction Software for the Muon Ionization Cooling Experiment Trackers

A. Dobbs; Kenneth Long; E. Santos; D. Adey; P Hanlet; C. Heidt

The international Muon Ionisation Cooling Experiment (MICE) is designed to demonstrate the principle of muon ionization cooling, for application to a future Neutrino Factory or Muon Collider. In order to measure the change in emittance, MICE is equipped with a pair of high precision scintillating fibre trackers. The trackers are required to measure a 10% change in emittance to 1% accuracy (giving an overall precision of 0.1%). This paper describes the tracker reconstruction software, as a part of the overall MICE software framework, MAUS. Channel clustering is described, proceeding to the formation of space-points, which are then associated with particle tracks using pattern recognition algorithms. Finally a full custom Kalman track fit is performed, to account for energy loss and multiple scattering. Exemplar results are shown for Monte Carlo data.


Journal of Physics: Conference Series | 2013

The MICE luminosity monitor

A. Dobbs; David Forrest; F. J. P. Soler

The MICE experiment will provide the first measurement of ionisation cooling, a technique suitable for reducing the transverse emittance of a tertiary muon beam in a future neutrino factory accelerator facility. MICE is presently in the final stages of commissioning its beam line. The MICE luminosity monitor has proved an invaluable tool throughout this process, providing independent measurements of particle rate from the MICE target, normalisation for beam line detectors and verification of simulation codes.


Journal of Instrumentation | 2016

The reconstruction software for the MICE scintillating fibre trackers

A. Dobbs; C. Hunt; Kenneth Long; E. Santos; M. A. Uchida; P. Kyberd; C. Heidt; S. Blot; E. Overton

The Muon Ionization Cooling Experiment (MICE) will demonstrate the principle of muon beam phase-space reduction via ionization cooling. Muon beam cooling will be required for the proposed Neutrino Factory or Muon Collider. The phase-space before and after the cooling cell must be measured precisely. This is achieved using two scintillating-fibre trackers, each placed in a solenoidal magnetic field. This paper describes the software reconstruction for the fibre trackers: the GEANT4 based simulation; the implementation of the geometry; digitisation; space-point reconstruction; pattern recognition; and the final track fit based on a Kalman filter. The performance of the software is evaluated by means of Monte Carlo studies and the precision of the final track reconstruction is evaluated.

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Kenneth Long

Imperial College London

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E. Santos

Imperial College London

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P. Kyberd

Brunel University London

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C. Heidt

University of California

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E. Overton

University of Sheffield

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C. Hunt

Imperial College London

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D. Adams

Rutherford Appleton Laboratory

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E Capocci

Rutherford Appleton Laboratory

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