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Showing papers by "S. R. Mishra published in 2013"


Journal ArticleDOI
P. Adamson1, I. Anghel2, I. Anghel3, C. Backhouse4, G.D. Barr4, M. Bishai5, Andrew Blake6, G. J. Bock1, D. Bogert1, S. V. Cao7, C. M. Castromonte8, S. Childress1, Joao A B Coelho9, Joao A B Coelho10, L. Corwin11, Daniel P Cronin-Hennessy, J. K. De Jong4, A. V. Devan12, N. E. Devenish13, M. V. Diwan5, Carlos Escobar9, J. J. Evans, E. Falk13, G. J. Feldman14, M. V. Frohne15, H. R. Gallagher10, R. A. Gomes8, Maury Goodman2, P. Gouffon16, N. Graf17, R. Gran, K. Grzelak18, Alec Habig, S. R. Hahn1, J. Hartnell13, R. Hatcher1, A. Himmel19, A. Holin20, J. Hylen1, G. M. Irwin21, Z. Isvan22, Z. Isvan5, C. James1, D. A. Jensen1, T. Kafka10, S. M. S. Kasahara23, G. Koizumi1, M. Kordosky12, A. E. Kreymer1, Karol Lang7, P. J. Litchfield, P. Lucas, W. A. Mann, Marvin L Marshak, M. Mathis, N. Mayer, A. M. McGowan, M. M. Medeiros, R. Mehdiyev, J. R. Meier, M. D. Messier, D. G. Michael, W. H. Miller, S. R. Mishra, S. Moed Sher, C. D. Moore, L. Mualem, J. A. Musser, D. Naples, J. K. Nelson, Harvey B Newman, R. J. Nichol, J. A. Nowak, J. O'Connor, W. P. Oliver, M. Orchanian, R. B. Pahlka, J. M. Paley, R. B. Patterson, Gregory J Pawloski, S. Phan-Budd, R. K. Plunkett, X. Qiu, A. Radovic, B. Rebel, C. Rosenfeld, H. A. Rubin, M. C. Sanchez, J. Schneps, A. Schreckenberger, P. Schreiner, R. Sharma, A. Sousa, N. Tagg, R. L. Talaga, Juergen Thomas, M. A. Thomson, G. Tinti, S. C. Tognini, R. Toner, D. Torretta, G. Tzanakos, J. Urheim, P. Vahle, B. Viren, A. C. Weber, R. C. Webb, Christopher G. White, L. Whitehead, L. H. Whitehead, Stanley G. Wojcicki, R. Zwaska 
TL;DR: Measurements of oscillation parameters from ν (μ) and ν(μ) disappearance using beam and atmospheric data from MINOS are reported, with minimal change to the neutrino parameters.
Abstract: We report measurements of oscillation parameters from ν_μ and ν_μ disappearance using beam and atmospheric data from MINOS. The data comprise exposures of 10.71×10^(20) protons on target in the ν_μ-dominated beam, 3.36×10^(20) protons on target in the ν_μ-enhanced beam, and 37.88 kton yr of atmospheric neutrinos. Assuming identical ν and ν oscillation parameters, we measure |Δm^2|=(2.41_(-0.10)^(+0.09))×10^(-3) eV^2 and sin^⁡2(2θ)=0.950_(-0.036)^(+0.035). Allowing independent ν and ν oscillations, we measure antineutrino parameters of |Δm^2|=(2.50_(-0.25)^(+0.23))×10^(-3) eV^2 and sin^⁡2(2θ)=0.97_(-0.08)^(+0.03), with minimal change to the neutrino parameters.

314 citations


ReportDOI
D. Adey, Sanjib Kumar Agarwalla, Charles M. Ankenbrandt, R. Asfandiyarov, J. J. Back, Gareth J. Barker, Eric Baussan, R. Bayes, S. Bhadra, V. Blackmore, A. Blondel, S. A. Bogacz, C. N. Booth, S. B. Boyd, A. Bravar, S. J. Brice, A. D. Bross, Franck Cadoux, H. Cease, A. Cervera, J.H. Cobb, David Colling, P. Coloma, L. Coney, A. Dobbs, J. Dobson, Andrea Donini, P. J. Dornan, Marcos Dracos, F. Dufour, Rob Edgecock, John Evans, M. Geelhoed, M. George, T.K. Ghosh, J.J. Gómez-Cadenas, A. de Gouvea, A. Haesler, Gordon H. Hanson, P. F. Harrison, M. Hartz, Porfidio Hernández, J. A. Hernando Morata, Paul Hodgson, Patrick Huber, A. Izmaylov, Y. Karadzhov, T. Kobilarcik, Joachim Kopp1, L. L. Kormos, A. Korzenev, Y. Kuno, A. Kurup, P. Kyberd, J.-B. Lagrange, A. Laing, A. Liud, J. M. Link, Kenneth Long, Kendall Mahn, C. Mariani, C. Martin, J.P. Martin, N. McCauley, K. T. McDonald, O. Mena, S. R. Mishra, N.V. Mokhov, Jorge G. Morfin, Y. Mori, W. J. Murray, David Neuffer, R. J. Nichol, Etam Noah, M.A. Palmer, Stephen J. Parke, Silvia Pascoli, Jaroslaw Pasternak, Milorad Popovic, P. N. Ratoff, M. Ravonel, M. A.M. Rayner, S. Ricciardi, C. Rogers, P. Rubinov, E. M. Santos, A. Sato, Tanaji Sen, E. Scantamburlo, J. K. Sedgbeer, David R. Smith, Patrick Smith, Jan T. Sobczyk, L. Soby, F. J. P. Soler, S. Söldner-Rembold, M. Sorel, Pavel Snopok, P. Stamoulis, Luca Stanco, Sergei Striganov, H.A. Tanaka, I. Taylor, C. Touramanis, C. Tunnell, Y. Uchida, N. Vassilopoulos, M. O. Wascko, A. C. Weber, M. J. Wilking, Elena Wildner, Walter Winter, U. K. Yang 
TL;DR: The nuSTORM facility as discussed by the authors was designed to deliver beams of neutrinos and their anti-particles from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum acceptance of 10%.
Abstract: The nuSTORM facility has been designed to deliver beams of electron neutrinos and muon neutrinos (and their anti-particles) from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum acceptance of 10%. The facility is unique in that it will: 1. Allow searches for sterile neutrinos of exquisite sensitivity to be carried out; 2. Serve future long- and short-baseline neutrino-oscillation programs by providing definitive measurements of electron neutrino and muon neutrino scattering cross sections off nuclei with percent-level precision; and 3. Constitutes the crucial first step in the development of muon accelerators as a powerful new technique for particle physics. The document describes the facility in detail and demonstrates its physics capabilities. This document was submitted to the Fermilab Physics Advisory Committee in consideration for Stage I approval.

65 citations


Posted Content
TL;DR: The existence of neutrino neutrinos has been investigated in this article, where the LSND antineutrino appearance signal has been shown to be consistent with neutrini oscillations at a mass of roughly 1$ eV/c$^2.
Abstract: There exists a need to address and resolve the growing evidence for short-baseline neutrino oscillations and the possible existence of sterile neutrinos. Such non-standard particles require a mass of $\sim 1$ eV/c$^2$, far above the mass scale associated with active neutrinos, and were first invoked to explain the LSND $\bar u_\mu \rightarrow \bar u_e$ appearance signal. More recently, the MiniBooNE experiment has reported a $2.8 \sigma$ excess of events in antineutrino mode consistent with neutrino oscillations and with the LSND antineutrino appearance signal. MiniBooNE also observed a $3.4 \sigma$ excess of events in their neutrino mode data. Lower than expected neutrino-induced event rates using calibrated radioactive sources and nuclear reactors can also be explained by the existence of sterile neutrinos. Fits to the world's neutrino and antineutrino data are consistent with sterile neutrinos at this $\sim 1$ eV/c$^2$ mass scale, although there is some tension between measurements from disappearance and appearance experiments. In addition to resolving this potential major extension of the Standard Model, the existence of sterile neutrinos will impact design and planning for all future neutrino experiments. It should be an extremely high priority to conclusively establish if such unexpected light sterile neutrinos exist. The Spallation Neutron Source (SNS) at Oak Ridge National Laboratory, built to usher in a new era in neutron research, provides a unique opportunity for US science to perform a definitive world-class search for sterile neutrinos.

31 citations


Posted Content
D. Adey, Sanjib Kumar Agarwalla, Charles M. Ankenbrandt, R. Asfandiyarov, J. J. Back, Gareth J. Barker, Eric Baussan, R. Bayes, S. Bhadra, V. Blackmore, A. Blondel, S. A. Bogacz, C. N. Booth, S. B. Boyd, A. Bravar, S. J. Brice, A. D. Bross, Franck Cadoux, H. Cease, A. Cervera, J.H. Cobb, David Colling, L. Coney, A. Dobbs, J. Dobson, Andrea Donini, P. J. Dornan, Marcos Dracos, F. Dufour, Rob Edgecock, John Evans, M. George, T.K. Ghosh, A. deGouvea, J.J. Gómez-Cadenas, A. Haesler, G. G. Hanson, M. Geelhoed, P. F. Harrison, M. Hartz, Porfidio Hernández, J. A. Hernando-Morata, P. Hodgson, Patrick Huber, A. Izmaylov, Y. Karadhzov, T. Kobilarcik, Joachim Kopp1, L. L. Kormos, A. Korzenev, A. Kurup, Y. Kuno, P. Kyberd, J. P. Lagrange, A. Laing, J. M. Link, Ao Liu, Kenneth Long, N. McCauley, K. T. McDonald, Kendall Mahn, Christopher Blake Martin, J.P. Martin, O. Mena, S. R. Mishra, N.V. Mokhov, Jorge G. Morfin, Y. Mori, W. J. Murray, David Neuffer, R. J. Nichol, Etam Noah, M.A. Palmer, Stephen J. Parke, Silvia Pascoli, Jaroslaw Pasternak, Milorad Popovic, P. N. Ratoff, M. Ravonel, M. A.M. Rayner, S. Ricciardi, C. Rogers, P. Rubinov, E. M. Santos, A. Sato, E. Scantamburlo, J. K. Sedgbeer, David R. Smith, Patrick Smith, Jan T. Sobczyk, S. Söldner-Rembold, F. J. P. Soler, M. Sorel, A. Stahl, Luca Stanco, P. Stamoulis, Sergei Striganov, H.A. Tanaka, I. Taylor, C. Touramanis, C. D. Tunnel, Y. Uchida, N. Vassilopoulos, M. O. Wascko, A. C. Weber, Elena Wildner, M. J. Wilking, Walter Winter, U. K. Yang 
TL;DR: The nuSTORM facility as mentioned in this paper is designed to deliver beams of electron and muon neutrinos from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum spread of 10%.
Abstract: The nuSTORM facility has been designed to deliver beams of electron and muon neutrinos from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum spread of 10%. The facility is unique in that it will: serve the future long- and short-baseline neutrino-oscillation programmes by providing definitive measurements of electron-neutrino- and muon-neutrino-nucleus cross sections with percent-level precision; allow searches for sterile neutrinos of exquisite sensitivity to be carried out; and constitute the essential first step in the incremental development of muon accelerators as a powerful new technique for particle physics. Of the world's proton-accelerator laboratories, only CERN and FNAL have the infrastructure required to mount nuSTORM. Since no siting decision has yet been taken, the purpose of this Expression of Interest (EoI) is to request the resources required to: investigate in detail how nuSTORM could be implemented at CERN; and develop options for decisive European contributions to the nuSTORM facility and experimental programme wherever the facility is sited. The EoI defines a two-year programme culminating in the delivery of a Technical Design Report.

29 citations