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NuMI

About: NuMI is a research topic. Over the lifetime, 528 publications have been published within this topic receiving 7470 citations. The topic is also known as: Neutrinos at the Main Injector.


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Journal ArticleDOI
P. Adamson1, D. J. Auty2, D. S. Ayres3, C. Backhouse4, G.D. Barr4, M. Betancourt5, M. Bishai6, Andrew Blake7, G. J. Bock1, D. J. Boehnlein1, D. Bogert1, S. V. Cao8, S. Cavanaugh9, D. Cherdack10, S. Childress1, Joao A B Coelho11, L. Corwin12, D. Cronin-Hennessy, I. Z. Danko13, J. K. de Jong4, N. E. Devenish2, M. V. Diwan6, M. Dorman14, Carlos Escobar11, J. J. Evans, E. Falk2, G. J. Feldman9, M. V. Frohne15, H. R. Gallagher10, R. A. Gomes16, Maury Goodman3, P. Gouffon17, N. Graf18, R. Gran, K. Grzelak19, Alec Habig, J. Hartnell2, R. Hatcher1, A. Himmel20, A. Holin14, Xian-Rong Huang3, J. Hylen1, G. M. Irwin21, Z. Isvan13, D. E. Jaffe6, C. James1, D. A. Jensen1, T. Kafka10, S. M. S. Kasahara, G. Koizumi, Sacha E Kopp, M. Kordosky, A. E. Kreymer, Karol Lang, G. Lefeuvre, P. J. Litchfield, L. Loiacono, P. Lucas, W. A. Mann, Marvin L Marshak, M. Mathis, N. Mayer, A. M. McGowan, R. Mehdiyev, J. R. Meier, M. D. Messier, D. G. Michael, W. H. Miller, S. R. Mishra, John C. Mitchell, C. D. Moore, L. Mualem, S. L. Mufson, J. A. Musser, D. Naples, J. K. Nelson, Harvey B Newman, R. J. Nichol, J. A. Nowak, Juan Pedro Ochoa-Ricoux, W. P. Oliver, M. Orchanian, J. M. Paley, R. B. Patterson, Gregory J Pawloski, G. F. Pearce, S. Phan-Budd, R. K. Plunkett, X. Qiu, J. Ratchford, B. Rebel, C. Rosenfeld, H. A. Rubin, M. C. Sanchez, J. Schneps, A. Schreckenberger, P. Schreiner, P. Shanahan, Rohit Sharma, A. Sousa, N. Tagg, R. L. Talaga, J. C. Thomas, M. A. Thomson, R. Toner, D. Torretta, G. Tzanakos, J. Urheim, P. Vahle, B. Viren, J. Walding, A. C. Weber, R. C. Webb, C. White, L. H. Whitehead, Stanley G. Wojcicki, T. Yang, R. Zwaska1 
TL;DR: The results of a search for ν(e) appearance in a ν (μ) beam in the MINOS long-baseline neutrino experiment find that 2 sin(2) (θ(23))sin(2)(2θ (13))<0.12 at 90% confidence level for δ = 0 and the normal (inverted) neutrinos mass hierarchy.
Abstract: We report the results of a search for ν(e) appearance in a ν(μ) beam in the MINOS long-baseline neutrino experiment. With an improved analysis and an increased exposure of 8.2 × 10(20) protons on the NuMI target at Fermilab, we find that 2 sin(2) (θ(23))sin(2)(2θ(13))<0.12(0.20) at 90% confidence level for δ = 0 and the normal (inverted) neutrino mass hierarchy, with a best-fit of 2sin(2) (θ(23))sin(2)(2θ(13)) = 0.041(-0.031)(+0.047) (0.079(-0.053) (+0.071)). The θ(13) = 0 hypothesis is disfavored by the MINOS data at the 89% confidence level.

730 citations

Journal ArticleDOI
P. Adamson1, C. Andreopoulos2, K. E. Arms3, R. Armstrong4  +174 moreInstitutions (29)
TL;DR: The data disfavor two alternative explanations for the disappearance of neutrinos in flight: namely, neutrino decays into lighter particles and quantum decoherence of neutRinos, at the 3.7 and 5.7 standard-deviation levels, respectively.
Abstract: This Letter reports new results from the MINOS experiment based on a two-year exposure to muon neutrinos from the Fermilab NuMI beam. Our data are consistent with quantum-mechanical oscillations of neutrino flavor with mass splitting |Δm^2|=(2.43±0.13)×10^-3 eV^2 (68% C.L.) and mixing angle sin^2(2θ)>0.90 (90% C.L.). Our data disfavor two alternative explanations for the disappearance of neutrinos in flight: namely, neutrino decays into lighter particles and quantum decoherence of neutrinos, at the 3.7 and 5.7 standard-deviation levels, respectively.

340 citations

Posted Content
TL;DR: A 30 kiloton tracking calorimeter with liquid scintillator filled PVC extrusion modules is proposed in the NOvA proposal as mentioned in this paper, with alternating horizontal and vertical rectangular cells.
Abstract: This is an updated version of the NOvA proposal The detector is a 30 kiloton tracking calorimeter, 157 m by 157 m by 132 m long, with alternating horizontal and vertical rectangular cells of liquid scintillator contained in PVC extrusion modules Light from each 157 m long cell of liquid scintillator filled PVC is collected by a wavelength shifting fiber and routed to an avalanche photodiode pixel The reach of NOvA for sin^2(2_theta_13) and related topics is increased relative to earlier versions of the proposal with the assumption of increased protons available from the Fermilab Main Injector following the end of Tevatron Collider operations in 2009

301 citations

Journal ArticleDOI
D. G. Michael1, P. Adamson2, P. Adamson3, P. Adamson4  +294 moreInstitutions (32)
TL;DR: The main injector neutrino oscillation search (MINOS) experiment as mentioned in this paper uses an accelerator-produced Neutrino beam to perform precision measurements of the neutrinos oscillation parameters.
Abstract: The Main Injector Neutrino Oscillation Search (MINOS) experiment uses an accelerator-produced neutrino beam to perform precision measurements of the neutrino oscillation parameters in the “atmospheric neutrino” sector associated with muon neutrino disappearance. This long-baseline experiment measures neutrino interactions in Fermilab's NuMI neutrino beam with a near detector at Fermilab and again 735 km downstream with a far detector in the Soudan Underground Laboratory in northern Minnesota. The two detectors are magnetized steel-scintillator tracking calorimeters. They are designed to be as similar as possible in order to ensure that differences in detector response have minimal impact on the comparisons of event rates, energy spectra and topologies that are essential to MINOS measurements of oscillation parameters. The design, construction, calibration and performance of the far and near detectors are described in this paper.

265 citations

Journal ArticleDOI
P. Adamson1, C. Andreopoulos2, R. Armstrong3, D. J. Auty4, D. S. Ayres5, C. Backhouse6, G.D. Barr6, M. Bishai7, Andrew Blake8, G. J. Bock1, D. J. Boehnlein1, D. Bogert1, S. Cavanaugh9, D. Cherdack10, S. Childress1, Brajesh C Choudhary1, Joao A B Coelho11, S. J. Coleman12, L. Corwin3, Daniel P Cronin-Hennessy13, I. Z. Danko14, J. K. de Jong6, N. E. Devenish4, M. V. Diwan7, M. Dorman15, Carlos Escobar11, J. J. Evans15, E. Falk4, G. J. Feldman9, M. V. Frohne16, H. R. Gallagher10, R. A. Gomes17, Maury Goodman5, P. Gouffon18, N. Graf19, R. Gran13, N. Grant2, K. Grzelak20, Alec Habig13, D. A. Harris1, J. Hartnell2, R. Hatcher1, A. Himmel21, A. Holin15, Xian-Rong Huang5, J. Hylen1, J. Ilic2, G. M. Irwin22, Z. Isvan14, D. E. Jaffe7, C. James1, D. A. Jensen1, T. Kafka10, S. M. S. Kasahara13, G. Koizumi1, Sacha E Kopp23, M. Kordosky12, A. E. Kreymer1, Karol Lang23, G. Lefeuvre4, P. J. Litchfield2, R. P. Litchfield6, L. Loiacono23, P. Lucas1, W. A. Mann10, Marvin L Marshak13, N. Mayer3, A. M. McGowan5, R. Mehdiyev23, J. R. Meier13, M. D. Messier3, D. G. Michael21, W. H. Miller13, S. R. Mishra24, John C. Mitchell8, C. D. Moore1, Jorge G. Morfin1, L. Mualem21, S. L. Mufson3, J. A. Musser3, D. Naples14, J. K. Nelson12, Harvey B Newman21, R. J. Nichol15, J. A. Nowak13, W. P. Oliver10, M. Orchanian21, R. Ospanov23, J. M. Paley5, R. B. Patterson21, Gregory J Pawloski22, G. F. Pearce2, David Petyt13, S. Phan-Budd5, R. K. Plunkett1, X. Qiu22, J. Ratchford23, T. M. Raufer2, B. Rebel1, P. A. Rodrigues6, C. Rosenfeld24, H. A. Rubin19, M. C. Sanchez5, J. Schneps10, P. Schreiner5, P. Shanahan1, Caleb Smith15, A. Sousa9, P. Stamoulis25, Matthew L Strait13, N. Tagg26, R. L. Talaga5, Juergen Thomas15, M. A. Thomson8, G. Tinti6, R. Toner8, G. Tzanakos25, J. Urheim3, P. Vahle12, B. Viren7, A. C. Weber6, R. C. Webb27, Christopher G. White19, L. Whitehead7, Stanley G. Wojcicki22, T. Yang22, R. Zwaska1 
TL;DR: Measurements of neutrino oscillations using the disappearance of muon neutrinos from the Fermilab NuMI Neutrino beam as observed by the two MINOS detectors are reported.
Abstract: Measurements of neutrino oscillations using the disappearance of muon neutrinos from the Fermilab NuMI neutrino beam as observed by the two MINOS detectors are reported. New analysis methods have been applied to an enlarged data sample from an exposure of 7.25×10^(20) protons on target. A fit to neutrino oscillations yields values of |Δm^2|=(2.32_(-0.08)^(+0.12))×10^(-3) eV^2 for the atmospheric mass splitting and sin^2(2θ)>0.90 (90% C.L.) for the mixing angle. Pure neutrino decay and quantum decoherence hypotheses are excluded at 7 and 9 standard deviations, respectively.

247 citations

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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
202113
20204
20199
201817
201732
201628