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This paper describes the performance and sensitivity to neutrino mixing parameters of a Magnetised Iron Neutrino Detector (MIND) at a Neutrino Factory with a neutrino beam created from the decay of 10 GeV muons. Specifically, it is…

High Energy Physics - Experiment · Physics 2013-10-14 R. Bayes , A. Laing , F. J. P. Soler , A. Cervera Villanueva , J. J. Gómez Cadenas , P. Hernández , J. Martín-Albo , J. Burguet-Castell

We report constraints on antineutrino oscillation parameters that were obtained by using the two MINOS detectors to measure the 7% muon antineutrino component of the NuMI neutrino beam. In the Far Detector, we select 130 events in the…

High Energy Physics - Experiment · Physics 2013-05-29 MINOS Collaboration , P. Adamson , D. J. Auty , D. S. Ayres , C. Backhouse , G. Barr , M. Bishai , A. Blake , G. J. Bock , D. J. Boehnlein , D. Bogert , S. V. Cao , S. Cavanaugh , D. Cherdack , S. Childress , B. C. Choudhary , J. A. B. Coelho , S. J. Coleman , L. Corwin , D. Cronin-Hennessy , I. Z. Danko , J. K. de Jong , N. E. Devenish , M. V. Diwan , M. Dorman , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , M. V. Frohne , H. R. Gallagher , R. A. Gomes , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , N. Grant , K. Grzelak , A. Habig , J. Hartnell , R. Hatcher , A. Himmel , A. Holin , C. Howcroft , X. Huang , J. Hylen , G. M. Irwin , Z. Isvan , D. E. Jaffe , C. James , D. Jensen , T. Kafka , S. M. S. Kasahara , G. Koizumi , S. Kopp , M. Kordosky , A. Kreymer , K. Lang , G. Lefeuvre , J. Ling , P. J. Litchfield , L. Loiacono , P. Lucas , W. A. Mann , M. L. Marshak , M. Mathis , N. Mayer , R. Mehdiyev , J. R. Meier , M. D. Messier , D. G. Michael , W. H. Miller , S. R. Mishra , J. Mitchell , C. D. Moore , L. Mualem , S. Mufson , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , J. A. Nowak , J. P. Ochoa-Ricoux , W. P. Oliver , M. Orchanian , R. Pahlka , J. Paley , R. B. Patterson , G. 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 , R. Sharma , A. Sousa , M. Strait , N. Tagg , R. L. Talaga , M. A. Tavera , J. Thomas , M. A. Thomson , G. Tinti , R. Toner , D. Torretta , G. Tzanakos , J. Urheim , P. Vahle , B. Viren , J. J. Walding , A. Weber , R. C. Webb , C. White , L. Whitehead , S. G. Wojcicki , T. Yang , R. Zwaska

The search for weakly interacting massive particles (WIMPs) by direct detection faces an encroaching background due to coherent neutrino-nucleus scattering. As the sensitivity of these experiments improves, the question of how to best…

Cosmology and Nongalactic Astrophysics · Physics 2015-09-21 Ciaran A. J. O'Hare , Anne M. Green , Julien Billard , Enectali Figueroa-Feliciano , Louis E. Strigari

Probably the most promising way of detecting cosmic neutrinos is measuring the mechanical force exerted by elastic scattering of cosmic neutrinos from macroscopic targets. The expected acceleration is $\sim 10^{-23} cm/s^2$ for Dirac…

Astrophysics · Physics 2009-10-31 C. Hagmann

The MUNU detector has been designed to study antineutrino-electron elastic scattering at low energy. The central tracking detector is a 1 m3 Time Projection Chamber surrounded by an anti-Compton detector. In this paper the results from…

High Energy Physics - Experiment · Physics 2019-08-13 Zornitza Daraktchieva

Neutrino telescopes of kilometer size are currently being planned. They will be two or three orders of magnitude bigger than presently operating detectors, but they will have a much higher muon energy threshold. We discuss the trade-off…

High Energy Physics - Phenomenology · Physics 2016-08-25 L. Bergstrom , J. Edsjo , P. Gondolo

The OPERA detector, designed to search for $\nu_{\mu} \to \nu_{\tau}$ oscillations in the CNGS beam, is located in the underground Gran Sasso laboratory, a privileged location to study TeV-scale cosmic rays. For the analysis here presented,…

High Energy Physics - Experiment · Physics 2015-06-18 N. Agafonova , A. Anokhina , S. Aoki , A. Ariga , T. Ariga , D. Bender , A. Bertolin , C. Bozza , R. Brugnera , A. Buonaura , S. Buontempo , B. Buettner , M. Chernyavsky , A. Chukanov , L. Consiglio , N. D'Ambrosio , G. De Lellis , M. De Serio , P. Del Amo Sanchez , A. Di Crescenzo , D. Di Ferdinando , N. Di Marco , S. Dmitrievski , M. Dracos , D. Duchesneau , S. Dusini , T. Dzhatdoev , J. Ebert , A. Ereditato , R. A. Fini , T. Fukuda , G. Galati , A. Garfagnini , G. Giacomelli , C. Goellnitz , J. Goldberg , Y. Gornushkin , G. Grella , M. Guler , C. Gustavino , C. Hagner , T. Hara , A. Hollnagel , B. Hosseini , H. Ishida , K. Ishiguro , K. Jakovcic , C. Jollet , C. Kamiscioglu , M. Kamiscioglu , J. Kawada , J. H. Kim , S. H. Kim , N. Kitagawa , B. Klicek , K. Kodama , M. Komatsu , U. Kose , I. Kreslo , A. Lauria , J. Lenkeit , A. Ljubicic , A. Longhin , P. Loverre , A. Malgin , M. Malenica , G. Mandrioli , T. Matsuo , V. Matveev , N. Mauri , E. Medinaceli , A. Meregaglia , S. Mikado , P. Monacelli , M. C. Montesi , K. Morishima , M. T. Muciaccia , N. Naganawa , T. Naka , M. Nakamura , T. Nakano , Y. Nakatsuka , K. Niwa , S. Ogawa , N. Okateva , A. Olshevsky , T. Omura , K. Ozaki , A. Paoloni , B. D. Park , I. G. Park , L. Pasqualini , A. Pastore , L. Patrizii , H. Pessard , C. Pistillo , D. Podgrudkov , N. Polukhina , M. Pozzato , F. Pupilli , M. Roda , H. Rokujo , T. Roganova , G. Rosa , O. Ryazhskaya , O. Sato , A. Schembri , I. Shakiryanova , T. Shchedrina , A. Sheshukov , H. Shibuya , T. Shiraishi , G. Shoziyoev , S. Simone , M. Sioli , C. Sirignano , G. Sirri , M. Spinetti , L. Stanco , N. Starkov , S. M. Stellacci , M. Stipcevic , P. Strolin , S. Takahashi , M. Tenti , F. Terranova , V. Tioukov , S. Tufanli , P. Vilain , M. Vladimirov , L. Votano , J. L. Vuilleumier , G. Wilquet , B. Wonsak , C. S. Yoon , S. Zemskova , A. Zghiche

We briefly discuss the physics motivation for a neutrino factory with varying baseline distances of about 1000 to 9000 km. We describe the amount of non planarity of the storage ring required to service three or four detectors at once. A…

High Energy Physics - Experiment · Physics 2009-10-31 D. B. Cline , Y. Fukui , A. Garren

A neutrino factory has unparalleled physics reach for the discovery and measurement of CP violation in the neutrino sector. A far detector for a neutrino factory must have good charge identification with excellent background rejection and a…

The results of the MACRO experiment on atmospheric neutrino oscillations are presented and discussed. The data concern different event topologies with average neutrino energies of ~ 4 and ~ 50 GeV. The Multiple Coulomb Scattering of muons…

High Energy Physics - Experiment · Physics 2019-08-14 G. Giacomelli

This Letter reports new results on muon neutrino disappearance from NOvA, using a 14 kton detector equivalent exposure of $6.05\times10^{20}$ protons-on-target from the NuMI beam at the Fermi National Accelerator Laboratory. The measurement…

High Energy Physics - Experiment · Physics 2017-04-18 The NOvA Collaboration , P. Adamson , L. Aliaga , D. Ambrose , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , K. Augsten , A. Aurisano , C. Backhouse , M. Baird , B. A. Bambah , K. Bays , B. Behera , S. Bending , R. Bernstein , V. Bhatnagar , B. Bhuyan , J. Bian , T. Blackburn , A. Bolshakova , C. Bromberg , J. Brown , G. Brunetti , N. Buchanan , A. Butkevich , V. Bychkov , M. Campbell , E. Catano-Mur , S. Childress , B. C. Choudhary , B. Chowdhury , T. E. Coan , J. A. B. Coelho , M. Colo , J. Cooper , L. Corwin , L. Cremonesi , D. Cronin-Hennessy , G. S. Davies , J. P. Davies , P. F. Derwent , S. Desai , R. Dharmapalan , P. Ding , Z. Djurcic , E. C. Dukes , H. Duyang , S. Edayath , R. Ehrlich , G. J. Feldman , M. Gabrielyan , H. R. Gallagher , S. Germani , T. Ghosh , A. Giri , R. A. Gomes , M. C. Goodman , V. Grichine , R. Group , D. Grover , B. Guo , A. Habig , J. Hartnell , R. Hatcher , A. Hatzikoutelis , K. Heller , A. Himmel , A. Holin , J. Hylen , F. Jediny , M. Judah , G. K. Kafka , D. Kalra , S. M. S. Kasahara , S. Kasetti , R. Keloth , L. Kolupaeva , S. Kotelnikov , I. Kourbanis , A. Kreymer , A. Kumar , S. Kurbanov , K. Lang , W. M. Lee , S. Lin , J. Liu , M. Lokajicek , J. Lozier , S. Luchuk , K. Maan , S. Magill , W. A. Mann , M. L. Marshak , K. Matera , V. Matveev , D. P. Méndez , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. R. Mishra , R. Mohanta , A. Moren , L. Mualem , M. Muether , S. Mufson , R. Murphy , J. Musser , J. K. Nelson , R. Nichol , E. Niner , A. Norman , T. Nosek , Y. Oksuzian , A. Olshevskiy , T. Olson , J. Paley , P. Pandey , R. B. Patterson , G. Pawloski , D. Pershey , O. Petrova , R. Petti , S. Phan-Budd , R. K. Plunkett , R. Poling , B. Potukuchi , C. Principato , F. Psihas , A. Radovic , R. A. Rameika , B. Rebel , B. Reed , D. Rocco , P. Rojas , V. Ryabov , K. Sachdev , P. Sail , O. Samoylov , M. C. Sanchez , R. Schroeter , J. Sepulveda-Quiroz , P. Shanahan , A. Sheshukov , J. Singh , J. Singh , P. Singh , V. Singh , J. Smolik , N. Solomey , E. Song , A. Sousa , K. Soustruznik , M. Strait , L. Suter , R. L. Talaga , M. C. Tamsett , P. Tas , R. B. Thayyullathil , J. Thomas , X. Tian , S. C. Tognini , J. Tripathi , A. Tsaris , J. Urheim , P. Vahle , J. Vasel , L. Vinton , A. Vold , T. Vrba , B. Wang , M. Wetstein , D. Whittington , S. G. Wojcicki , J. Wolcott , N. Yadav , S. Yang , J. Zalesak , B. Zamorano , R. Zwaska

Neutrino interaction rates for experiments placed off axis in the NuMI beam are calculated. Primary proton beam energy is 120 GeV and four locations at 810 km from target and 6, 12, 30 and 40 km off axis are considered. This report is part…

High Energy Physics - Experiment · Physics 2007-05-23 B. Viren

In experiments for direct dark matter searches, neutrinos coherently scattering off nuclei can produce similar events as Weakly Interacting Massive Particles (WIMPs). To reach sensitivities better than about 10^-10 pb for the elastic WIMP…

For neutrino physics and rare event searches, background related to cosmic muons poses a notable challenge, and must be identified and rejected. It is also a challenge to control the cost with good performance for a large array of cosmic…

The NOvA long-baseline neutrino experiment consists of two highly active, finely segmented, liquid scintillator detectors located 14.6 mrad off Fermilab's NuMI beam axis, with a Near Detector located at Fermilab, and a Far Detector located…

High Energy Physics - Experiment · Physics 2015-11-03 Louise Suter

I present a scheme to obtain a 2 to 40 GeV low emittance muon beam, not requiring cooling and within today's technological resources, to be used for early commissioning of muon accelerator projects, or alternatively dedicated muon and…

Accelerator Physics · Physics 2021-04-27 O. R. Blanco Garcia

Large underwater telescopes have been proposed as a challenging method to measure high energy neutrinos from astrophysical objects. In recent years, The Antares collaboration has designed and realized the first detector of this type in the…

Instrumentation and Methods for Astrophysics · Physics 2026-05-21 K. Gracheva , M. Anghinolfi , V. Kulikovskiy , E. Shirokov , Y. Yakovenko

The elastic nuclear recoil signal, being under intense scrutiny by multiple underground experiments, can be interpreted either as coming from the interaction of nuclei with WIMP dark matter or from the scattering of new species of…

High Energy Physics - Phenomenology · Physics 2014-03-26 Maxim Pospelov , Josef Pradler

Cosmology observations indicate that our universe is composed of 25% dark matter (DM), yet we know little about its microscopic properties. Whereas the gravitational interaction of DM is well understood, its interaction with the Standard…

High Energy Physics - Experiment · Physics 2015-01-05 R. T. Thornton , MiniBooNE-DM collaboration

The neutrino experiment KARMEN is situated at the beam stop neutrino source ISIS. It provides nu_mu's, nu_e's and nu_mu_bar's in equal intensities from the pi+ mu+ decay at rest. The oscillation channels nu_mu->nu_e and nu_mu_bar->nu_e_bar…

High Energy Physics - Experiment · Physics 2012-08-27 KARMEN Collaboration