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A measurement is presented of the flux ratio of positive and negative muons from cosmic ray interactions in the atmosphere, using data collected by the CMS detector at ground level and in the underground experimental cavern. The excellent…

High Energy Physics - Experiment · Physics 2011-04-22 Lars Sonnenschein

This paper describes a new measurement of the flux ratio of positive and negative muons from cosmic-ray interactions in the atmosphere, using data collected by the CMS detector at ground level and in the underground experimental cavern. The…

High Energy Physics - Experiment · Physics 2010-10-07 Gavin Hesketh

We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN…

High Energy Physics - Experiment · Physics 2012-08-27 The CMS Collaboration

This work presents the measurements of the cosmic muon charge ratio as a function of full azimuthal angle and momentum within the range of 0.8 to 3.0 GeV/c, using the mini-ICAL detector. The detector, comprising 10 layers of RPCs, has…

High Energy Physics - Experiment · Physics 2024-10-10 Raj Shah , J. M. John , Suryanarayan Mondal , S. Pethuraj , G. Majumder , P. Shukla

The charge ratio ${k \equiv \mu^+/\mu^-}$ for atmospheric muons has been measured using Large Volume Detector (LVD) in the INFN Gran Sasso National Laboratory, Italy (minimal depth is 3000 m w.e.). To reach this depth muons should have the…

The muon charge ratio of ultrahigh energy cosmic rays may provide information to detect the composition of the primary cosmic rays. We propose to extract the charge information of high energy muons in very inclined extensive air showers by…

Astrophysics · Physics 2009-11-13 Bo-Qiang Ma

The performance of muon reconstruction in CMS is evaluated using a large data sample of cosmic-ray muons recorded in 2008. Efficiencies of various high-level trigger, identification, and reconstruction algorithms have been measured for a…

Instrumentation and Detectors · Physics 2012-08-27 CMS Collaboration

The magnetized MINOS near detector can accurately determine the charge sign of atmospheric muons, this facilitates a measurement of the atmospheric muon charge ratio. To reduce the systematic error associated with geometric bias and…

High Energy Physics - Experiment · Physics 2019-08-13 J. K. de Jong

A magnetic detector such as MINOS which is measuring the sign of muons has to deal with issues of bending, which depend on the magnetic field configuration, and multiple scattering, which depends on the amount of material which is…

Instrumentation and Detectors · Physics 2007-06-06 Maury Goodman

The charge ratio, $R_\mu = N_{\mu^+}/N_{\mu^-}$, for cosmogenic multiple-muon events observed at an under- ground depth of 2070 mwe has been measured using the magnetized MINOS Far Detector. The multiple-muon events, recorded nearly…

High Energy Physics - Experiment · Physics 2016-04-06 Minos Collaboration , P. Adamson , I. Anghel , A. Aurisano , G. Barr , M. Bishai , A. Blake , G. J. Bock , D. Bogert , S. V. Cao , T. J. Carroll , C. M. Castromonte , R. Chen , S. Childress , J. A. B. Coelho , L. Corwin , D. Cronin-Hennessy , J. K. de Jong , S. De Rijck , A. V. Devan , N. E. Devenish , M. V. Diwan , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , W. Flanagan , M. V. Frohne , M. Gabrielyan , H. R. Gallagher , S. Germani , R. A. Gomes , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , K. Grzelak , A. Habig , S. R. Hahn , J. Hartnell , R. Hatcher , A. Holin , J. Huang , J. Hylen , G. M. Irwin , Z. Isvan , C. James , D. Jensen , T. Kafka , S. M. S. Kasahara , G. Koizumi , M. Kordosky , A. Kreymer , K. Lang , J. Ling , P. J. Litchfield , P. Lucas , W. A. Mann , M. L. Marshak , N. Mayer , C. McGivern , M. M. Medeiros , R. Mehdiyev , J. R. Meier , M. D. Messier , W. H. Miller , S. R. Mishra , S. Moed Sher , C. D. Moore , L. Mualem , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , J. A. Nowak , J. O'Connor , M. Orchanian , R. B. Pahlka , J. Paley , R. B. Patterson , G. Pawloski , A. Perch , M. Pfützner , D. D. Phan , S. Phan-Budd , R. K. Plunkett , N. Poonthottathil , X. Qiu , A. Radovic , B. Rebel , C. Rosenfeld , H. A. Rubin , P. Sail , M. C. Sanchez , J. Schneps , A. Schreckenberger , P. Schreiner , R. Sharma , A. Sousa , N. Tagg , R. L. Talaga , J. Thomas , M. A. Thomson , X. Tian , A. Timmons , J. Todd , S. C. Tognini , R. Toner , D. Torretta , G. Tzanakos , J. Urheim , P. Vahle , B. Viren , A. Weber , R. C. Webb , C. White , L. Whitehead , L. H. Whitehead , S. G. Wojcicki , R. Zwaska

This work presents a novel cosmic-ray scattering experiment employing a Resistive Plate Chambers (RPC) muon tomography system. By introducing the scattering angle between incident and outgoing cosmic-ray tracks as a key observable, this…

Muons from cosmic-ray interactions in the atmosphere provide a high-statistics source of particles that can be used to study the performance and calibration of the ATLAS detector. Cosmic-ray muons can penetrate to the cavern and deposit…

Instrumentation and Detectors · Physics 2012-08-27 The ATLAS Collaboration

The muon charge ratio of the lateral muon density distributions in single EAS is studied by simulations, in context of recent proposals to measure this observable in coincidence with EAS observations. While effects of the hadronic…

Astrophysics · Physics 2009-11-13 H. Rebel , O. Sima , A. Haungs , C. Manailescu , B. Mitrica , C. Morariu

The OPERA detector at the Gran Sasso underground laboratory (LNGS) was used to measure the atmospheric muon charge ratio in the TeV energy region. We analyzed 403069 atmospheric muons corresponding to 113.4 days of livetime during the 2008…

High Energy Physics - Experiment · Physics 2010-03-10 OPERA Collaboration , N. Agafonova , A. Anokhina , S. Aoki , A. Ariga , T. Ariga , D. Autiero , A. Badertscher , A. Bagulya , A. Bertolin , M. Besnier , D. Bick , V. Boyarkin , C. Bozza , T. Brugière , R. Brugnera , G. Brunetti , S. Buontempo , A. Cazes , L. Chaussard , M. Chernyavsky , V. Chiarella , N. Chon-Sen , A. Chukanov , M. Cozzi , G. D'Amato , F. Dal Corso , N. D'Ambrosio , G. De Lellis , Y. D'eclais , M. De Serio , F. Di Capua , D. Di Ferdinando , A. Di Giovanni , N. Di Marco , S. Dmitrievski , M. Dracos , D. Duchesneau , S. Dusini , J. Ebert , O. Egorov , R. Enikeev , A. Ereditato , L. S. Esposito , J. Favier , G. Felici , T. Ferber , R. Fini , D. Frekers , T. Fukuda , C. Fukushima , V. I. Galkin , A. Garfagnini , G. Giacomelli , M. Giorgini , C. Goellnitz , J. Goldberg , D. Golubkov , L. Goncharova , Y. Gornushkin , G. Grella , F. Grianti , M. Guler , C. Gustavino , C. Hagner , K. Hamada , T. Hara , M. Hierholzer , K. Hoshino , M. Ieva , K. Jakovcic , C. Jollet , F. Juget , M. Kazuyama , S. H. Kim , M. Kimura , B. Klicek , J. Knuesel , K. Kodama , M. Komatsu , U. Kose , I. Kreslo , H. Kubota , C. Lazzaro , J. Lenkeit , A. Ljubicic , A. Longhin , G. Lutter , A. Malgin , G. Mandrioli , A. Marotta , J. Marteau , T. Matsuo , V. Matveev , N. Mauri , E. Medinaceli , F. Meisel , A. Meregaglia , P. Migliozzi , S. Mikado , S. Miyamoto , P. Monacelli , K. Morishima , U. Moser , M. T. Muciaccia , N. Naganawa , T. Naka , M. Nakamura , T. Nakano , D. Naumov , V. Nikitina , K. Niwa , Y. Nonoyama , S. Ogawa , A. Olchevski , C. Oldorf , G. Orlova , V. Osedlo , M. Paniccia , A. Paoloni , B. D. Park , I. G. Park , A. Pastore , L. Patrizii , E. Pennacchio , H. Pessard , V. Pilipenko , C. Pistillo , G. Policastro , N. Polukhina , M. Pozzato , K. Pretzl , P. Publichenko , F. Pupilli , R. Rescigno , T. Roganova , H. Rokujo , G. Romano , G. Rosa , I. Rostovtseva , A. Rubbia , A. Russo , V. Ryasny , O. Ryazhskaya , O. Sato , Y. Sato , A. Schembri , W. Schmidt Parzefall , H. Schroeder , L. Scotto Lavina , A. Sheshukov , H. Shibuya , S. Simone , M. Sioli , C. Sirignano , G. Sirri , J. S. Song , M. Spinetti , L. Stanco , N. Starkov , M. Stipcevic , T. Strauss , P. Strolin , S. Takahashi , M. Tenti , F. Terranova , I. Tezuka , V. Tioukov , P. Tolun , T. Tran , S. Tufanli , P. Vilain , M. Vladimirov , L. Votano , J. L. Vuilleumier , G. Wilquet , B. Wonsak , V. Yakushev , C. S. Yoon , T. Yoshioka , J. Yoshida , Y. Zaitsev , S. Zemskova , A. Zghiche , R. Zimmermann

MINOS is the first large magnetic detector deep underground and is the first to measure the muon charge ratio with high statistics in the region near 1 TeV.\cite{bib:adamson} An approximate formula for the muon charge ratio can be expressed…

High Energy Physics - Experiment · Physics 2007-06-07 Philip Schreiner , Maury Goodman

High-energy cosmic rays are observed indirectly by detecting the extensive air showers initiated in Earth's atmosphere. The interpretation of these observations relies on accurate models of air shower physics, which is a challenge and an…

In this work, we propose a new approach to cosmic ray muon momentum measurement using multiple pressurized gaseous Cherenkov radiators. Knowledge of cosmic ray muon momentum has the potential to significantly improve and expand the use of a…

Instrumentation and Detectors · Physics 2021-10-29 Junghyun Bae , Stylianos Chatzidakis

Cosmic-rays with energies up to $3\times10^{20}$ eV have been observed. The nuclear composition of these cosmic rays is unknown but if the incident nuclei are protons then the corresponding center of mass energy is $\sqrt{s_{nn}} = 700$…

Nuclear Experiment · Physics 2009-11-18 Spencer R. Klein

We present a new measurement of atmospheric muons made during an ascent of the High Energy Antimatter Telescope balloon experiment. The muon charge ratio mu+/mu- as a function of atmospheric depth in the momentum interval 0.3-0.9 GeV/c is…

Interpretation of measurements of the muon charge ratio in the TeV range depends on the spectra of protons and neutrons in the primary cosmic radiation and on the inclusive cross sections for production of $\pi^\pm$ and $K^\pm$ in the…

High Energy Astrophysical Phenomena · Physics 2015-06-03 Thomas K. Gaisser
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