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Future experiments based on the observation of Earth's atmosphere from sub-orbital and orbital altitudes plan to include optical Cherenkov cameras to observe extensive air showers produced by high-energy cosmic radiation via its interaction…

Instrumentation and Methods for Astrophysics · Physics 2021-09-22 Austin Cummings , Roberto Aloisio , Johannes Eser , John Krizmanic

IceCube is a cubic-kilometer Cherenkov detector located in the deep ice at the geographic South Pole. The dominant event yield in the deep ice detector consists of penetrating atmospheric muons produced in cosmic ray air showers with…

High Energy Astrophysical Phenomena · Physics 2019-09-11 Dennis Soldin

Current experiments seeking first-ever observation of Ultra-High Energy Neutrinos (UHEN) typically utilize radio frequency (RF) receiver antennas deployed in cold, radio-transparent polar ice, to measure the coherent RF signals resulting…

Instrumentation and Methods for Astrophysics · Physics 2025-12-18 Christian Hornhuber , Mohammad Ful Hossain Seikh , Mark Stockham , Scott Voigt , Rob Young , Alisa Nozdrina , Sanyukta Agarwal , Shoukat Ali , Kenny Couberly , Dave Besson

The Askaryan Radio Array (ARA) is an ultra-high energy ($>10^{17}$ eV) cosmic neutrino detector in phased construction near the South Pole. ARA searches for radio Cherenkov emission from particle cascades induced by neutrino interactions in…

The Askaryan Radio Array (ARA) is an in-ice ultra high energy (UHE, $>10$ PeV) neutrino experiment at the South Pole that aims to detect UHE neutrino-induced radio emission in ice. ARA consists of five independent stations each consisting…

High Energy Astrophysical Phenomena · Physics 2024-10-01 Paramita Dasgupta

The Muon Ionization Cooling Experiment (MICE) will perform a detailed study of ionization cooling to evaluate the feasibility of the technique. To carry out this program, MICE requires an efficient particle-identification (PID) system to…

Instrumentation and Detectors · Physics 2016-01-20 D. Adams , A. Alekou , M. Apollonio , R. Asfandiyarov , G. Barber , P. Barclay , A. de Bari , R. Bayes , V. Bayliss , P. Bene , R. Bertoni , V. J. Blackmore , A. Blondel , S. Blot , M. Bogomilov , M. Bonesini , C. N. Booth , D. Bowring , S. Boyd , T. W. Bradshaw , U. Bravar , A. D. Bross , F. Cadoux , M. Capponi , T. Carlisle , G. Cecchet , C. Charnley , F. Chignoli , D. Cline , J. H. Cobb , G. Colling , N. Collomb , L. Coney , P. Cooke , M. Courthold , L. M. Cremaldi , S. Debieux , A. DeMello , A. Dick , A. Dobbs , P. Dornan , F. Drielsma , F. Filthaut , T. Fitzpatrick , P. Franchini , V. Francis , L. Fry , A. Gallagher , R. Gamet , R. Gardener , S. Gourlay , A. Grant , J. S. Graulich , J. Greis , S. Griffiths , P. Hanlet , O. M. Hansen , G. G. Hanson , T. L. Hart , T. Hartnett , T. Hayler , C. Heidt , M. Hills , P. Hodgson , C. Hunt , C. Husi , A. Iaciofano , S. Ishimoto , G. Kafka , D. M. Kaplan , Y. Karadzhov , Y. K. Kim , Y. Kuno , P. Kyberd , J-B Lagrange , J. Langlands , W. Lau , M. Leonova , D. Li , A. Lintern , M. Littlefield , K. Long , T. Luo , C. Macwaters , B. Martlew , J. Martyniak , F. Masciocchi , R. Mazza , S. Middleton , A. Moretti , A. Moss , A. Muir , I. Mullacrane , J. J. Nebrensky , D. Neuffer , A. Nichols , R. Nicholson , L. Nicola , E. Noah Messomo , J. C. Nugent , A. Oates , Y. Onel , D. Orestano , E. Overton , P. Owens , V. Palladino , J. Pasternak , F. Pastore , C. Pidcott , M. Popovic , R. Preece , S. Prestemon , D. Rajaram , S. Ramberger , M. A. Rayner , S. Ricciardi , T. J. Roberts , M. Robinson , C. Rogers , K. Ronald , K. Rothenfusser , P. Rubinov , P. Rucinski , H. Sakamato , D. A. Sanders , R. Sandstrom , E. Santos , T. Savidge , P. J. Smith , P. Snopok , F. J. P. Soler , D. Speirs , T. Stanley , G. Stokes , D. J. Summers , J. Tarrant , I. Taylor , L. Tortora , Y. Torun , R. Tsenov , C. D. Tunnell , M. A. Uchida , G. Vankova-Kirilova , S. Virostek , M. Vretenar , P. Warburton , S. Watson , C. White , C. G. Whyte , A. Wilson , H. Wisting , X. Yang , A. Young , M. Zisman

The radio approach for detecting the ultra-high energy cosmic neutrinos has become a mature field. The Cherenkov pulse in radio detection originates from the charge excess of particle showers due to Askaryan effect. The conventional way of…

High Energy Astrophysical Phenomena · Physics 2014-04-29 Chia-Yu Hu , Chih-Ching Chen , Pisin Chen

IceCube is a cubic kilometer neutrino telescope under construction at the South Pole. The primary goal is to discover astrophysical sources of high energy neutrinos. We describe the detector and present results on atmospheric muon neutrinos…

Astrophysics · Physics 2019-08-13 J. Kiryluk

Since the end of the eighties, in response to a reported increase of the total neutrino flux in the Homestake experiment in coincidence with solar flares, neutrino detectors have searched for signals of neutrinos associated with solar flare…

High Energy Astrophysical Phenomena · Physics 2016-06-03 G. de Wasseige

The detection of astrophysical neutrinos by IceCube in the TeV-PeV energy range motivates the development of instruments for observing these particles at higher energies. Moreover, the detection of very-high-energy (VHE) neutrinos could…

High Energy Astrophysical Phenomena · Physics 2023-10-12 Oscar Fernando Romero Matamala

Recently, we reported the commissioning of the new cryogenic ion storage ring RICE, which demonstrated potential capabilities for the precise studies of molecular structures and reaction dynamics. In the present article, we describe the…

Instrumentation and Detectors · Physics 2021-07-07 Y. Nakano , R Igosawa , S. Iida , S. Okada , M. Lindley , S. Menk , R. Nagaoka , T. Hashimoto , S. Yamada , T. Yamaguchi , S. Kuma , T. Azuma

In the field of neutrino astronomy, large volumes of optically transparent matter like glacial ice, lake water, or deep ocean water are used as detector media. Elementary particle interactions are studied using in situ detectors recording…

We present a semi-analytical method for the calculation of coherent Askaryan radiation in showers induced by neutrinos of any flavor in ice. We compare our results with those of a full Monte Carlo simulation based on the ZHAireS code. This…

High Energy Astrophysical Phenomena · Physics 2020-04-15 Jaime Alvarez-Muñiz , P. M. Hansen , Andrés Romero-Wolf , Enrique Zas

The Dual Imaging Cerenkov Experiment (DICE) was designed and operated for making elemental composition measurements of cosmic rays near the knee of the spectrum at several PeV. Here we present the first results using this experiment from…

Astrophysics · Physics 2009-10-30 K. Boothby , M. Chantell , K. D. Green , D. B. Kieda , J. Knapp , C . G. Larsen , S. P. Swordy

We present an approximation for the numerical calculation of Cherenkov radio pulses in the Fraunhofer limit from very high energy showers in dense media. We compare it to full Montecarlo simulations in ice studying its range of…

Astrophysics · Physics 2009-12-30 J. Alvarez-Muñiz , R. A. Vázquez , E. Zas

The IceCube Neutrino Observatory is a detector array at the South Pole with the central aim of studying astrophysical neutrinos. However, the majority of the detected neutrinos originates from cosmic ray interactions in the atmosphere. The…

High Energy Astrophysical Phenomena · Physics 2021-07-21 Karolin Hymon , Tim Ruhe

The main challenge in detecting ultra-high energy (UHE) neutrinos is discriminating a neutrino-induced shower in the background of showers initiated by ultra-high energy nuclei. The resulting shower development from neutrinos exhibits…

High Energy Astrophysical Phenomena · Physics 2024-09-04 Abha R. Khakurdikar , Washington R. Carvalho. , Jörg R. Hörandel

We revisit the theory of Cherenkov radiation in uniaxial crystals. Historically, a number of flawed attempts have been made at explaining this radiation phenomenon and a consistent error-free description is nowhere available. We apply our…

High Energy Physics - Phenomenology · Physics 2016-03-23 R. E. Mikkelsen , T. Poulsen , U. I. Uggerhøj , S. R. Klein

IceCube is a 1 km^3 neutrino telescope currently under construction at the South Pole. The detector will consist of 5160 optical sensors deployed at depths between 1450 m and 2450 m in clear Antarctic ice distributed over 86 strings. An air…

High Energy Astrophysical Phenomena · Physics 2019-08-13 A. Karle

The IceCube Neutrino Observatory instruments about 1 km$^3$ of deep, glacial ice at the geographic South Pole using 5160 photomultipliers to detect Cherenkov light from relativistic, charged particles. Most IceCube science goals rely on…

Instrumentation and Methods for Astrophysics · Physics 2021-10-27 Martin Rongen , Dmitry Chirkin
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