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The South Pole Acoustic Test Setup (SPATS) has been deployed to study the feasibility of acoustic neutrino detection in Antarctic ice around the South Pole. An array of four strings equipped with acoustic receivers and transmitters,…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 Timo Karg

Encompasing a volume of ~1 km^3 of glacial ice at the South Pole, IceCube is currently the worlds largest neutrino detector. It consists of 5160 optical modules on 86 strings in a depth between 1450m and 2450m, as well as 324 optical…

High Energy Astrophysical Phenomena · Physics 2019-08-13 Sebastian Böser

One of the most promising techniques for detecting ultra-high energy neutrinos involves the use of radio antennas to observe the 10-1000 MHz radiation generated by the showers that neutrinos induce in large volumes of ice. The expected…

High Energy Astrophysical Phenomena · Physics 2025-06-05 Alan Coleman , Christian Glaser , Ryan Rice-Smith , Steven Barwick , Dave Besson

High light collection efficiency is an important requirement in any application of scintillation detectors. The purpose of this study is to investigate the possibility for improving this parameter in cryogenic scintillation bolometers,…

Instrumentation and Detectors · Physics 2014-02-11 F. A. Danevich , R. V. Kobychev , V. V. Kobychev , H. Kraus , V. B. Mikhailik , V. M. Mokina

The excellent radio frequency transparency of cold polar ice, combined with the coherent Cherenkov emission produced by neutrino-induced showers when viewed at wavelengths longer than a few centimeters, has spurred considerable interest in…

Astrophysics · Physics 2010-04-30 H. Landsman , L. Ruckman , G. S. Varner

IceCube-DeepCore is a compact Cherenkov detector located in the clear ice of the bottom center of the IceCube Neutrino Telescope. Its purpose is to enhance the sensitivity of IceCube for low neutrino energies (< 1 TeV) and to lower the…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 Christopher Wiebusch

Neutrons are the only neutral hadrons that remain stable over the timescale of an air-shower development. Their energy is lost only through hadronic interactions and quasi-elastic scattering, which results in their high abundance at the…

High Energy Astrophysical Phenomena · Physics 2025-07-24 Tobias Schulz

IceTop, the surface component of the IceCube detector, has been used to measure the energy spectrum of cosmic ray primaries in the range between 1.58 PeV and 1.26 EeV. It can also be used to study the low energy muons in air showers by…

High Energy Astrophysical Phenomena · Physics 2019-08-13 Javier G. Gonzalez

The IceCube Upgrade is an extension of the IceCube detector at the geographic South Pole. It consists of seven new strings with novel instrumentation. More than 430 multi-PMT optical modules called "mDOMs", housing 24 3-inch PMTs each, will…

High Energy Astrophysical Phenomena · Physics 2021-07-22 Lasse Halve , Johannes Werthebach

For the in-ice component of the next generation neutrino observatory at the South Pole, IceCube-Gen2, a new sensor module is being developed, which is an evolution of the D-Egg and mDOM sensors developed for the IceCube Upgrade. The sensor…

Instrumentation and Methods for Astrophysics · Physics 2021-12-16 Vedant Basu , Aya Ishihara , Markus Dittmer , Nobuhiro Shimizu

This study presents preliminary results from the analysis of cosmic-ray anisotropy using air showers detected by the IceTop surface array between 2011 and 2022. With improved statistical precision and updated Monte Carlo simulation events…

High Energy Astrophysical Phenomena · Physics 2025-08-01 Rasha Abbasi , Paolo Desiati , Juan Carlos Díaz Vélez , Frank McNally

The Precision IceCube Next Generation Upgrade (PINGU) is a proposed low-energy in-fill extension to the IceCube Neutrino Observatory. With detection technology modeled closely on the successful IceCube example, PINGU will provide a 6Mton…

High Energy Physics - Experiment · Physics 2017-04-10 Gen2 Collaboration

The IceCube Neutrino Observatory is a cubic-kilometer-scale high-energy neutrino detector built into the ice at the South Pole. Construction of IceCube, the largest neutrino detector built to date, was completed in 2011 and enabled the…

Instrumentation and Methods for Astrophysics · Physics 2024-02-08 IceCube Collaboration , M. G. Aartsen , M. Ackermann , J. Adams , J. A. Aguilar , M. Ahlers , M. Ahrens , D. Altmann , K. Andeen , T. Anderson , I. Ansseau , G. Anton , M. Archinger , C. Argüelles , R. Auer , J. Auffenberg , S. Axani , J. Baccus , X. Bai , S. Barnet , S. W. Barwick , V. Baum , R. Bay , K. Beattie , J. J. Beatty , J. Becker Tjus , K. -H. Becker , T. Bendfelt , S. BenZvi , D. Berley , E. Bernardini , A. Bernhard , D. Z. Besson , G. Binder , D. Bindig , M. Bissok , E. Blaufuss , S. Blot , D. Boersma , C. Bohm , M. Börner , F. Bos , D. Bose , S. Böser , O. Botner , A. Bouchta , J. Braun , L. Brayeur , H. -P. Bretz , S. Bron , A. Burgman , C. Burreson , T. Carver , M. Casier , E. Cheung , D. Chirkin , A. Christov , K. Clark , L. Classen , S. Coenders , G. H. Collin , J. M. Conrad , D. F. Cowen , R. Cross , C. Day , M. Day , J. P. A. M. de André , C. De Clercq , E. del Pino Rosendo , H. Dembinski , S. De Ridder , F. Descamps , P. Desiati , K. D. de Vries , G. de Wasseige , M. de With , T. DeYoung , J. C. Díaz-Vélez , V. di Lorenzo , H. Dujmovic , J. P. Dumm , M. Dunkman , B. Eberhardt , W. R. Edwards , T. Ehrhardt , B. Eichmann , P. Eller , S. Euler , P. A. Evenson , S. Fahey , A. R. Fazely , J. Feintzeig , J. Felde , K. Filimonov , C. Finley , S. Flis , C. -C. Fösig , A. Franckowiak , M. Frère , E. Friedman , T. Fuchs , T. K. Gaisser , J. Gallagher , L. Gerhardt , K. Ghorbani , W. Giang , L. Gladstone , T. Glauch , D. Glowacki , T. Glüsenkamp , A. Goldschmidt , J. G. Gonzalez , D. Grant , Z. Griffith , L. Gustafsson , C. Haack , A. Hallgren , F. Halzen , E. Hansen , T. Hansmann , K. Hanson , J. Haugen , D. Hebecker , D. Heereman , K. Helbing , R. Hellauer , R. Heller , S. Hickford , J. Hignight , G. C. Hill , K. D. Hoffman , R. Hoffmann , K. Hoshina , F. Huang , M. Huber , P. O. Hulth , K. Hultqvist , S. In , M. Inaba , A. Ishihara , E. Jacobi , J. Jacobsen , G. S. Japaridze , M. Jeong , K. Jero , A. Jones , B. J. P. Jones , J. Joseph , W. Kang , A. Kappes , T. Karg , A. Karle , U. Katz , M. Kauer , A. Keivani , J. L. Kelley , J. Kemp , A. Kheirandish , J. Kim , M. Kim , T. Kintscher , J. Kiryluk , N. Kitamura , T. Kittler , S. R. Klein , S. Kleinfelder , M. Kleist , G. Kohnen , R. Koirala , H. Kolanoski , R. Konietz , L. Köpke , C. Kopper , S. Kopper , D. J. Koskinen , M. Kowalski , M. Krasberg , K. Krings , M. Kroll , G. Krückl , C. Krüger , J. Kunnen , S. Kunwar , N. Kurahashi , T. Kuwabara , M. Labare , K. Laihem , H. Landsman , J. L. Lanfranchi , M. J. Larson , F. Lauber , A. Laundrie , D. Lennarz , H. Leich , M. Lesiak-Bzdak , M. Leuermann , L. Lu , J. Ludwig , J. Lünemann , C. Mackenzie , J. Madsen , G. Maggi , K. B. M. Mahn , S. Mancina , M. Mandelartz , R. Maruyama , K. Mase , H. Matis , R. Maunu , F. McNally , C. P. McParland , P. Meade , K. Meagher , M. Medici , M. Meier , A. Meli , T. Menne , G. Merino , T. Meures , S. Miarecki , R. H. Minor , T. Montaruli , M. Moulai , T. Murray , R. Nahnhauer , U. Naumann , G. Neer , M. Newcomb , H. Niederhausen , S. C. Nowicki , D. R. Nygren , A. Obertacke Pollmann , A. Olivas , A. O'Murchadha , T. Palczewski , H. Pandya , D. V. Pankova , S. Patton , P. Peiffer , Ö. Penek , J. A. Pepper , C. Pérez de los Heros , C. Pettersen , D. Pieloth , E. Pinat , P. B. Price , G. T. Przybylski , M. Quinnan , C. Raab , L. Rädel , M. Rameez , K. Rawlins , R. Reimann , B. Relethford , M. Relich , E. Resconi , W. Rhode , M. Richman , B. Riedel , S. Robertson , M. Rongen , C. Roucelle , C. Rott , T. Ruhe , D. Ryckbosch , D. Rysewyk , L. Sabbatini , S. E. Sanchez Herrera , A. Sandrock , J. Sandroos , P. Sandstrom , S. Sarkar , K. Satalecka , P. Schlunder , T. Schmidt , S. Schoenen , S. Schöneberg , A. Schukraft , L. Schumacher , D. Seckel , S. Seunarine , M. Solarz , D. Soldin , M. Song , G. M. Spiczak , C. Spiering , T. Stanev , A. Stasik , J. Stettner , A. Steuer , T. Stezelberger , R. G. Stokstad , A. Stößl , R. Ström , N. L. Strotjohann , K. -H. Sulanke , G. W. Sullivan , M. Sutherland , H. Taavola , I. Taboada , J. Tatar , F. Tenholt , S. Ter-Antonyan , A. Terliuk , G. Tešić , L. Thollander , S. Tilav , P. A. Toale , M. N. Tobin , S. Toscano , D. Tosi , M. Tselengidou , A. Turcati , E. Unger , M. Usner , J. Vandenbroucke , N. van Eijndhoven , S. Vanheule , M. van Rossem , J. van Santen , M. Vehring , M. Voge , E. Vogel , M. Vraeghe , D. Wahl , C. Walck , A. Wallace , M. Wallraff , N. Wandkowsky , Ch. Weaver , M. J. Weiss , C. Wendt , S. Westerhoff , D. Wharton , B. J. Whelan , S. Wickmann , K. Wiebe , C. H. Wiebusch , L. Wille , D. R. Williams , L. Wills , P. Wisniewski , M. Wolf , T. R. Wood , E. Woolsey , K. Woschnagg , D. L. Xu , X. W. Xu , Y. Xu , J. P. Yanez , G. Yodh , S. Yoshida , M. Zoll

The IceCube neutrino observatory is a 3D array of photodetectors installed in the Antarctic ice. It consists of 5,160 photomultiplier-tubes spread among 86 vertical strings making a total detector volume of more than a cubic kilometer. It…

High Energy Astrophysical Phenomena · Physics 2019-08-21 Christoph Tönnis

Current generation neutrino telescopes cover an energy range from about 10 GeV to beyond $10^9$ GeV. IceCube sets the scale for future experiments to make improvements. Strategies for future upgrades will be discussed in three energy…

Instrumentation and Methods for Astrophysics · Physics 2015-06-11 Albrecht Karle

We present development work aiming towards a large scale ice-based hybrid detector including acoustic sensors for the detection of neutrinos in the GZK range. A facility for characterization and calibration of acoustic sensors in clear…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 Thomas Meures , Larissa Paul , Mathieu Ribordy

In 2013 the IceCube collaboration announced the discovery of a cosmic neutrino flux up to PeV energies, validating neutrino astronomy as the next promising observational technique to explore the high-energy Universe. The neutrino community…

High Energy Physics - Experiment · Physics 2019-08-27 S. Toscano , P. Coppin , K. D. de Vries , N. van Eijndhoven , J. A. Aguilar

The SNO+ experiment is the follow up of the SNO experiment, replacing the heavy water volume with about 780 tons of liquid scintillator (LAB) in order to shift the sensitive threshold to lower energy range. The 6000 m.w.e. natural rock…

High Energy Physics - Experiment · Physics 2019-08-14 V. Lozza

The primary motivation for building neutrino telescopes is to open the road for neutrino astronomy, and to offer another observational window for the study of cosmic ray origins. Other physics topics, such as the search for WIMPs, can also…

Astrophysics · Physics 2019-08-13 Cecile Portello-Roucelle

We compared the performance of a SiPM array and a PMT in a laboratory setting using a single 5.08x5.08-cm cylindrical sodium iodide scintillating crystal. Photomultiplier tubes (PMTs) are the most commonly used device to monitor…

Instrumentation and Detectors · Physics 2020-01-23 Tyana Stiegler , Kareem Kazkaz , Erik Swanberg , Vladimir Mozin