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Related papers: Radiation hardness study for the COMET Phase-I ele…

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The Technical Design for the COMET Phase-I experiment is presented in this paper. COMET is an experiment at J-PARC, Japan, which will search for neutrinoless conversion of muons into electrons in the field of an aluminium nucleus ($\mu-e$…

Instrumentation and Detectors · Physics 2020-05-20 The COMET Collaboration , R. Abramishvili , G. Adamov , R. R. Akhmetshin , A. Allin , J. C. Angélique , V. Anishchik , M. Aoki , D. Aznabayev , I. Bagaturia , G. Ban , Y. Ban , D. Bauer , D. Baygarashev , A. E. Bondar , C. Cârloganu , B. Carniol , T. T. Chau , J. K. Chen , S. J. Chen , Y. E. Cheung , W. da Silva , P. D. Dauncey , C. Densham , G. Devidze , P. Dornan , A. Drutskoy , V. Duginov , Y. Eguchi , L. B. Epshteyn , P. Evtoukhovich , S. Fayer , G. V. Fedotovich , M. Finger , M. Finger , Y. Fujii , Y. Fukao , J. L. Gabriel , P. Gay , E. Gillies , D. N. Grigoriev , K. Gritsay , V. H. Hai , E. Hamada , I. H. Hashim , S. Hashimoto , O. Hayashi , T. Hayashi , T. Hiasa , Z. A. Ibrahim , Y. Igarashi , F. V. Ignatov , M. Iio , K. Ishibashi , A. Issadykov , T. Itahashi , A. Jansen , X. S. Jiang , P. Jonsson , T. Kachelhoffer , V. Kalinnikov , E. Kaneva , F. Kapusta , H. Katayama , K. Kawagoe , R. Kawashima , N. Kazak , V. F. Kazanin , O. Kemularia , A. Khvedelidze , M. Koike , T. Kormoll , G. A. Kozlov , A. N. Kozyrev , M. Kravchenko , B. Krikler , G. Kumsiashvili , Y. Kuno , Y. Kuriyama , Y. Kurochkin , A. Kurup , B. Lagrange , J. Lai , M. J. Lee , H. B. Li , R. P. Litchfield , W. G. Li , T. Loan , D. Lomidze , I. Lomidze , P. Loveridge , G. Macharashvili , Y. Makida , Y. J. Mao , O. Markin , Y. Matsuda , A. Melkadze , A. Melnik , T. Mibe , S. Mihara , N. Miyamoto , Y. Miyazaki , F. Mohamad Idris , K. A. Mohamed Kamal Azmi , A. Moiseenko , M. Moritsu , Y. Mori , T. Motoishi , H. Nakai , Y. Nakai , T. Nakamoto , Y. Nakamura , Y. Nakatsugawa , Y. Nakazawa , J. Nash , H. Natori , V. Niess , M. Nioradze , H. Nishiguchi , K. Noguchi , T. Numao , J. O'Dell , T. Ogitsu , S. Ohta , K. Oishi , K. Okamoto , T. Okamura , K. Okinaka , C. Omori , T. Ota , J. Pasternak , A. Paulau , D. Picters , V. Ponariadov , G. Quémener , A. A. Ruban , V. Rusinov , B. Sabirov , H. Sakamoto , P. Sarin , K. Sasaki , A. Sato , J. Sato , Y. K. Semertzidis , N. Shigyo , Dz. Shoukavy , M. Slunecka , D. Stöckinger , M. Sugano , T. Tachimoto , T. Takayanagi , M. Tanaka , J. Tang , C. V. Tao , A. M. Teixeira , Y. Tevzadze , T. Thanh , J. Tojo , S. S. Tolmachev , M. Tomasek , M. Tomizawa , T. Toriashvili , H. Trang , I. Trekov , Z. Tsamalaidze , N. Tsverava , T. Uchida , Y. Uchida , K. Ueno , E. Velicheva , A. Volkov , V. Vrba , W. A. T. Wan Abdullah , P. Warin-Charpentier , M. L. Wong , T. S. Wong , C. Wu , T. Y. Xing , H. Yamaguchi , A. Yamamoto , M. Yamanaka , T. Yamane , Y. Yang , T. Yano , W. C. Yao , B. Yeo , H. Yoshida , M. Yoshida , T. Yoshioka , Y. Yuan , Yu. V. Yudin , M. V. Zdorovets , J. Zhang , Y. Zhang , K. Zuber

The COMET experiment at J-PARC, Japan, aims to search for muon to electron conversion with aluminium nuclei, achieving a sensitivity four orders of magnitude higher than the current upper limit at a 90% confidence level. The proton beam…

High Energy Physics - Experiment · Physics 2023-08-29 Yuki Fujii

The COMET experiment aims to search for the neutrinoless muon to electron transition process with new sensitivity levels. The online trigger system is an integral part of achieving the sensitivity levels required and will be subject to an…

Instrumentation and Detectors · Physics 2024-10-30 Sam Dekkers , Yu Nakazawa , Yuki Fujii , Hisataka Yoshida , Ting Sam Wong , Kazuki Ueno , Jordan Nash

Charged Lepton Flavor Violation is expected to be one of the most powerful tools to reveal physics beyond the Standard Model. The COMET experiment aims to search for the neutrinoless coherent transition of a muon into an electron in the…

High Energy Physics - Experiment · Physics 2022-03-29 Manabu Moritsu

The scheduled High Luminosity upgrade of the CERN Large Hadron Collider presents new challenges in terms of radiation hardness. As a consequence, campaigns to qualify the radiation hardness of detector sensors and components are undertaken…

Electrical and electronic systems can be disturbed by radiation-induced effects. In some cases, radiation-induced effects are of a low probability and can be ignored; however, radiation effects must be considered when designing systems that…

Accelerator Physics · Physics 2016-07-07 B. Todd , S. Uznanski

The electronics used in the data readout and triggering system for the Compact Muon Solenoid (CMS) experiment at the Large Hadron Collider (LHC) particle accelerator at CERN are exposed to high radiation levels. This radiation can cause…

Electronic components used in high energy physics experiments are subjected to a radiation background composed of high energy hadrons, mesons and photons. These particles can induce permanent and transient effects that affect the normal…

Instrumentation and Detectors · Physics 2015-09-02 Kai Chen , Hucheng Chen , James Kierstead , Helio Takai , Sergio Rescia , Xueye Hu , Hao Xu , Joseph Mead , Francesco Lanni , Marena Minelli

The experimental search for coherent neutrinoless conversion of muon to electron in the presence of a nucleus, aims to probe the possibility of charged lepton flavour violation. The COMET experiment at J-PARC is one such setup offering…

High Energy Physics - Experiment · Physics 2022-01-14 D. Mulmule

Radiation hardness is an important requirement for solid state readout devices operating in high radiation environments common in particle physics experiments. The MEGII experiment, at PSI, Switzerland, investigates the forbidden decay…

Instrumentation and Detectors · Physics 2017-08-02 P. W. Cattaneo , T. Cervi , A. Menegolli , M. Oddone , M. Prata , M. C. Prata , M. Rossella

An irradiation campaign was conducted to provide guidance in the selection of materials and components for the radiation hardening of LED lights for use in CERN accelerator tunnels. This work describes the effects of gamma-rays on…

Accelerator Physics · Physics 2020-10-14 Alessandro Floriduz , James D. Devine

Pixel detectors are used in the innermost part of the multi purpose experiments at LHC and are therefore exposed to the highest fluences of ionising radiation, which in this part of the detectors consists mainly of charged pions. The…

Instrumentation and Detectors · Physics 2010-11-30 T. Rohe , A. Bean , W. Erdmann , H. -C. Kaestli , S. Khalatyan , B. Meier , V. Radicci , J. Sibille

We present the design and initial prototype results of a pixellized proton beam profile monitor for the COMET experiment at J-PARC. The goal of COMET is to look for charged lepton flavor violation by direct muon to electron conversion at a…

Instrumentation and Detectors · Physics 2014-11-18 M. Cerv , P. Sarin , H. Pernegger , P. Vageesvaran , E. Griesmayer

The COMET experiment, conducted at J-PARC, aims to search for muon-to-electron conversion with an unprecedentedly high sensitivity. One of the severest backgrounds in the Phase-I experiment originates from cosmic-ray muons. A cosmic muon…

High Energy Physics - Experiment · Physics 2025-08-22 Manabu Moritsu , Hai-Bo Li , Tianyu Xing , Ye Yuan , Yao Zhang

We argue that the COMET experiment --- a dedicated experiment for the $\mu$-$e$ conversion search --- can be a powerful facility to search for heavy neutrinos in the mass range $1\,{\rm MeV} \lesssim M \lesssim 100\,{\rm MeV}$. The stopped…

High Energy Physics - Phenomenology · Physics 2016-03-16 Takehiko Asaka , Atsushi Watanabe

The physics potential of an intense source of low-energy muons is studied. Such a source is a necessary stage towards building the neutrino factories and muon colliders which are being considered at present. The CERN Neutrino Factory could…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Aysto , A. Baldini , A. Blondel , A. de Gouvea , J. Ellis , W. Fetscher , G. F. Giudice , K. Jungmann , S. Lola , V. Palladino , K. Tobe , A. Vacchi , A. van der Schaaf , K. Zuber

Materials to be deployed in space applications have to undergo a variety of different test scenarios, simulating actual space conditions. Among these materials solar photovoltaic cells, optics, meta-materials and more will be directly…

The bulk irradiation of materials with 10-30 MeV protons promises to advance the study of radiation damage for fission and fusion power plants. Intermediate energy proton beams can now be dedicated to materials irradiation within…

A novel type of resistive plate chamber, based on diamond-like carbon (DLC) electrodes is under development for background identification in the MEG II experiment. The DLC-RPC is required to have a radiation hardness to mass irradiation…

Instrumentation and Detectors · Physics 2024-07-09 Masato Takahashi , Sei Ban , Weiyuan Li , Atsuhiko Ochi , Wataru Ootani , Atsushi Oya , Hiromu Suzuki , Kensuke Yamamoto

Forbidden in the Standard Model, Charged Lepton Flavour Violation is a strong probe for New Physics. The COMET Experiment will measure one of these processes: that of COherent Muon to Electron Transitions, where a muon converts to an…

Instrumentation and Detectors · Physics 2015-12-31 Benjamin Edward Krikler
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