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The SoLid experiment aims to make a measurement of very short distance neutrino oscillations using reactor antineutrinos. Key to its sensitivity are the experiments high spatial and energy resolution, combined with a very suitable reactor…

Instrumentation and Detectors · Physics 2019-08-13 Daniel Saunders

The mission of the Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt is to explore the QCD phase diagram at high net baryon densities likely to exist in the core of…

Nuclear Experiment · Physics 2020-06-24 Anna Senger

We report on the performance evaluation of a prototype muon trigger detector for the PSI muEDM experiment, conducted as a proof-of-principle test at the $\pi$E1 beamline of the Paul Scherrer Institute (PSI) using \SI{27.5}{MeV/c} muons. The…

The Compact Muon Solenoid (CMS) is a general purpose detector, designed to run at the highest luminosity at the CERN Large Hadron Collider (LHC). Its distinctive features include a 4 T superconducting solenoid with 6-m-diameter by…

Instrumentation and Detectors · Physics 2016-08-09 V. I. Klyukhin , N. Amapane , A. Ball , B. Curé , A. Gaddi , H. Gerwig , M. Mulders , A. Hervé , R. Loveless

Xenon dual-phase time projections chambers (TPCs) have proven to be a successful technology in studying physical phenomena that require low-background conditions. With 40t of liquid xenon (LXe) in the TPC baseline design, DARWIN will have a…

Instrumentation and Detectors · Physics 2024-07-26 M. Adrover , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , B. Antunovic , E. Aprile , M. Babicz , D. Bajpai , E. Barberio , L. Baudis , M. Bazyk , N. Bell , L. Bellagamba , R. Biondi , Y. Biondi , A. Bismark , C. Boehm , A. Breskin , E. J. Brookes , A. Brown , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , A. Chauvin , A. P. Cimental Chavez , A. P. Colijn , J. Conrad , J. J. Cuenca-García , V. D'Andrea , M. P. Decowski , A. Deisting , P. Di Gangi , S. Diglio , M. Doerenkamp , G. Drexlin , K. Eitel , A. Elykov , R. Engel , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , W. Fulgione , P. Gaemers , R. Gaior , M. Galloway , N. Garroum , S. Ghosh , F. Girard , R. Glade-Beucke , F. Glück , L. Grandi , J. Grigat , R. Größle , H. Guan , M. Guida , R. Hammann , V. Hannen , S. Hansmann-Menzemer , N. Hargittai , T. Hasegawa , C. Hils , A. Higuera , K. Hiraoka , L. Hoetzsch , M. Iacovacci , Y. Itow , J. Jakob , F. Jörg , M. Kara , P. Kavrigin , S. Kazama , M. Keller , B. Kilminster , M. Kleifges , M. Kobayashi , A. Kopec , B. von Krosigk , F. Kuger , H. Landsman , R. F. Lang , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , F. Lombardi , J. Loizeau , T. Luce , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , T. Marrodán Undagoitia , J. A. M. Lopes , F. Marignetti , K. Martens , J. Masbou , S. Mastroianni , S. Milutinovic , K. Miuchi , R. Miyata , A. Molinario , C. M. B. Monteiro , K. Morå , E. Morteau , Y. Mosbacher , J. Müller , M. Murra , J. L. Newstead , K. Ni , U. G. Oberlack , I. Ostrovskiy , B. Paetsch , M. Pandurovic , Q. Pellegrini , R. Peres , J. Pienaar , M. Pierre , M. Piotter , G. Plante , T. R. Pollmann , L. Principe , J. Qi , J. Qin , M. Rajado Silva , D. Ramírez García , A. Razeto , S. Sakamoto , L. Sanchez , P. Sanchez-Lucas , J. M. F. dos Santos , G. Sartorelli , A. Scaffidi , P. Schulte , H. -C. Schultz-Coulon , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Sharma , W. Shen , M. Silva , H. Simgen , R. Singh , M. Solmaz , O. Stanley , M. Steidl , P. L. Tan , A. Terliuk , D. Thers , T. Thümmler , F. Tönnies , F. Toschi , G. Trinchero , R. Trotta , C. Tunnell , P. Urquijo , K. Valerius , S. Vecchi , S. Vetter , G. Volta , D. Vorkapic , W. Wang , K. M. Weerman , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , J. Wolf , T. Wolf , V. H. S. Wu , M. Wurm , Y. Xing , M. Yamashita , J. Ye , G. Zavattini , K. Zuber

The Muon Scattering Experiment (MUSE) was developed to address the proton radius puzzle through simultaneous electron-proton and muon-proton scattering using the Paul Scherrer Institute's PiM1 secondary beamline. MUSE uses a…

Luminosity spectrum and accelerator background levels strongly influence the experimental conditions and have an important impact on detector design. The expected rates of the main beam-beam products at CLIC 3 TeV CM energy, taking into…

Accelerator Physics · Physics 2012-02-06 B. Dalena , J. Esberg , D. Schulte

A muon-flux measurement behind the beam dump of the J-PARC Hadron Experimental Facility was performed with a compact muon detector that can be inserted into a vertical observing hole with 81 mm in diameter which was dug underground. The…

Instrumentation and Detectors · Physics 2024-10-30 T. Matsumura , Y. Hirayama , G. Y. Lim , H. Nanjo , T. Nomura , K. Shiomi , H. Watanabe

A novel device to compress the phase space of a muon beam by a factor of $10^{10}$ with a $10^{-3}$ efficiency is under development. A surface muon beam is stopped in a helium gas target consisting of several compression stages, wherein…

Experiments like ATLAS at the HL-LHC or detectors at future hadron colliders need muon detectors with excellent momentum resolution up to the TeV scale both at the trigger and offline reconstruction levels. This requires muon tracking…

The powerful muon and tracker systems of the CMS detector together with dedicated reconstruction software allow precise and efficient measurement of muon tracks originating from proton-proton collisions. The standard muon reconstruction…

Instrumentation and Detectors · Physics 2008-10-22 Norbert Neumeister , Chang Liu

The Compact Muon Solenoid (CMS) Experiment is a general purpose particle detector experiment located at the Large Hadron Collider (LHC) at CERN. In 2008, the LHC beam was commissioned and successfully steered through the CMS detector. First…

High Energy Physics - Experiment · Physics 2019-08-13 Toyoko J. Orimoto

The muons reconstruction package for the SID/ILC detector has been extended to include the Electro-Magnetic Calorimeter. The procedure previously used to reconstruct the charged tracks, an helical fit approximation, has been replaced by a…

Instrumentation and Detectors · Physics 2007-05-23 C. Milstene , G. Fisk , A. Para

In this paper, we present development of a portable cosmic muon tracker tailored for both on-site measurements of cosmic muon flux as well as for outreach activities. The tracker comprises of two 70 mm x 70 mm plastic scintillators,…

Instrumentation and Detectors · Physics 2026-03-02 Yuvaraj Elangovan , Shashwat Kakkad , B. Satyanarayana

Due to the muon tomography's capability of imaging high Z materials, some potential applications have been reported on inspecting smuggled nuclear materials in customs. A compact Cosmic Ray Muons (CRM) imaging prototype, Lanzhou University…

The Compressed Baryonic Matter~(CBM) experiment in the upcoming Facility for Antiproton and Ion Research~(FAIR), designed to take data in nuclear collisions at very high interaction rates of up to 10 MHz, will employ a free-streaming data…

Instrumentation and Detectors · Physics 2021-09-01 V. Singhal , S. Chatterjee , V. Friese , S. Chattopadhyay

The accurate knowledge of the $\bar\nu_e (\nu_\mu)$ beam produced in $\mu^-$ decays and the absence of $\nu_e (\bar\nu_\mu)$ contamination, make a future muon storage ring the ideal place to look for $\numunue$ ($\numubarnuebar$)…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Bueno , M. Campanelli , A. Rubbia

We propose and demonstrate two practical mitigation methods to attenuate the cosmic muon flux, compatible with experiments involving superconducting qubits: shallow underground sites and specific device orientation. Using a…

The NUCLEUS experiment aims at measuring the coherent elastic scattering of nuclear reactor antineutrinos off nuclei using cryogenic calorimeters. Operating at an overburden of 3m.w.e., muon-induced backgrounds are expected to be dominant.…

We revise the process of muon pair production by high-energy muons in rock using the recently published cross-section. The three-dimensional Monte Carlo code MUSIC has been used to obtain the characteristics of the muon bundles initiated…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. A. Kudryavtsev , E. V. Korolkova , N. J. C. Spooner
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