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Muon beams of low emittance provide the basis for the intense, well characterised neutrino beams of a neutrino factory and for multi-TeV lepton-antilepton collisions at a muon collider. The international Muon Ionization Cooling Experiment…

Accelerator Physics · Physics 2018-05-21 Paolo Franchini

Electron-cooling offers a relatively simple scheme to enable high-luminosity collisions in future electron-ion and hadron colliders. Contemplated TeV-energy hadron colliders require relativistic (sub 100 MeV) high-charge [${\cal…

Accelerator Physics · Physics 2022-01-19 A. Fetterman , D. Mihalcea , S. Benson , D. Crawford , D. Edstrom , F. Hannon , P. Piot , J. Ruan , S. Wang

A muon collider would open new frontiers of investigation in high energy particle physics, allowing precision measurements to be made at the TeV energy frontier. One of the greatest challenges to constructing a muon collider is the…

Accelerator Physics · Physics 2010-12-20 Daniel Greenwald , Yu Bao , Allen Caldwell , Daniel Kollar

This paper presents the measurement of the scattering of 172 MeV/c muons in assorted materials, including liquid hydrogen, motivated by the need to understand ionisation cooling for muon acceleration. Data are compared with predictions from…

We extend our analysis of holographic meson dissociation in the presence of an intense magnetic field. In addition to the previously known critical temperature above which the mesons melt, we found that for certain magnetic field…

High Energy Physics - Theory · Physics 2020-06-09 Daniel Ávila , Leonardo Patiño

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of parameters of the Higgs boson and the neutrino mixing…

Accelerator Physics · Physics 2019-10-23 Daniel M. Kaplan

The muon detectors of the experiments at the Large Hadron Collider (LHC) have to cope with unprecedentedly high neutron and gamma ray background rates. In the forward regions of the muon spectrometer of the ATLAS detector, for instance,…

Instrumentation and Detectors · Physics 2016-10-04 B. Bittner , J. Dubbert , O. Kortner , H. Kroha , F. Legger , R. Richter , O. Biebel , A. Engl , R. Hertenberger , F. Rauscher

The general-purpose Compact Muon Solenoid (CMS) detector at the Large Hadron Collider (LHC) at CERN includes the hadronic calorimeter to register the energies of the charged and neutral hadrons produced in the proton-proton collisions at…

Instrumentation and Detectors · Physics 2024-01-08 Vyacheslav Klyukhin

We have developed high-efficiency normal-conducting RF accelerating structures by combining H-mode resonator cavities and a transverse beam focusing by permanent-magnet quadrupoles (PMQ), for beam velocities in the range of a few percent of…

Accelerator Physics · Physics 2011-04-20 Sergey S. Kurennoy , Lawrence J. Rybarcyk , James F. O'Hara , Eric R. Olivas , Thomas P. Wangler

A biased tunnel junction between a superconductor and a normal metal can cool the latter electrode. Based on a recently developed cooler with high power and superior performance, we have successfully integrated it with a dielectric silicon…

Mesoscale and Nanoscale Physics · Physics 2015-01-28 Hung Q. Nguyen , Matthias Meschke , Jukka P. Pekola

We describe the status of our effort to realize a first neutrino factory and the progress made in understanding the problems associated with the collection and cooling of muons towards that end. We summarize the physics that can be done…

High Energy Physics - Experiment · Physics 2009-09-29 M. M. Alsharo'a

Ionization cooling of a muon beam is a key technique for a Neutrino Factory or Muon Collider. An international collaboration is mounting an experiment to demonstrate muon ionization cooling at the Rutherford Appleton Laboratory. We aim to…

Accelerator Physics · Physics 2009-11-11 Daniel M. Kaplan

The presence of strong electron clouds in the quadrupole magnetic field regions of the Large Hadron Collider (LHC) leads to considerable heating that poses challenges for the cryogenic cooling system, and under certain conditions to proton…

Collimation systems in particle accelerators are designed to safely and efficiently dispose of unavoidable beam losses during operation. Their specific roles vary depending on the type of accelerator. The state of the art in hadron beam…

Accelerator Physics · Physics 2025-11-06 Stefano Redaelli

A water-based cooling system is being investigated to meet the cooling requirement of the Gas Electron Multiplier (GEM) based Muon Chamber (MuCh) detector system of the Compressed Baryonic Matter (CBM) experiment at GSI, Germany. The system…

We describe a helium evaporation refrigerator used to cool dynamically polarized proton and deuteron targets for electron-scattering experiments using the CEBAF Large Acceptance Spectrometer CLAS12 at Jefferson Lab. The geometry of the…

The Compact Muon Solenoid Collaboration is designing a new high-granularity endcap calorimeter, HGCAL, to be installed later this decade. As part of this development work, a prototype system was built, with an electromagnetic section…

Instrumentation and Detectors · Physics 2022-05-25 B. Acar , G. Adamov , C. Adloff , S. Afanasiev , N. Akchurin , B. Akgün , F. Alam Khan , M. Alhusseini , J. Alison , A. Alpana , G. Altopp , M. Alyari , S. An , S. Anagul , I. Andreev , P. Aspell , I. O. Atakisi , O. Bach , A. Baden , G. Bakas , A. Bakshi , S. Bannerjee , P. Bargassa , D. Barney , F. Beaudette , F. Beaujean , E. Becheva , A. Becker , P. Behera , A. Belloni , T. Bergauer , M. Besancon , S. Bhattacharya , D. Bhowmik , B. Bilki , P. Bloch , A. Bodek , M. Bonanomi , A. Bonnemaison , S. Bonomally , J. Borg , F. Bouyjou , N. Bower , D. Braga , J. Brashear , E. Brondolin , P. Bryant , A. Buchot Perraguin , J. Bueghly , B. Burkle , A. Butler-Nalin , O. Bychkova , S. Callier , D. Calvet , X. Cao , A. Cappati , B. Caraway , S. Caregari , A. Cauchois , L. Ceard , Y. C. Cekmecelioglu , S. Cerci , G. Cerminara , M. Chadeeva , N. Charitonidis , R. Chatterjee , Y. M. Chen , Z. Chen , H. J. Cheng , K. y. Cheng , S. Chernichenko , H. Cheung , C. H. Chien , S. Choudhury , D. Čoko , G. Collura , F. Couderc , M. Danilov , D. Dannheim , W. Daoud , P. Dauncey , A. David , G. Davies , O. Davignon , E. Day , P. DeBarbaro , F. De Guio , C. de La Taille , M. De Silva , P. Debbins , M. M. Defranchis , E. Delagnes , J. M. Deltoro Berrio , G. Derylo , P. G. Dias de Almeida , D. Diaz , P. Dinaucourt , J. Dittmann , M. Dragicevic , S. Dugad , F. Dulucq , I. Dumanoglu , V. Dutta , S. Dutta , M. Dünser , J. Eckdahl , T. K. Edberg , M. El Berni , F. Elias , S. C. Eno , Yu. Ershov , P. Everaerts , S. Extier , F. Fahim , C. Fallon , G. Fedi , B. A. Fontana Santos Alves , E. Frahm , G. Franzoni , J. Freeman , T. French , P. Gandhi , S. Ganjour , X. Gao , A. Garcia-Bellido , F. Gastaldi , Z. Gecse , Y. Geerebaert , H. Gerwig , O. Gevin , S. Ghosh , A. Gilbert , W. Gilbert , K. Gill , C. Gingu , S. Gninenko , A. Golunov , I. Golutvin , T. Gonzalez , N. Gorbounov , L. Gouskos , A. B. Gray , Y. Gu , F. Guilloux , Y. Guler , E. Gülmez , J. Guo , E. Gurpinar Guler , M. Hammer , H. M. Hassanshahi , K. Hatakeyama , A. Heering , V. Hegde , U. Heintz , N. Hinton , J. Hirschauer , J. Hoff , W. -S. Hou , X. Hou , H. Hua , J. Incandela , A. Irshad , C. Isik , S. Jain , H. R. Jheng , U. Joshi , V. Kachanov , A. Kalinin , L. Kalipoliti , A. Kaminskiy , A. Kapoor , O. Kara , A. Karneyeu , M. Kaya , O. Kaya , A. Kayis Topaksu , A. Khukhunaishvili , J. Kiesler , M. Kilpatrick , S. Kim , K. Koetz , T. Kolberg , O. K. Köseyan , A. Kristić , M. Krohn , K. Krüger , N. Kulagin , S. Kulis , S. Kunori , C. M. Kuo , V. Kuryatkov , S. Kyre , Y. Lai , K. Lamichhane , G. Landsberg , C. Lange , J. Langford , M. Y. Lee , A. Levin , A. Li , B. Li , J. H. Li , Y. y. Li , H. Liao , D. Lincoln , L. Linssen , R. Lipton , Y. Liu , A. Lobanov , R. -S. Lu , M. Lupi , I. Lysova , A. -M. Magnan , F. Magniette , A. Mahjoub , A. A. Maier , A. Malakhov , S. Mallios , I. Mandjavize , M. Mannelli , J. Mans , A. Marchioro , A. Martelli , G. Martinez , P. Masterson , B. Meng , T. Mengke , A. Mestvirishvili , I. Mirza , S. Moccia , G. B. Mohanty , F. Monti , I. Morrissey , S. Murthy , J. Musić , Y. Musienko , S. Nabili , A. Nagar , M. Nguyen , A. Nikitenko , D. Noonan , M. Noy , K. Nurdan , C. Ochando , B. Odegard , N. Odell , H. Okawa , Y. Onel , W. Ortez , J. Ozegović , S. Ozkorucuklu , E. Paganis , D. Pagenkopf , V. Palladino , S. Pandey , F. Pantaleo , C. Papageorgakis , I. Papakrivopoulos , J. Parshook , N. Pastika , M. Paulini , P. Paulitsch , T. Peltola , R. Pereira Gomes , H. Perkins , P. Petiot , T. Pierre-Emile , F. Pitters , E. Popova , H. Prosper , M. Prvan , I. Puljak , H. Qu , T. Quast , R. Quinn , M. Quinnan , M. T. Ramos Garcia , K. K. Rao , K. Rapacz , L. Raux , G. Reichenbach , M. Reinecke , M. Revering , A. Roberts , T. Romanteau , A. Rose , M. Rovere , A. Roy , P. Rubinov , R. Rusack , V. Rusinov , V. Ryjov , O. M. Sahin , R. Salerno , A. M. Sanchez Rodriguez , R. Saradhy , T. Sarkar , M. A. Sarkisla , J. B. Sauvan , I. Schmidt , M. Schmitt , E. Scott , C. Seez , F. Sefkow , S. Sharma , I. Shein , A. Shenai , R. Shukla , E. Sicking , P. Sieberer , P. Silva , A. E. Simsek , Y. Sirois , V. Smirnov , U. Sozbilir , E. Spencer , A. Steen , J. Strait , N. Strobbe , J. W. Su , E. Sukhov , L. Sun , D. Sunar Cerci , C. Syal , B. Tali , C. L. Tan , J. Tao , I. Tastan , T. Tatli , R. Thaus , S. Tekten , D. Thienpont , E. Tiras , M. Titov , D. Tlisov , U. G. Tok , J. Troska , L. -S. Tsai , Z. Tsamalaidze , G. Tsipolitis , A. Tsirou , N. Tyurin , S. Undleeb , D. Urbanski , V. Ustinov , A. Uzunian , M. Van de Klundert , J. Varela , M. Velasco , O. Viazlo , M. Vicente Barreto Pinto , P. Vichoudis T. Virdee , R. Vizinho de Oliveira , J. Voelker , E. Voirin , M. Vojinovic , A. Wade , C. Wang , F. Wang , X. Wang , Z. Wang , Z. Wang , M. Wayne , S. N. Webb , A. Whitbeck , D. White , R. Wickwire , J. S. Wilson , D. Winter , H. y. Wu , L. Wu , M. Wulansatiti Nursanto , C. H Yeh , R. Yohay , D. Yu , G. B. Yu , S. S. Yu , C. Yuan , F. Yumiceva , I. Yusuff , A. Zacharopoulou , N. Zamiatin , A. Zarubin , S. Zenz , A. Zghiche , H. Zhang , J. Zhang , Y. Zhang , Z. Zhang

In order to develop an RF cavity that is applicable for a muon beam cooling channel, a new facility, called Mucool Test Area (MTA) has been built at Fermilab. MTA is a unique facility whose purpose is to test RF cavities in various…

Accelerator Physics · Physics 2019-08-15 Katsuya Yonehara

Muon ionization cooling provides the only practical solution for preparing high brightness beams necessary for a neutrino factory or muon collider. The Muon Ionization Cooling Experiment (MICE) is under development at the Rutherford…

Instrumentation and Detectors · Physics 2009-10-20 L. Coney

To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized proton operation in the Relativistic Heavy Ion Collider (RHIC), we will introduce a low-energy DC electron beam into each ring to collide…

Accelerator Physics · Physics 2014-10-22 Y. Luo , W. Fischer , N. P. Abreu , X. Gu , A. Pikin , G. Robert-Demolaize
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