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Muon accelerators offer an attractive option for a range of future particle physics experiments. They can enable high energy (TeV+) high energy lepton colliders whilst mitigating the difficulty of synchrotron losses, and can provide intense…

To achieve the true diffraction-limited emittance of a storage ring light source, such as ~10 pm.rad for medium-energy electron beams, within a limited circumference, it is generally necessary to increase the number of bending magnets in a…

Accelerator Physics · Physics 2023-08-22 Zhiliang Ren , Zhenghe Bai , Penghui Yang , Lin Wang , Hongliang Xu

A 3.9 GHz deflecting mode (pi, TM110) cavity has been long used for six-dimensional phase-space beam manipulation tests at the A0 Photo-Injector Lab (16 MeV) in Fermilab and their extended applications with vacuum cryomodules are currently…

Accelerator Physics · Physics 2014-09-19 Young-Min Shin , Michael Church

The multi-MW target proposed for the EURISOL facility will be based on fission of uranium (or thorium) compounds to produce rare isotopes far from stability. A two-step process is used for the isotope production. First, neutrons are…

Accelerator Physics · Physics 2007-05-23 M. Felcini , A. Herrera-Martinez , Y. Kadi , T. Otto , L. Tecchio

A portion of the Muon g-2 Storage Ring electric system, which provides vertical beam focusing, exhibited an unexpected time dependence that produced a characteristic evolution of the stored beam during Run-1 of the Muon g-2 Experiment at…

In an antiproton production (Pbar) target station of the Fermi National Accelerator Laboratory (FNAL), the secondary particles produced by bombarding a target with 120-GeV protons are shielded by a thick iron shield. In order to obtain…

We theoretically and computationally investigate the cooling of antihydrogen, $\bar{H}$, using optical molasses cooling. This updates the results in Ref. [1] to the current capabilities of the ALPHA experiment. Through Monte Carlo…

Atomic Physics · Physics 2025-02-11 Spencer J. Walsh , C. Ø. Rasmussen , F. Robicheaux

A staged approach towards muon based facilities for Intensity and Energy Frontier science, building upon existing and proposed facilities at Fermilab, is presented. At each stage, a facility exploring new physics also provides an R&D…

The ICARUS-T600 Liquid Argon Time Projection Chamber is operating at Fermilab at shallow depth and thus exposed to a high flux of cosmic rays that can fake neutrino interactions. A cosmic ray tagging (CRT) system ($\sim$1100 m$^2$),…

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

An interlock system has been designed for the Fermilab Cryo-module Test Stand (CMTS), a test bed for the cryomodules to be used in the upcoming Linac Coherent Light Source 2 (LCLS-II) project at SLAC. The interlock system features 8…

Accelerator Physics · Physics 2017-05-02 T. Petersen , J. S. Diamond , D. McDowell , D. Nicklaus , P. S. Prieto , A. Semenov

MALTA2 is the latest full-scale prototype of the MALTA family of Depleted Monolithic Active Pixel Sensors (DMAPS) produced in Tower Semiconductor 180 nm CMOS technology. In order to comply with the requirements of High Energy Physics (HEP)…

We built a test stand for evaluating the performance of the thermionic electron sources for the electron lens project at the Integrable Optics Test Accelerator (IOTA) in Fermilab. The lens will be used to study nonlinear dynamics and…

Accelerator Physics · Physics 2023-07-06 S. Kladov , M. Bossard , J. Brandt , Y-K. Kim , N. Banerjee , G. Stancari , B. Cathey , S. Nagaitsev

Fermi National Accelerator Laboratory is constructing an Advanced Accelerator Research and Development facility at New Muon Lab. The cryogenic infrastructure in support of the initial phase of the facility consists of two Tevatron style…

Accelerator Physics · Physics 2012-09-13 A. Martinez , A. L. Klebaner , J. C. Theilacker , B. D. DeGraff , M. White , G. S. Johnson

The Mu2e experiment at Fermilab will search for Charged Lepton Flavor Violating conversion of a muon to an electron in an atomic field. The Mu2e detector is composed of a tracker, an electromagnetic calorimeter and an external system,…

The Mu2e experiment at Fermilab will search for the coherent $\mu \to e$ conversion on aluminum atoms. The detector system consists of a straw tube tracker and a crystal calorimeter. A pre-production of 150 Silicon Photomultiplier arrays…

Fast muon beam six dimensional (6D) phase space cooling is essential for muon colliders. The Helical Cooling Channel (HCC) uses hydrogen-pressurized RF cavities imbedded in a magnet system with solenoid, helical dipole, and helical…

Accelerator Physics · Physics 2012-02-06 K. Yonehara , R. P. Johnson , Y. S. Derbenev

LQXFA/B production series cryogenic assemblies are being built for the LHC upgrade by the HL-LHC Accelerator Upgrade Project (AUP). These contain a pair of MQXFA quadrupole magnets combined as a cold mass within a vacuum vessel, and are to…

Recent discovery of a Higgs boson boosted interest in a low-energy medium-luminosity Muon Collider as a Higgs Factory (HF). A preliminary design of the HF storage ring (SR) is based on cos-theta Nb3Sn superconducting (SC) magnets with the…

We report the test of many of the key elements of the laser-based calibration system for muon g - 2 experiment E989 at Fermilab. The test was performed at the Laboratori Nazionali di Frascati's Beam Test Facility using a 450 MeV electron…