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A portion of the remnant Tevatron program infrastructure at Fermilab is being reconfigured to be used for the generation and delivery of proton and muon beams for new high-precision particle physics experiments. With the 8 GeV Booster as…

Accelerator Physics · Physics 2016-12-23 J. A. Johnstone , M. J. Syphers

The Muon Ionization Cooling Experiment (MICE) is a strategic R&D project intended to demonstrate the only practical solution to providing high brilliance beams necessary for a neutrino factory or muon collider. MICE is under development at…

Accelerator Physics · Physics 2013-08-01 U. Bravar , M. Bogomilov , Y. Karadzhov , D. Kolev , I. Russinov , R. Tsenov , L. Wang , F. Y. Xu , S. X. Zheng , R. Bertoni , M. Bonesini , R. Mazza , V. Palladino , G. Cecchet , A. de Bari , M. Capponi , A. Iaciofano , D. Orestano , F. Pastore , L. Tortora , S. Ishimoto , S. Suzuki , K. Yoshimura , Y. Mori , Y. Kuno , H. Sakamoto , A. Sato , T. Yano , M. Yoshida , F. Filthaut , M. Vretenar , S. Ramberger , A. Blondel , F. Cadoux , F. Masciocchi , J. S. Graulich , V. Verguilov , H. Wisting , C. Petitjean , R. Seviour , M. Ellis , P. Kyberd , M. Littlefield , J. J. Nebrensky , D. Forrest , F. J. P. Soler , K. Walaron , P. Cooke , R. Gamet , A. Alecou , M. Apollonio , G. Barber , A. Dobbs , P. Dornan , A. Fish , R. Hare , A. Jamdagni , V. Kasey , M. Khaleeq , K. Long , J. Pasternak , H. Sakamoto , T. Sashalmi , V. Blackmore , J. Cobb , W. Lau , M. Rayner , C. D. Tunnell , H. Witte , S. Yang , J. Alexander , G. Charnley , S. Griffiths , B. Martlew , A. Moss , I. Mullacrane , A. Oats , S. York , R. Apsimon , R. J. Alexander , P. Barclay , D. E. Baynham , T. W. Bradshaw , M. Courthold , R. Edgecock T. Hayler , M. Hills , T. Jones , N. McCubbin , W. J. Murray , C. Nelson , A. Nicholls , P. R. Norton , C. Prior , J. H. Rochford , C. Rogers , W. Spensley , K. Tilley , C. N. Booth , P. Hodgson , R. Nicholson , E. Overton , M. Robinson , P. Smith , D. Adey , J. Back , S. Boyd , P. Harrison , J. Norem , A. D. Bross , S. Geer , A. Moretti , D. Neuffer , M. Popovic , Z. Qian , R. Raja , R. Stefanski , M. A. C. Cummings , T. J. Roberts , A. DeMello , M. A. Green , D. Li , A. M. Sessler , S. Virostek , M. S. Zisman , B. Freemire , P. Hanlet , D. Huang , G. Kafka , D. M. Kaplan , P. Snopok , Y. Torun , Y. Onel , D. Cline , K. Lee , Y. Fukui , X. Yang , R. A. Rimmer , L. M. Cremaldi , T. L. Hart , D. J. Summers , L. Coney , R. Fletcher , G. G. Hanson , C. Heidt , J. Gallardo , S. Kahn , H. Kirk , R. B. Palmer

A muon storage ring neutrino source uses an induction linac for muon capture, a 200 MHz copper cavity system for cooling, and 200 and 400 MHz superconducting rf systems for acceleration to a final energy of up to 50 GeV. These systems and…

Accelerator Physics · Physics 2009-08-17 David Neuffer

The muon-to-electron conversion (Mu2e) experiment at Fermilab will be used to search for the charged lepton flavor-violating conversion of muons to electrons in the field of an atomic nucleus. The Mu2e experiment is currently in the…

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

SRF cavities for particle acceleration are conventionally operated immersed in a bath of liquid helium at 4.2 K and below. Although this cooling configuration is practically and economically viable for large scientific accelerator…

Accelerator Physics · Physics 2022-07-13 R. C. Dhuley , S. Posen , M. I. Geelhoed , J. C. T. Thangaraj

The Muon-to-Electron (Mu2e) experiment at Fermilab, will seek the evidence of direct muon to electron conversion at the sensitivity level where it cannot be explained by the Standard Model. An 8-GeV 25-kW proton beam will be directed onto a…

Accelerator Physics · Physics 2012-02-20 V. S. Pronskikh , V. V. Kashikhin , N. V. Mokhov

ATLAS muon detector upgrades aim for increased acceptance for muon triggering and precision tracking and for improved rate capability of the muon chambers in the high-background regions of the detector with increasing LHC luminosity. The…

Instrumentation and Detectors · Physics 2017-03-08 Hubert Kroha , Oliver Kortner , Korbinian Schmidt-Sommerfeld , Eric Takasugi

Muon ionization cooling is the only practical method for preparing high-brilliance beams needed for a neutrino factory or muon collider. The muon ionization cooling experiment (MICE) under development at the Rutherford Appleton Laboratory…

Accelerator Physics · Physics 2008-10-11 Alan D. Bross , Daniel M. kaplan

The Mu2e experiment at Fermilab will search for the charged-lepton flavor-violating process of a neutrino less muon-to-electron decay in the presence of a nucleus. The experiment expects a single-event sensitivity of $2.9\times10^{-17}$,…

Instrumentation and Detectors · Physics 2019-10-03 Hannah Woodward

The Fermilab proton source is capable of providing 8 GeV protons for both the future long-baseline neutrino program (NuMI), and for a new program of low energy muon experiments. In particular, if the 8 GeV protons are rebunched and then…

Accelerator Physics · Physics 2007-05-23 C. Ankenbrandt , D. Bogert , F. DeJongh , S. Geer , D. McGinnis , D. Neuffer , M. Popovic , E. Prebys

We report on a feasibility study conducted at the ELBA facility at ELI Beamlines in 2025 to investigate the possible production of muons from high-energy electron beams generated by extended laser-plasma interactions in optically generated…

The European XFEL is a new research facility currently under construction at DESY in the Hamburg area in Germany. From 2015 on, it will generate extremely intense X-ray flashes that will be used by researchers from all over the world. The…

Accelerator Physics · Physics 2015-06-16 J. Schaffran , Y. Bozhko , B. Petersen , D. Meissner , M. Chorowski , J. Polinski

MICE is an experiment with a section of an ionization cooling channel and a muon beam. The muons will be produced by the decay of pions from a target dipping into the ISIS proton beam at Rutherford Appleton Laboratory (RAL). The channel…

Instrumentation and Detectors · Physics 2015-05-14 Terrence Lee Hart

I report on the progress of two new muon anomalous magnetic moment experiments, which are in advanced design and construction phases. The goal of Fermilab E989 is to reduce the experimental uncertainty of $a_\mu$ from Brookhaven E821 by a…

High Energy Physics - Experiment · Physics 2016-06-22 David W. Hertzog

This paper presents a setup capable of producing a high-flux continuous beam of cold rubidium atoms for cavity QED experiments in the regime of strong coupling. A 2 $D^+$ MOT, loaded by rubidium getters in a dry film coated vapor cell, fed…

Atomic Physics · Physics 2015-06-04 Basudev Roy , Michael Scholten

The international Muon Ionization Cooling Experiment (MICE), which is under construction at the Rutherford Appleton Laboratory (RAL), will demonstrate the principle of ionization cooling as a technique for the reduction of the phase-space…

Accelerator Physics · Physics 2015-06-04 MICE Collaboration

We experimentally and theoretically study the continuous accumulation of cold atoms from a magneto-optical trap (MOT) into a finite depth trap, consisting in a magnetic quadrupole trap dressed by a radiofrequency (RF) field. Chromium atoms…

The current program at Fermilab involves the construction of a new superconducting linear accelerator (LINAC) to replace the existing warm version. The new LINAC, together with other planned improvements, is in support of proton beam…

Accelerator Physics · Physics 2023-10-03 R. Thurman-Keup , T. Folan , M. Mwaniki , S. Sas-Pawlik

The central part of PIP-II program of upgrades pro-posed for the Fermilab injection complex is an 800 MeV, 2 mA, CW-compatible SRF linac. Acceleration in super-conducting cavities begins from a low energy of 2.1 MeV, so that the first…

Accelerator Physics · Physics 2019-12-09 A. Chen , R. Andrews , C. Baffes , D. Lambert , L. Prost , A. Shemyakin , T. Zuchnik