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In the next decade the Fermilab Muon Campus will host two world class experiments dedicated to the search for signals of new physics. The Muon g-2 experiment will determine with unprecedented precision the anomalous magnetic moment of the…

Accelerator Physics · Physics 2017-09-18 D. Stratakis

The LCLS-II HE superconducting linac can produce multi-energy beams by supporting multiple undulator lines simultaneously. This could be achieved by using the cavity SRF tuner in the off-frequency detune mode. This off-frequency operation…

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. First stage of the Project-X consists of superconducting linac which will be operated in continuous wave (CW) mode to accelerate the beam from 2.5 MeV to…

Accelerator Physics · Physics 2012-03-08 A. Saini , K. Ranjan , N. Solyak , S. Mishra , V. Yakovlev

The aim of the FAMU experiment is to realize the first measurement of the hyperfine splitting (hfs) in the 1S state of muonic hydrogen $\Delta E^{hfs}_{1S}$, by using the RIKEN-RAL intense pulsed muon beam and a high-energy mid-infrared…

Instrumentation and Detectors · Physics 2018-11-20 FAMU collaboration

PIP-II is a superconducting linac that is in the initial acceleration chain for the Fermilab accelerator complex. The RF system consists of a warm front-end with an RFQ and buncher cavities along with 25 superconducting cryo-modules…

Accelerator Physics · Physics 2025-10-29 P. Varghese , S. Raman , M. Guran , L. Reyes , L. Doolittle , Q. Du , S. Murthy

The new g-2 experiment at Fermilab aims to measure the muon anomalous magnetic moment by a fourfold improvement in precision compared to the BNL experiment. Achieving this goal requires the delivery of highly polarized 3.094 GeV/c muons…

Cooling of hadron beams (including heavy-ions) is a powerful technique by which accelerator facilities around the world achieve the necessary beam brightness for their physics research. In this paper, we will give an overview of the latest…

Accelerator Physics · Physics 2009-09-29 L. R. Prost , P. Derwent

The potentially realizable beam power at the Fermilab long-baseline neutrino program has motivated a reinvigorated design and optimization effort for a rapid-cycling synchrotron (RCS) intensity upgrade of the Fermilab proton complex. We…

Accelerator Physics · Physics 2020-01-17 Jeffrey Eldred

A new high field spectrometer has been built to extend the capabilities of the $\beta$-detected nuclear magnetic resonance ($\beta$-NMR) facility at TRIUMF. This new beamline extension allows $\beta$-NMR spectroscopy to be performed with…

A single gap, 352 MHz superconducting reentrant cavity for 5-100 MeV beams has been designed and it is presently under construction. This development is being done in the framework of a 30 mA proton linac project for nuclear waste…

Accelerator Physics · Physics 2009-10-05 A. Facco , M. Pasini , V. Zviagintsev

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…

The Mu2e experiment at Fermilab is being designed to study the coherent neutrino-less conversion of a negative muon into an electron in the field of a nucleus. This process has an extremely low probability in the Standard Model, and its…

Accelerator Physics · Physics 2016-12-30 V. Pronskikh , D. Glenzinski , K. Knoepfel , N. Mokhov , R. Tschirhart

The Fermilab Booster uses multi-turn beam injection with all its cavities phased such that beam sees a net zero RF voltage even when each station is at the same maxi-mum voltage. During beam capture the RF voltage is increased slowly by…

The Mu2e experiment at Fermilab is being designed to study the coherent neutrino-less conversion of a negative muon into an electron in the field of a nucleus. This process has an extremely low probability in the Standard Model and its…

Accelerator Physics · Physics 2017-10-11 V. Pronskikh , D. Glenzinski , N. Mokhov , R. Tschirhart

Since the discovery of the muon, particle physicists have carried out a series of experiments aimed at measuring flavor violation in charged-lepton interactions. To date, no such violation has been observed. The Mu2e experiment at Fermilab…

Instrumentation and Detectors · Physics 2014-01-20 Robert Craig Group , Yuri Oksuzian

A possible application of the HTS (ReBCO) rapid-cycling dipole magnet [1] in the first stages of muon acceleration consisting of Recirculating Linear Accelerator (RLA) and followed-up first Rapid Cycling Synchrotron (RCS-1) is presented.…

Accelerator Physics · Physics 2025-09-19 Henryk Piekarz

We report a study of muon neutrino charged-current quasi-elastic events in the segmented scintillator inner tracker of the MINERvA experiment running in the NuMI neutrino beam at Fermilab. The events were selected by requiring a {\mu}^- and…

High Energy Physics - Experiment · Physics 2014-11-25 The MINERvA collaboration , G. A. Fiorentini , D. W. Schmitz , P. A. Rodrigues , L. Aliaga , O. Altinok , B. Baldin , A. Baumbaugh , A. Bodek , D. Boehnlein , S. Boyd , R. Bradford , W. K. Brooks , H. Budd , A. Butkevich , D. A. Martinez Caicedo , C. M. Castromonte , M. E. Christy , H. Chung , J. Chvojka , M. Clark , H. da Motta , D. S. Damiani , I. Danko , M. Datta , M. Day , R. DeMaat , J. Devan , E. Draeger , S. A. Dytman , G. A. Díaz , B. Eberly , D. A. Edmondson , J. Felix , T. Fitzpatrick , L. Fields , A. M. Gago , H. Gallagher , C. A. George , J. A. Gielata , C. Gingu , B. Gobbi , R. Gran , N. Grossman , J. Hanson , D. A. Harris , J. Heaton , A. Higuera , I. J. Howley , K. Hurtado , M. Jerkins , T. Kafka , J. Kaisen , M. O. Kanter , C. E. Keppel , J. Kilmer , M. Kordosky , A. H. Krajeski , S. A. Kulagin , T. Le , H. Lee , A. G. Leister , G. Locke , G. Maggi , E. Maher , S. Manly , W. A. Mann , C. M. Marshall , K. S. McFarland , C. L. McGivern , A. M. McGowan , A. Mislivec , J. G. Morfń , J. Mousseau , D. Naples , J. K. Nelson , G. Niculescu , I. Niculescu , N. Ochoa , C. D. O'Connor , J. Olsen , B. Osmanov , J. Osta , J. L. Palomino , V. Paolone , J. Park , C. E. Patrick , G. N. Perdue , C. Peña , L. Rakotondravohitra , R. D. Ransome , H. Ray , L. Ren , C. Rude , K. E. Sassin , H. Schellman , R. M. Schneider , E. C. Schulte , C. Simon , F. D. Snider , M. C. Snyder , J. T. Sobczyk , C. J. Solano Salinas , N. Tagg , W. Tan , B. G. Tice , G. Tzanakos , J. P. Velásquez , J. Walding , T. Walton , J. Wolcott , B. A. Wolthuis , N. Woodward , G. Zavala , H. B. Zeng , D. Zhang , L. Y. Zhu , B. P. Ziemer

A 2.1 MeV, 10 mA CW RFQ has been installed and commissioned at Fermilab's test accelerator known as PIP-II Injector Test. This report describes the measurements of the beam properties after acceleration in the RFQ, including the energy and…

Accelerator Physics · Physics 2017-09-25 A. Shemyakin , J. -P. Carneiro , B. Hanna , L. Prost , A. Saini , V. Scarpine , V. L. S. Sista , J. Steimel

The Mu2e Experiment at Fermilab will search for coherent, neutrinoless conversion of muons into electrons in the field of a nucleus, with a sensitivity improvement of a factor of 10^4 over previous experiments. Such a charged lepton…

Instrumentation and Detectors · Physics 2019-08-12 Raffaella Donghia

RF cavities used in modern particle accelerators operate in TM$_{m10}$-like modes composed of a single, dominant multipole of order $m$; $m=0$ modes are used for the longitudinal acceleration of a particle beam and $m\neq0$ modes for…

Accelerator Physics · Physics 2022-06-22 L. M. Wroe , S. L. Sheehy , R. J. Apsimon