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The intense muon beams which will be available at a neutrino factory provide a unique opportunity for searching for physics beyond the standard model, both in lepton flavor violation and in the search for a permanent electric dipole moment…

High Energy Physics - Experiment · Physics 2009-11-11 B. Lee Roberts , Marco Grassi , Akira Sato

After the demonstration of the feasibility of hypernuclear spectroscopy with heavy-ion beams, the HypHI Collaboration will next focus on the study of proton- and neutron-rich hypernuclei. The use of a fragment separator for the production…

Nuclear Experiment · Physics 2016-11-02 C. Rappold , J. F. López Fidalgo

This whitepaper summarizes and the state of the field of high-power cyclotrons and FFAs as discussed by international experts during a three-day workshop of the same name. The workshop was held online from Sep 7 to Sep 9, 2021 as part of…

The next generation of lepton flavor violation experiments need high intensity and high quality muon beams. Production of such beams requires sending a short, high intensity proton pulse to the pion production target, capturing pions and…

Hadrontherapy is an emerging technique in cancer therapy that uses beams of charged particles. To meet the improved capability of hadrontherapy in matching the dose release with the cancer position, new dose monitoring techniques need to be…

The radiation hardened beam instrumentations workshop was held on February 3rd and 4th, 2022 to identify the technological challenges on the beam instrumentation for multi-Mega-Watt (MW) beam facilities. We invited a speaker from a high…

Accelerator Physics · Physics 2022-03-14 Katsuya Yonehara

The scheduled High Luminosity upgrade of the CERN Large Hadron Collider presents new challenges in terms of radiation hardness. As a consequence, campaigns to qualify the radiation hardness of detector sensors and components are undertaken…

The next generation of accelerators for Megawatt proton and heavy-ion beams moves us into a completely new domain of extreme specific energies of up to 0.1 MJ/g (Megajoule/gram) and specific power up to 1 TW/g (Terawatt/gram) in beam…

Accelerator Physics · Physics 2014-09-02 N. V. Mokhov , S. R. Childress , A. I. Drozhdin , V. S. Pronskikh , D. Reitzner , I. S. Tropin , K. Vaziri

Due to the potentially adverse effects of the generation of halo particles in intense proton beams, it is imperative to have a clear understanding of the mechanisms that can lead to halo formation for current and proposed high- intensity…

The Search for Hidden Particles (SHiP) Collaboration has shown that the CERN SPS accelerator with its 400 $\mathrm{\small GeV/c}$ proton beam offers a unique opportunity to explore the Hidden Sector. The proposed experiment is an intensity…

Instrumentation and Detectors · Physics 2019-05-01 SHiP Collaboration

Ion beam analysis techniques are among the most powerful tools for advanced material characterization. Despite their growing relevance in a widening number of fields, most ion beam analysis facilities still rely on the oldest accelerator…

Plasma Physics · Physics 2019-03-06 Matteo Passoni , Luca Fedeli , Francesco Mirani

The theoretical and experimental aspects of particle production from the strong equivalent photon fluxes present at high energy hadron colliders are reviewed. The goal is to show how photons at hadron colliders can improve what we have…

High Energy Physics - Phenomenology · Physics 2010-01-27 Joakim Nystrand

Project X is a high intensity proton facility that will support a world-leading Intensity Frontier research program over the next several decades at Fermilab. When compared to other facilities in the planning stages elsewhere in the world…

Accelerator Physics · Physics 2013-06-24 Stephen Holmes , Sergei Nagaitsev , Robert Tschirhart

These reports present the results of the 2013 Community Summer Study of the APS Division of Particles and Fields ("Snowmass 2013") on the future program of particle physics in the U.S. Chapter 8, on the Instrumentation Frontier, discusses…

High Energy Physics - Experiment · Physics 2014-01-24 M. Demarteau , R. Lipton , H. Nicholson , I. Shipsey , D. Akerib , A. Albayrak-Yetkin , J. Alexander , J. Anderson , M. Artuso , D. Asner , R. Ball , M. Battaglia , C. Bebek , J. Beene , Y. Benhammou , E. Bentefour , M. Bergevin , A. Bernstein , B. Bilki , E. Blucher , G. Bolla , D. Bortoletto , N. Bowden , G. Brooijmans , K. Byrum , B. Cabrera , G. Cancelo , J. Carlstrom , B. Casey , C. Chang , J. Chapman , C. H. Chen , I. Childres , D. Christian , M. Convery , W. Cooper J. Corso , J. Cumalat , P. Cushman , C. Da Via , S. Dazeley , P. Debbins , G. Deptuch , S. Dhawan , V. Di Benedetto , B. DiGiovene , Z. Djurcic , S. Dye , A. Elagin , J. Estrada , H. Evans , E. Etzion , J. Fast , C. Ferretti , P. Fisher , B. Fleming , K. Francis , P. Friedman , H. Frisch , M. Garcia-Sciveres , C. Gatto , G. Geronim , G. Gilchriese , S. Golwala , C. Grant , A. Grillo , E. Grünendahl , P. Gorham , L. Guan , G. Gutierrez , C. Haber , J. Hall , G. Haller , C. Hast , U. Heintz , T. Hemmick , D. G. Hitlin , C. Hogan , M. Hohlmann , E. Hoppe , L. Hsu , M. Huffer , K. Irwin , F. Izraelevitch , G. Jennings , M. Johnson , A. Jung , H. Kagan , C. Kenney , S. Kettell , R. Khanna , V. Khristenko , F. Krennrich , K. Kuehn , R. Kutschke , J. Learned , A. T. Lee , D. Levin , T. Liu , A. T. K. Liu , D. Lissauer , J. Love , D. Lynn , D. MacFarlane , S. Magill , S. Majewski , J. Mans , J. Maricic , P. Marleau , A. Mazzacane , D. McKinsey , J. Mehl , A. Mestvirisvilli , S. Meyer , N. Mokhov , M. Moshe , A. Mukherjee , P. Murat , S. Nahn , M. Narain , P. Nadel-Turonski , M. Newcomer , K. Nishimura , D. Nygren , E. Oberla , Y. Onel , M. Oreglia , J. Orrell , J. Paley , A. Para , S. Parker , V. Polychronakos , S. Pordes , P. Privitera , A. Prosser , M. Pyle , J. Raaf , E. Ramberg , R. Rameika , B. Rebel , J. Repond , D. Reyna , L. Ristori , R. Rivera , A. Ronzhin , R. Rusack , J. Russ , A. Ryd , H. Sadrozinski , H. Sahoo , M. C. Sanchez , C. Sanzeni , S. Schnetzer , S. Seidel , A. Seiden , I. Schmidt , A. Shenai , T. Shutt , Y. Silver , W. Smith , D. Snowden-Ifft , A. Sonnenschein , D. Southwick , L. Spiegel , M. Stanitzki , S. Striganov , D. Su , R. Sumner , R. Svoboda , M. Sweany , R. Talaga , R. Tayloe , S. Tentindo , N. Terentiev , J. Thom-Levy , C. Thorn , J. Tiffenberg , W. Trischuk , R. Tschirhart , M. Turner , D. Underwood , L. Uplegger , J. Urheim , M. Vagins , K. Van Bibber , G. Varner , R. Varner , J. Va'vra , H. Von der Lippe , R. Wagner , S. Wagner , C. Weaverdyck , H. Wenzel , A. Weinstein , M. Wetstein , A. White , R. Wigman , P. Wilson , D. Winn , P. Winter , C. Woody , L. Xia , J. Q. Xie , Z. Ye , M. F. Yeh , T. Yetkin , J. H. Yoo , J. Yu , J. M. Yu , S. Zeller , J. L. Zhang , J. J. Zhu , B. Zhou , R. Y. Zhu , B. Zitzer

Proton Induced X-ray Emission (PIXE) using high energy protons is a non destructive multi elemental technique that can analyze medium and heavy trace elements on thick samples. A new experimental setup is being built at the ARRONAX facility…

Nuclear Experiment · Physics 2010-11-18 C. Koumeir , F. Haddad , V. Metivier , N. Servagent , N. Michel

The Fermilab Proton Source machines, constituted by Pre-Injector, conventional Linac and Booster synchrotron, at Fermi National Accelerator Laboratory (Fermilab) had have a long history of successful beam operations. Built in late '60s, the…

Accelerator Physics · Physics 2014-09-01 F. G. Garcia , W. Pellico

With new forthcoming intense neutrino beams, for the study of neutrino oscillations, it is possible to consider other physics experiments that can be done with these extreme neutrino fluxes available close to the source.

High Energy Physics - Experiment · Physics 2009-10-31 N. Solomey

In nuclear and atomic physics experiments, charged ion beams often need to be guided from the ion production to the experimental site. In the PUMA experiment, an ion source beamline was developed, which can be operated with up to…