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Related papers: High Intensity Secondary Beams Driven by Protons

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The Gamma Factory initiative proposes to develop novel research tools at CERN by producing, accelerating and storing highly relativistic, partially stripped ion beams in the SPS and LHC storage rings. By exciting the electronic degrees of…

During the workshop "Compton Scattering off Protons and Light Nuclei: pinning down the nucleon polarisabilities" (ECT*, Trento, Italy, 29 July -- 2 August 2013, http://www.ectstar.eu/node/98), recent developments had been reviewed in…

Purpose: The purpose of this work was to provide a flexible platform for FLASH research with protons by adapting a former clinical pencil beam scanning gantry to irradiations with ultrahigh dose rates. Methods: PSI Gantry 1 treated patients…

This document describes the design of the accelerator and target systems for the AGS Super Neutrino Beam Facility. Under the direction of the Associate Laboratory Director Tom Kirk, BNL has established a Neutrino Working Group to explore…

High Energy Physics - Experiment · Physics 2007-05-23 M. Diwan

The opportunities which are offered by a next generation and multi-purpose fixed-target experiment exploiting the proton and lead LHC beams extracted by a bent crystal are outlined. In particular, such an experiment can greatly complement…

The intensity of charged particle beams at Fermilab must be kept within pre-determined safety and operational envelopes in part by assuring all beam within a few percent has been transported from any source to destination. Beam intensity…

Accelerator Physics · Physics 2012-09-25 J. Crisp , B. Fellenz , J. Fitzgerald , D. Heikkinen , M. A. Ibrahim

The feasibility of a European next-generation very massive neutrino observatory in seven potential candidate sites located at distances from CERN ranging from 130 km to 2300 km, is being considered within the LAGUNA design study. The study…

High Energy Physics - Phenomenology · Physics 2010-03-10 A. Rubbia

The AWAKE project at CERN uses a self-modulated \SI{400}{GeV/c} proton bunch to drive GV/m wakefields in a \SI{10}{m} long plasma with an electron density of $n_{pe} = 7 \times 10^{14}\,\rm{electrons/cm}^3$. We present the upgrade of a…

Accelerator Physics · Physics 2018-10-05 M. Turner , V. Clerc , I. Gorgisyan , E. Gschwendtner , S. Mazzoni , A. Petrenko

The next generation of high-energy physics experiments requires high intensity protons in the multi-GeV energy range for efficient production of secondary beams. The Fermilab long-term future requires an 8 GeV proton source to feed the Main…

Accelerator Physics · Physics 2012-03-09 L. Jenner , C. Johnstone , D. Neuffer , J. Pasternak

We have commenced experiments with intense short pulses of ion beams on the Neutralized Drift Compression Experiment-II at Lawrence Berkeley National Laboratory, by generating beam spots size with radius r < 1 mm within 2 ns FWHM and…

The Electron-Ion Collider is under construction at BNL. It will have high-energy high-intensity polarized beams of electrons and hadrons. These beams will allow a high accuracy investigation of nucleon structure in the low- to very-low-x…

Nuclear Experiment · Physics 2024-06-18 B. Wojtsekhowski

Extreme beams of charged particles and photons, reaching ultrahigh densities or producing intense gamma-ray bursts, are central to accelerator physics, laboratory astrophysics, and strong-field quantum electrodynamics research. Yet their…

A timely and long-term programme of kaon decay measurements at a new level of precision is presented, leveraging the capabilities of the CERN Super Proton Synchrotron (SPS). The proposed programme is firmly anchored on the experience built…

High Energy Physics - Experiment · Physics 2022-12-01 E. Cortina Gil , J. Jerhot , N. Lurkin , T. Numao , B. Velghe , V. W. S. Wong , D. Bryman , L. Bician , Z. Hives , T. Husek , K. Kampf , M. Koval , A. T. Akmete , R. Aliberti , V. Büscher , L. Di Lella , N. Doble , L. Peruzzo , M. Schott , H. Wahl , R. Wanke , B. Döbrich , L. Montalto , D. Rinaldi , F. Dettori , A. Cardini , A. Lai , L. Bomben , S. Carsi , M. Prest , A. Selmi , G. Lezzani , P. Monti-Guarnieri , L. Perna , P. Dalpiaz , V. Guidi , A. Mazzolari , I. Neri , F. Petrucci , M. Soldani , L. Bandiera , A. Cotta Ramusino , A. Gianoli , M. Romagnoni , A. Sytov , M. Lenti , I. Panichi , G. Ruggiero , A. Bizzeti , F. Bucci , A. Antonelli , E. Di Meco , G. Lanfranchi , S. Martellotti , M. Martini , M. Moulson , D. Paesani , I. Sarra , T. Spadaro , G. Tinti , E. Vallazza , F. Ambrosino , R. Giordano , P. Massarotti , M. Napolitano , G. Saracino , C. Di Donato , G. D'Ambrosio , M. D'Errico , M. Mirra , S. Neshatpour , R. Fiorenza , I. Rosa , D. De Salvador , F. Sgarbossa , G. Anzivino , S. Germani , R. Volpe , P. Cenci , S. Cutini , V. Duk , P. Lubrano , M. Pepe , M. Piccini , F. Costantini , S. Donati , M. Giorgi , S. Giudici , G. Lamanna , E. Pedreschi , J. Pinzino , M. Sozzi , R. Fantechi , V. Giusti , F. Spinella , I. Mannelli , M. Raggi , A. Biagioni , P. Cretaro , O. Frezza , F. Lo Cicero , A. Lonardo , M. Turisini , P. Vicini , R. Ammendola , V. Bonaiuto , A. Fucci , A. Salamon , F. Sargeni , R. Arcidiacono , B. Bloch-Devaux , E. Menichetti , E. Migliore , C. Biino , F. Marchetto , D. Baigarashev , Y. Kambar , D. Kereibay , Y. Mukhamejanov , S. Sakhiyev , A. Briano Olvera , J. Engelfried , N. Estrada-Tristan , R. Piandani , M. A. Reyes Santos , K. A. Rodriguez Rivera , P. C. Boboc , A. M. Bragadireanu , S. A. Ghinescu , O. E. Hutanu , T. Blazek , V. Cerny , A. Kleimenova , Z. Kucerova , D. Martinez Santos , C. Prouve , M. Boretto , F. Brizioli , A. Ceccucci , M. Corvino , H. Danielsson , F. Duval , E. Gamberini , R. Guida , E. B. Holzer , B. Jenninger , G. Lehmann Miotto , P. Lichard , K. Massri , E. Minucci , M. Perrin-Terrin , V. Ryjov , J. Swallow , M. Van Dijk , M. Zamkovsky , R. Marchevski , A. Gerbershagen , J. R. Fry , F. Gonnella , E. Goudzovski , J. Henshaw , C. Kenworthy , C. Lazzeroni , C. Parkinson , A. Romano , J. Sanders , A. Shaikhiev , A. Tomczak , H. Heath , D. Britton , A. Norton , D. Protopopescu , J. B. Dainton , R. W. L. Jones , A. De Santo , F. Salvatore , P. Cooper , D. Coward , P. Rubin

The TOP-IMPLART project consists of the design and implementation of a linear proton accelerator, its control and monitoring systems for the treatment of superficial and semi-deep tumors. The energy of 150 MeV (corresponding to a…

Radiation-hard ionization chambers were tested using an intense electron beam from the accelerator test facility (ATF) at the Brookhaven National Laboratory (BNL). The detectors were designed to be used as the basic element for monitoring…

Instrumentation and Detectors · Physics 2009-11-07 J. McDonald , D. Naples , C. Velissaris , A. Erwin , H. Ping , B. Viren , M. Diwan

European perspectives are discussed on fixed-target electron or positron scattering experiments using polarized and unpolarized beams and targets in various combinations. The goal envisioned is a deep and complete understanding of the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Wolf-Dieter Nowak

Crossing a horizontal nonlinear resonance is the approach that can be used to split a beam in several beamlets with the goal to perform multi-turn extraction from a circular particle accelerator. Such an approach has been successfully…

Accelerator Physics · Physics 2022-11-29 G. Russo , F. Cerutti , L. S. Esposito , G. Franchetti , M. Giovannozzi , J. R. Hunt , A. Huschauer

A proton irradiation site for silicon detectors has been developed and commissioned at the Bonn Isochronous Cyclotron. The accelerator provides 14 MeV proton beams of up to 1 $\mu$A at beam widths of a few mm to the setup. Devices Under…

Instrumentation and Detectors · Physics 2024-05-07 Pascal Wolf , Dennis Sauerland , Reinhard Beck , Jochen Dingfelder

The variety of beams, needed to set-up in the injectors as requested in the LHC, are reviewed, in terms of priority but also performance expectations and reach during 2015. This includes the single bunch beams for machine commissioning and…

Accelerator Physics · Physics 2014-12-30 Y. Papaphilippou , H. Bartosik , G. Rumolo , D. Manglunki

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental program at the next generation of lepton accelerators. In the context of the Hadronic Physics program at the Jefferson Laboratory…

Nuclear Experiment · Physics 2019-06-25 A. Afanasev , I. Albayrak , S. Ali , M. Amaryan , A. D'Angelo , J. Annand , J. Arrington , A. Asaturyan , H. Avakian , T. Averett , L. Barion , M. Battaglieri , V. Bellini , V. Berdnikov , J. Bernauer , A. Biselli , M. Boer , M. Bondì , K. -T. Brinkmann , B. Briscoe , V. Burkert , A. Camsonne , T. Cao , L. Cardman , M. Carmignotto , L. Causse , A. Celentano , P. Chatagnon , G. Ciullo , M. Contalbrigo , D. Day , M. Defurne , S. Diehl , B. Dongwi , R. Dupré , D. Dutta , M. Ehrhart , L. Elouadrhiri , R. Ent , I. Fernando , A. Filippi , Y. Furletova , H. Gao , A. Gasparian , D. Gaskell , F. Georges , F. -X. Girod , J. Grames , C. Gu , M. Guidal , D. Hamilton , D. Hasell , D. Higinbotham , M. Hoballah , T. Horn , C. Hyde , A. Italiano , N. Kalantarians , G. Kalicy , D. Keller , C. Keppel , M. Kerver , P. King , E. Kinney , H. -S. Ko , M. Kohl , V. Kubarovsky , L. Lanza , P. Lenisa , N. Liyanage , S. Liuti , J. Mamei , D. Marchand , P. Markowitz , L. Marsicano , M. Mazouz , M. McCaughan , B. McKinnon , M. Mihovilovič , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , C. Muñoz Camacho , P. Nadel-Turońs , M. De Napoli , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , L. Pappalardo , R. Paremuzyan , E. Pasyuk , T. Patel , I. Pegg , D. Perera , A. Puckett , N. Randazzo , M. Rashad , M. Rathnayake , A. Rizzo , J. Roche , O. Rondon , A. Schmidt , M. Shabestari , Y. Sharabian , S. Širca , D. Sokhan , A. Somov , N. Sparveris , S. Stepanyan , I. Strakovsky , V. Tadevosyan , M. Tiefenback , R. Trotta , R. De Vita , H. Voskanyan , E. Voutier , R. Wang , B. Wojtsekhowski , S. Wood , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhao , X. Zheng , C. Zorn
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