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Both the Energy Recovery Linac (ERL) and Free Electron laser (FEL) are considered to be candidates of the fourth generation light source. It is proposed to combine FEL into an ERL facility to integrate the advantages of both ERL and FEL,…

Accelerator Physics · Physics 2015-06-16 Xiao-Hao Cui , Yi Jiao , Jiu-Qing Wang , Shu-Hong Wang

High average current, transportable energy recovery linacs (ERLs) can be very attractive tools for a number of applications including next generation high-luminosity, compact light sources. Conventional ERLs are based on an electron beam…

Accelerator Physics · Physics 2017-12-05 I. V. Konoplev , K. Metodiev , A. J. Lancaster , G. Burt , R. Ainsworth , A. Seryi

We discuss a concept of a lower-energy version of the Large Hadron-electron Collider (LHeC), delivering electron-hadron collisions concurrently to the hadron-hadron collisions at the high-luminosity LHC at CERN. Assuming the use of a 20 GeV…

High Energy Physics - Experiment · Physics 2026-05-05 Kevin David J André , Laurent Forthomme , Bernhard Holzer , Krzysztof Piotrzkowski

In the past decade, the fourth-generation light source based on the combination of Energy Recovery Linac (ERL) and Free-Electron Laser (FEL) using superconducting linear accelerators has garnered significant attention. It holds immense…

Accelerator Physics · Physics 2024-10-24 Xiuji Chen , Zipeng Liu , Si Chen , Duan Gu , Xuan Huang , Houjun Qian , Dong Wang , Haixiao Deng

SLAC National Accelerator Laboratory is collaborating with Arizona State University to design a LLRF system towards the advancement of the ASU Compact X-ray Light Source (CXLS). The CXLS is a phased project to develop small brilliant x-ray…

Accelerator Physics · Physics 2019-10-02 A. Young , J. M. D Ewart , J. Frisch , B. Hong , T. Straumann , M. Weaver , C. Xu

Cornell's electron/positron storage ring (CESR) was modified over a series of accelerator shutdowns beginning in May 2008, which substantially improves its capability for research and development for particle accelerators. CESR's energy…

Accelerator Physics · Physics 2015-09-02 M. G. Billing

The Large Hadron electron Collider (LHeC) is a proposed future particle physics project colliding 60 GeV electrons from a six-pass recirculating energy-recovery linac (ERL) with 7 TeV protons stored in the LHC. The ERL technology allows for…

Accelerator Physics · Physics 2023-05-25 Najmeh Sadat Mirian , Elham Salehi , Frank Zimmermann

I present here a new ring-ring design of eRHIC, a polarized electron-ion collider based on RHIC at BNL. This alternate eRHIC design utilizes high repetition rate colliding beams and is likely able to deliver the performance to meet the…

Accelerator Physics · Physics 2015-02-27 Yuhong Zhang

In a multipass energy recovery linac (ERL), each cavity must regain all energy expended from beam acceleration during beam deceleration, and the beam should achieve specific energy targets during each loop that returns it to the linac. For…

To date, linear accelerators (linacs) as electron sources used to produce ionizing radiation for industrial purposes have been limited to less than 100 kW. When the electron beam is used directly, this is sufficient for most potential…

Accelerator Physics · Physics 2022-02-17 Thomas K. Kroc

The Large Hadron electron Collider (LHeC) is designed to move the field of deep inelastic scattering (DIS) to the energy and intensity frontier of particle physics. Exploiting energy recovery technology, it collides a novel, intense…

High Energy Physics - Experiment · Physics 2022-09-20 P. Agostini , H. Aksakal , S. Alekhin , P. P. Allport , N. Andari , K. D. J. Andre , D. Angal-Kalinin , S. Antusch , L. Aperio Bella , L. Apolinario , R. Apsimon , A. Apyan , G. Arduini , V. Ari , A. Armbruster , N. Armesto , B. Auchmann , K. Aulenbacher , G. Azuelos , S. Backovic , I. Bailey , S. Bailey , F. Balli , S. Behera , O. Behnke , I. Ben-Zvi , M. Benedikt , J. Bernauer , S. Bertolucci , S. S. Biswal , J. Blümlein , A. Bogacz , M. Bonvini , M. Boonekamp , F. Bordry , G. R. Boroun , L. Bottura , S. Bousson , A. O. Bouzas , C. Bracco , J. Bracinik , D. Britzger , S. J. Brodsky , C. Bruni , O. Brüning , H. Burkhardt , O. Cakir , R. Calaga , A. Caldwell , A. Calıskan , S. Camarda , N. C. Catalan-Lasheras , K. Cassou , J. Cepila , V. Cetinkaya , V. Chetvertkova , B. Cole , B. Coleppa , A. Cooper-Sarkar , E. Cormier , A. S. Cornell , R. Corsini , E. Cruz-Alaniz , J. Currie , D. Curtin , M. D'Onofrio , J. Dainton , E. Daly , A. Das , S. P. Das , L. Dassa , J. de Blas , L. Delle Rose , H. Denizli , K. S. Deshpande , D. Douglas , L. Duarte , K. Dupraz , S. Dutta , A. V. Efremov , R. Eichhorn , K. J. Eskola , E. G. Ferreiro , O. Fischer , O. Flores-Sánchez , S. Forte , A. Gaddi , J. Gao , T. Gehrmann , A. Gehrmann-De Ridder , F. Gerigk , A. Gilbert , F. Giuli , A. Glazov , N. Glover , R. M. Godbole , B. Goddard , V. Gonçalves , G. A. Gonzalez-Sprinberg , A. Goyal , J. Grames , E. Granados , A. Grassellino , Y. O. Gunaydin , Y. C. Guo , V. Guzey , C. Gwenlan , A. Hammad , C. C. Han , L. Harland-Lang , F. Haug , F. Hautmann , D. Hayden , J. Hessler , I. Helenius , J. Henry , J. Hernandez-Sanchez , H. Hesari , T. J. Hobbs , N. Hod , G. H. Hoffstaetter , B. Holzer , C. G. Honorato , B. Hounsell , N. Hu , F. Hug , A. Huss , A. Hutton , R. Islam , S. Iwamoto , S. Jana , M. Jansova , E. Jensen , T. Jones , J. M. Jowett , W. Kaabi , M. Kado , D. A. Kalinin , H. Karadeniz , S. Kawaguchi , U. Kaya , R. A. Khalek , H. Khanpour , A. Kilic , M. Klein , U. Klein , S. Kluth , M. Köksal , F. Kocak , M. Korostelev , P. Kostka , M. Krelina , J. Kretzschmar , S. Kuday , G. Kulipanov , M. Kumar , M. Kuze , T. Lappi , F. Larios , A. Latina , P. Laycock , G. Lei , E. Levitchev , S. Levonian , A. Levy , R. Li , X. Li , H. Liang , V. Litvinenko , M. Liu , T. Liu , W. Liu , Y. Liu , S. Liuti , E. Lobodzinska , D. Longuevergne , X. Luo , W. Ma , M. Machado , S. Mandal , H. Mäntysaari , F. Marhauser , C. Marquet , A. Martens , R. Martin , S. Marzani , J. McFayden , P. Mcintosh , B. Mellado , F. Meot , A. Milanese , J. G. Milhano , B. Militsyn , M. Mitra , S. Moch , M. Mohammadi Najafabadi , S. Mondal , S. Moretti , T. Morgan , A. Morreale , P. Nadolsky , F. Navarra , Z. Nergiz , P. Newman , J. Niehues , E. A. Nissen , M. Nowakowski , N. Okada , G. Olivier , F. Olness , G. Olry , J. A. Osborne , A. Ozansoy , R. Pan , B. Parker , M. Patra , H. Paukkunen , Y. Peinaud , D. Pellegrini , G. Perez-Segurana , D. Perini , L. Perrot , N. Pietralla , E. Pilicer , B. Pire , J. Pires , R. Placakyte , M. Poelker , R. Polifka , A. Polini , P. Poulose , G. Pownall , Y. A. Pupkov , F. S. Queiroz , K. Rabbertz , V. Radescu , R. Rahaman , S. K. Rai , N. Raicevic , P. Ratoff , A. Rashed , D. Raut , S. Raychaudhuri , J. Repond , A. H. Rezaeian , R. Rimmer , L. Rinolfi , J. Rojo , A. Rosado , X. Ruan , S. Russenschuck , M. Sahin , C. A. Salgado , O. A. Sampayo , K. Satendra , N. Satyanarayan , B. Schenke , K. Schirm , H. Schopper , M. Schott , D. Schulte , C. Schwanenberger , T. Sekine , A. Senol , A. Seryi , S. Setiniyaz , L. Shang , X. Shen , N. Shipman , N. Sinha , W. Slominski , S. Smith , C. Solans , M. Song , H. Spiesberger , J. Stanyard , A. Starostenko , A. Stasto , A. Stocchi , M. Strikman , M. J. Stuart , S. Sultansoy , H. Sun , M. Sutton , L. Szymanowski , I. Tapan , D. Tapia-Takaki , M. Tanaka , Y. Tang , A. T. Tasci , A. T. Ten-Kate , P. Thonet , R. Tomas-Garcia , D. Tommasini , D. Trbojevic , M. Trott , I. Tsurin , A. Tudora , I. Turk Cakir , K. Tywoniuk , C. Vallerand , A. Valloni , D. Verney , E. Vilella , D. Walker , S. Wallon , B. Wang , K. Wang , K. Wang , X. Wang , Z. S. Wang , H. Wei , C. Welsch , G. Willering , P. H. Williams , D. Wollmann , C. Xiaohao , T. Xu , C. E. Yaguna , Y. Yamaguchi , Y. Yamazaki , H. Yang , A. Yilmaz , P. Yock , C. X. Yue , S. G. Zadeh , O. Zenaiev , C. Zhang , J. Zhang , R. Zhang , Z. Zhang , G. Zhu , S. Zhu , F. Zimmermann , F. Zomer , J. Zurita , P. Zurita

The mid-infrared range is an important spectrum range where materials exhibit a characteristic response corresponding to their molecular structure. A free-electron laser (FEL) is a promising candidate for a high-power light source with…

The Linac Coherent Light Source (LCLS) is the first x-ray laser user facility based upon a free electron laser (FEL). In addition to many other stringent requirements, the LCLS XFEL requires extraordinary beam quality to saturate at 1.5…

The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e$^+$e$^-$-collider under development by the CLIC accelerator collaboration, hosted by CERN. The CLIC accelerator has been optimised for three energy stages at…

We have explored a concept for an advanced Normal-Conducting Radio-Frequency (NCRF) C-band linear accelerator (linac) structure to achieve a high gradient, high power e$^+$e$^-$ linear collider in the TeV class. This design study represents…

The Cornell Electron Storage Ring (CESR) was reconfigured in 2008 as a test accelerator to investigate the physics of ultra-low emittance damping rings. During the approximately 40 days/year available for dedicated operation as a test…

Accelerator Physics · Physics 2013-08-13 David L. Rubin

We discuss the goals, the designs, the state of technical readiness, and the critical R&D needs of the accelerators that are currently under discussion as Higgs and electroweak factories. We also address the respective staging options…

"LUE200" - 200 MeV electron linac is being created at JINR as a driver of the pulsed neutron source "IREN" [1]. The special full-scale facilities for testing the main systems of LUE-200 (FSTF) are used at JINR, BINP, MEPhI and YerPhI [2].…

Accelerator Physics · Physics 2009-10-05 S. N. Dolya , W. I. Furman , V. V. Kobets , E. M. Laziev , Yu. A. Metelkin , V. A. Shvets , A. P. Soumbaev

Test beam and irradiation facilities are the key enabling infrastructures for research in high energy physics (HEP) and astro-particles. In the last 11 years the Beam-Test Facility (BTF) of the DA{\Phi}NE accelerator complex in the Frascati…