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Related papers: Preliminary RF design of an X-band linac for the E…

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In the framework of the Eupraxia Design Study an advanced accelerator facility EUPRAXIA@SPARC_LAB has been proposed to be realized at Frascati (Italy) Laboratories of INFN. Two advanced acceleration schemes will be applied, namely an…

SPARC_LAB is a high-brightness electron photoinjector dedicated to FEL radiation production and research on novel acceleration techniques. It has been in operation at LNF since 2005. It is composed of a newly designed brazeless 1.6-cell…

EuPRAXIA@SPARC_LAB is a new multi-disciplinary user-facility that is currently under construction at the Laboratori Nazionali di Frascati of the INFN in the framework of the EuPRAXIA collaboration. The electron beam will be accelerated by…

Accelerator Physics · Physics 2023-07-06 Fabio Villa

During the initial phase of operation, the linacs of the Next Linear Collider (NLC) will contain roughly 5000 X-Band accelerator structures that will accelerate beams of electrons and positrons to 250 GeV. These structures will nominally…

Accelerator Physics · Physics 2007-05-23 C. Adolphsen , W. Baumgartner , K. Jobe , R. Loewen , D. McCormick , M. Ross , T. Smith , J. W. Wang , T. Higo

At EuPRAXIA@SPARC_LAB, the unique combination of an advanced high-brightness RF injector and a plasma-based accelerator will drive a new multi-disciplinary user-facility. The facility, that is currently under study at INFN-LNF Laboratories…

Early tests of short low group velocity and standing wave structures indicated the viability of operating X-band linacs with accelerating gradients in excess of 100 MeV/m. Conventional scaling of traveling wave traveling wave linacs with…

On the wake of the results obtained so far at the SPARC\_LAB test-facility at the Laboratori Nazionali di Frascati (Italy), we are currently investigating the possibility to design and build a new multi-disciplinary user-facility, equipped…

Accelerator Physics · Physics 2018-12-26 M. Ferrario , D. Alesini , M. P. Anania , M. Artioli , A. Bacci , S. Bartocci , R. Bedogni , M. Bellaveglia , A. Biagioni , F. Bisesto , F. Brandi , E. Brentegani , F. Broggi , B. Buonomo , P. L. Campana , G. Campogiani , C. Cannaos , S. Cantarella , F. Cardelli , M. Carpanese , M. Castellano , G. Castorina , N. Catalan Lasheras , E. Chiadroni , A. Cianchi , R. Cimino , F. Ciocci , D. Cirrincione , G. A. P. Cirrone , R. Clementi , M. Coreno , R. Corsini , M. Croia , A. Curcio , G. Costa , C. Curatolo , G. Cuttone , S. Dabagov , G. Dattoli , G. D'Auria , I. Debrot , M. Diomede , A. Drago , D. Di Giovenale , S. Di Mitri , G. Di Pirro , A. Esposito , M. Faiferri , L. Ficcadenti , F. Filippi , O. Frasciello , A. Gallo , A. Ghigo , L. Giannessi , A. Giribono , L. Gizzi , A. Grudiev , S. Guiducci , P. Koester , S. Incremona , F. Iungo , L. Labate , A. Latina , S. Licciardi , V. Lollo , S. Lupi , R. Manca , A. Marcelli , M. Marini , A. Marocchino , M. Marongiu , V. Martinelli , C. Masciovecchio , C. Mastino , A. Michelotti , C. Milardi , V. Minicozzi , F. Mira , S. Morante , A. Mostacci , F. Nguyen , S. Pagnutti , L. Pellegrino , A. Petralia , V. Petrillo , L. Piersanti , S. Pioli , D. Polese , R. Pompili , F. Pusceddu , A. Ricci , R. Ricci , R. Rochow , S. Romeo , J. B. Rosenzweig , M. Rossetti Conti , A. R. Rossi , U. Rotundo , L. Sabbatini , E. Sabia , O. Sans Plannell , D. Schulte , J. Scifo , V. Scuderi , L. Serafini , B. Spataro , A. Stecchi , A. Stella , V. Shpakov , F. Stellato , E. Turco , C. Vaccarezza , A. Vacchi , A. Vannozzi , A. Variola , S. Vescovi , F. Villa , W. Wuensch , A. Zigler , M. Zobov

There is a strong demand for accelerating structures able to achieve higher gradients and more compact dimensions for the next generation of linear accelerators for research, industrial and medical applications. In the framework of the…

Accelerator Physics · Physics 2020-10-28 Mostafa Behtouei , Luigi Faillace , Bruno Spataro , Alessandro Variola , Mauro Migliorati

TEX facility if commissioned for high power testing to characterize accelerating structures and validate them for the operation on future particle accelerators for medical, industrial and research applications. At this aim, TEX is directly…

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…

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. Its Superconducting Linac, to be used at first stage of acceleration, will be operated in continuous wave (CW) mode. The Linac is divided into three…

Accelerator Physics · Physics 2012-02-27 A. Saini , K. Ranjan , N. Solyak , S. Mishra , V. Yakovlev

High-gradient linacs of next generation require novel accelerating structures which are compact, robust and cost-effective. Dedicated research and development have been launched in the linear-collider community. This paper focuses on the…

In the framework of the Compact Light XLS project, a short ultra-high gradient linearizer working on the third harmonic of the main LINAC frequency is requested. Increasing gradients and reducing dimensions are requirements for XLS and all…

Accelerator Physics · Physics 2021-04-27 Mostafa Behtouei , Bruno Spataro , Franco Di Paolo , Alberto Leggieri

Use of a traveling wave (TW) accelerating structure with a small phase advance per cell instead of standing wave may provide a significant increase of accelerating gradient in a superconducting linear accelerator. The TW section achieves an…

Accelerator Physics · Physics 2015-02-10 Pavel Avrakhov , Roman Kostin , Alexei Kanareykin , Nikolay Solyak , Vyacheslav P. Yakovlev

We are proposing a facility based on high gradient acceleration via x-band RF structures and plasma acceleration. We plan to reach an electron energy of the order of 1 GeV, suitable to drive a Free Electron Laser for applications in the so…

The proposed Next Linear Collider (NLC) contains linac systems operating at L,S,C, and X band. This paper describes a wideband modular low-level RF (LLRF) system applicable for all NLC pulsed RF systems. High speed digital IF techniques are…

Accelerator Physics · Physics 2007-05-23 P. Corredoura , C. Adolphsen

Notably innovative technologies will permit compact and affordable advanced accelerators as the linear collider and X-ray free-electron lasers (XFELs) with accelerating gradients over twice the value achieved with current technologies. In…

Front end of a CW linac of the Project X contains an H source, an RFQ, a medium energy transport line with the beam chopper, and a SC low-beta linac that accelerates H- from 2.5 MeV to 160 MeV. SC Single Spoke Resonators (SSR) will be used…

Accelerator Physics · Physics 2012-02-13 T. Khabiboulline , S. Barbanotti , I. Gonin , N. Solyak , I. Terechkine , V. Yakovlev

A 52MHz Radio Frequency Quadrupole (RFQ) linear accelerator (linac) is designed to serve as an initial structure for the SSC-linac system (injector into Separated Sector Cyclotron). The designed injection and output energy are 3.5 keV/u and…

Accelerator Physics · Physics 2016-09-08 Xiao Chen , He Yuan , Yuan You-Jin , Liu Yong , Xia Jia-Wen , Lu Yuan-Rong , Yuri Batygin

In this paper, we give some guidelines for the design of linear accelerators, with special emphasis on their use in a hadron therapy facility. We concentrate on two accelerator layouts, based on linacs. The conventional one based on a linac…

Accelerator Physics · Physics 2018-04-24 Alessandra Lombardi
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