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Related papers: An injector for the CLIC test Facility (CTF3)

200 papers

Using the China Spallation Neutron Source (CSNS) linac as the injector, a 500 MeV proton synchrotron is proposed for multidisciplinary application, such as biology, material and proton therapy. The synchrotron will deliver proton beam with…

Accelerator Physics · Physics 2016-09-21 Liang-Sheng Huang , Sheng Wang , Hong-Fei Ji

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

Purpose: In this study, procedures were developed to achieve efficient reversible conversion of a clinical linear accelerator (LINAC) and deliver electron FLASH (eFLASH) or conventional beams to the treatment room isocenter. Material &…

This report describes the physics potential and experiments at a future multi-TeV e+e- collider based on the Compact Linear Collider (CLIC) technology. The physics scenarios considered include precision measurements of known quantities as…

Instrumentation and Detectors · Physics 2012-04-22 Lucie Linssen , Akiya Miyamoto , Marcel Stanitzki , Harry Weerts

The Linac Coherent Light Source (LCLS) project at SLAC uses a dense 15 GeV electron beam passing through a long undulator to generate extremely bright x-rays at 1.5 angstroms. The project requires electron bunches with a nominal peak…

Accelerator Physics · Physics 2007-05-23 R. Akre , V. Bharadwaj , P. Emma , P. Krejcik

We report results of the beam commissioning and first operation of the 1.3 GHz superconducting RF electron linear accelerator at Fermilab Accelerator Science and Technology (FAST) facility. Construction of the linac was completed and the…

Ionization injection in a plasma wakefield accelerator was investigated experimentally using two lithium plasma sources of different lengths. The ionization of the helium gas, used to confine the lithium, injects electrons in the wake.…

The Compressed Baryonic Matter (CBM) experiment is one of the major scientific spectrometers of the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt. As one of the core sub-systems in CBM experiment for charged hadron…

Instrumentation and Detectors · Physics 2023-09-01 K. Wang , J. Zhou , X. Wang , X. Li , D. Hu , Y. Sun

The expected increase of total integrated luminosity by a factor of ten at the HL-LHC compared to the design goals for LHC essentially eliminates the safety factor for radiation hardness realized at the current cold amplifiers of the ATLAS…

Instrumentation and Detectors · Physics 2019-08-13 Martin Nagel

This article presents a new particle beam cooling scheme, namely cyclotron maser cooling (CMC). Relativistic gyrating particles, forced by a solenoidal magnetic field over some length of their trajectory, move in a helical path and undergo…

Accelerator Physics · Physics 2025-03-07 Hidetsugu Ikegami

ITER envisages the use of two heating neutral beam injectors plus an optional one as part of the auxiliary heating and current drive system. The 16.5 MW expected neutral beam power per injector is several notches higher than worldwide…

Plasma Physics · Physics 2023-04-05 D. Marcuzzi , V. Toigo , M. Boldrin , G. Chitarin , S. Dal Bello , L. Grando , A. Luchetta , R. Pasqualotto , M. Pavei , G. Serianni , L. Zanotto , R. Agnello , P. Agostinetti , M. Agostini , D. Aprile , M. Barbisan , M. Battistella , G. Berton , M. Bigi , M. Brombin , V. Candela , V. Candeloro , A. Canton , R. Casagrande , C. Cavallini , R. Cavazzana , L. Cordaro , N. Cruz , M. Dalla Palma , M. Dan , A. De Lorenzi , R. Delogu , M. De Muri , M. De Nardi , S. Denizeau , M. Fadone , F. Fellin , A. Ferro , E. Gaio , C. Gasparrini , F. Gnesotto , P. Jain , A. La Rosa , D. Lopez-Bruna , R. Lorenzini , A. Maistrello , G. Manduchi , S. Manfrin , N. Marconato , I. Mario , G. Martini , R. Milazzo , T. Patton , S. Peruzzo , N. Pilan , A. Pimazzoni , C. Poggi , N. Pomaro , B. Pouradier-Duteil , M. Recchia , A. Rigoni-Garola , D. Rizzetto , A. Rizzolo , F. Santoro , E. Sartori , B. Segalini , A. Shepherd , M. Siragusa , P. Sonato , A. Sottocornola , E. Spada , S. Spagnolo , M. Spolaore , C. Taliercio , P. Tinti , P. Tomsič , L. Trevisan , M. Ugoletti , M. Valente , M. Valisa , F. Veronese , M. Vignando , P. Zaccaria , R. Zagorski , B. Zaniol , M. Zaupa , M. Zuin , M. Cavenago , D. Boilson , C. Rotti , H. Decamps , F. Geli , A. Sharma , P. Veltri , J. Zacks , M. Simon , F. Paolucci , A. Garbuglia , D. Gutierrez , A. Masiello , G. Mico , C. Labate , P. Readman , E. Bragulat , L. Bailly-Maitre , G. Gomez , G. Kouzmenko , F. Albajar , M. Kashiwagi , H. Tobari , A. Kojima , M. Murayama , S. Hatakeyama , E. Oshita , T. Maejima , N. Shibata , Y. Yamashita , K. Watanabe , N. P. Singh , M. J. Singh , H. Dhola , U. Fantz , B. Heinemann , C. Wimmer , D. Wünderlich , K. Tsumori , G. Croci , G. Gorini , A. Muraro , M. Rebai , M. Tardocchi , L. Giacomelli , D. Rigamonti , F. Taccogna , D. Bruno , M. Rutigliano , S. Longo , S. Deambrosis , E. Miorin , F. Montagner , A. Tonti , F. Panin

We present a study of the capability of a 500 GeV e+e- collider based on CLIC technology for precision measurements of top quark properties. The analysis is based on full detector simulations of the CLIC_ILD detector concept using Geant4,…

High Energy Physics - Experiment · Physics 2012-02-16 Frank Simon , Katja Seidel , Stephane Poss

A comparison of the two most prominent electron sources of high average current high brightness electron beams, DC and superconducting RF photoemission guns, is carried out using a large-scale multivariate genetic optimizer interfaced with…

Accelerator Physics · Physics 2011-08-22 Ivan V. Bazarov , Allen Kim , Manu N. Lakshmanan , Jared M. Maxson

Terahertz radiation has broad application prospect due to its ability to penetrate deep into many organic materials without damage caused by ionizing radiations. A FEL-based THz source is the best choice to produce high-power radiation. In…

Accelerator Physics · Physics 2015-06-17 J. Li , Y. J. Pei , L. Shang , G. Feng , T. Hu , Q. Chen , C. Li

This article investigates electron bunch density fluctuations in the 1 - 10 $\mu m$ wavelength range, focusing on their impact on coherent electron cooling (CEC) in hadron storage rings. In this study, we thoroughly compare the shot-noise…

The China spallation neutron source (CSNS) linac is designed with beam energy of 81MeV and a peak current of 15mA in the first phase. The RF power system for the 81 MeV Linac requires 8 units of RF power sources, each unit has one…

Accelerator Physics · Physics 2019-09-26 Linyan Rong , Zhencheng Mu , Zhexin Xie , Bo Wang , Wenzhong Zhou , Maliang Wan , Meifei Liu , Jian Li , Xinan Xu

A compact accelerator design for irradiation purposes is being proposed at KEK. This design targets an energy of 10 MeV and a current of 50 mA. Current design includes a 100 kV thermionic DC electron gun with an RF grid, 1-cell…

Accelerator Physics · Physics 2024-04-15 Olga Tanaka , Yosuke Honda , Masahiro Yamamoto , Tomohiro Yamada , Hiroshi Sakai

In this paper, we will describe some of the recent experimental measurements [1, 2, 3] performed at CESRTA [4], and the supporting simulations, which probe the interaction of the electron cloud with the stored beam. These experiments have…

CIEMAT has been working on the RF power extractor so-called PETS (Power Extraction and Transfer Structure) for the CLIC Test Facility 3 (CTF3) since 2007. The first contribution has been installed at the Test Beam Line (TBL). Additionally,…