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000582401 035__ $$9CERN annual report$$a2003-3.1060
000582401 035__ $$9SPIRES$$a5258006
000582401 035__ $$9Inspire$$a599195
000582401 037__ $$aCERN-PS-2002-073-AE
000582401 037__ $$aCLIC-Note-540
000582401 041__ $$aeng
000582401 084__ $$2CERN Library$$aCLIC-Note-0540
000582401 088__ $$9CLIC-Note-540
000582401 088__ $$9CERN-PS-2002-073-AE
000582401 100__ $$aCorsini, R$$uCERN
000582401 245__ $$aOverview of CLIC and CTF3
000582401 260__ $$c2002
000582401 269__ $$aGeneva$$bCERN$$c24 Sep 2002
000582401 300__ $$a6 p
000582401 340__ $$apaper
000582401 520__ $$aThe CLIC study aims at the design of a high-energy (0.5-5 TeV), high luminosity e+e- linear collider, as a possible facility for the post-LHC era. The beams are accelerated using high-frequency (30 GHz) normal-conducting structures operating at high accelerating gradients to reduce the length and, in consequence, the cost of the linac. The RF power for these structures is generated using the so-called Two-Beam Acceleration (TBA) scheme, where a low-energy, high-intensity electron beam (drive beam) runs parallel to the main linacs and is decelerated in resonant structures, which extract RF power from the drive beam. The drive beam is first accelerated in a low-frequency fully-loaded normal-conducting linac. Its time structure is then obtained by funneling in isochronous rings using transverse RF deflectors. CTF3, a new generation CLIC Test Facility, is being built at CERN to demonstrate the technical feasibility of this novel drive beam generation and RF power production scheme, albeit on a much smaller scale. CTF3 will also constitute a 30 GHz source with the CLIC nominal peak power and pulse length, for RF component testing. In this paper we give an overview of the CLIC study, focusing on the most recent progress and describe the CTF3 status.
000582401 540__ $$aCC-BY-4.0
000582401 542__ $$f© CERN
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000582401 595__ $$aDigitized by Digitra under DO XXX
000582401 595__ $$aCERN EDS
000582401 595__ $$aPSARCHIVE
000582401 595__ $$aCLIC-Note
000582401 595__ $$aPS-AE2
000582401 595__ $$aOA
000582401 595__ $$aCLIC-Note
000582401 595__ $$aSIS LINAC02-2004
000582401 595__ $$aCLICARCHIVE
000582401 595__ $$zCLAS1
000582401 595__ $$aCERN-PS-*-REPORT
000582401 595__ $$aCLICARCHIVE
000582401 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
000582401 693__ $$aCLIC$$eCTF3
000582401 690C_ $$aCERN
000582401 690C_ $$aARTICLE
000582401 690C_ $$aREPORT
000582401 710__ $$5PS
000582401 710__ $$gCLIC Study Group
000582401 859__ $$fAnne-Francoise.Molat-Berbiers@cern.ch
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000582401 916__ $$sn$$w200239$$ya2003
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000582401 980__ $$aConferencePaper
000582401 980__ $$bARTICLE