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Compact Linear Collider
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=== Drive beam === Each Drive Beam complex is composed of a 2.5 km-long linac, followed by a Drive Beam Recombination Complex: a system of delay lines and combiner rings where the incoming beam pulses are interleaved to ultimately form a 12 GHz sequence and a local beam [[electric current|current]] as high as 100[[ampere|A]].<ref name=2018_proj_imp/> Each 2.5 km-long Drive Beam linac is powered by 1 GHz [[klystron]]''s''. This produces a 148 μs-long beam (for the 1.5 TeV energy stage scenario) with a bunching [[frequency]] of 0.5 GHz. Every 244 ns the bunching phase is switched by 180 degrees, i.e. odd and even buckets at 1 GHz are filled alternately. This phase-coding allows the first factor two recombination: the odd bunches are delayed in a Delay Loop (DL), while the even bunches bypass it. The [[time of flight]] of the DL is about 244 ns and tuned at the picosecond level such that the two trains of bunches can merge, forming several 244 ns-long trains with bunching frequency at 1 GHz, separated by 244 ns of empty space. This new time-structure allows for further factor 3 and factor 4 recombination in the following combiner rings with a similar mechanism as in the DL. The final [[time]] structure of the beam is made of several (up to 25) 244 ns-long trains of bunches at 12 GHz, spaced by gaps of about 5.5 μs. The recombination is timed such that each combined train arrives in its own decelerator sector, synchronized with the arrival of the Main Beam. The use of low-frequency (1 GHz), long-pulse-length (148 μs) klystrons for accelerating the Drive Beam and the beam recombination makes it more convenient than using klystrons to directly accelerate the Main Beam.<ref name=2018_proj_imp />[[File:CLIC two beam module installed in the CLIC Test Facility at CERN (CTF3).jpg|thumb|Image of the CLIC Two Beam Module in the CLIC Test Facility, CERN ([[CTF3]]). The beam travels from left to right.|alt=|280x280px]]
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