CERN - European Organization for Nuclear Research

Minutes of the CLIC Meeting - 20 February 2004


Agenda:

Ongoing work for a new parameter list:

Update on accelerating structure parameters
CLIC module layout variants
Permissible Trip Rate for 30 GHz Structures
Speakers:
Alexej Grudiev, Igor Syratchev, Hans Braun


Alexej presented an update of the HDS structure parameter scan. Since his last presentation on HDS a bug in the program GdFidl had been discovered, which led to a overestimation of the Wakefield amplitudes by a factor 2. For the new parameter this was corrected and the change in pulsed surface heating due to the use of Cu/Zr instead of Cu was taken into account.
He introduced L/N*η as a figure of merit which is proportional to the integrated Luminosity divided by the available power. He compared a structure with a maximum for this figure of merit with a structure with maximum efficiency. Even though the structure has a 8% higher figure of merit, the more effective structure is preferable because of the lower input power (132 vs. 173 MW).
Hans mentioned that the experience showed that large aperture structures did not go high in accelerating gradient and that the reason for this are still not fully understood. He also remarked that the consequences for reducing the bunch separation from 20 to 10 or now even 8/9 RF cycles has not been checked (damping ring RF, kink instability).
Alexej will extend his parameter space to smaller and larger aperture and will investigate other phase advance, frequency and gradient in terms of efficiency.

copy of Alexej's transparencies (pdf format)
Igor showed possibilities for a new CLIC module layout motivated by the shorter structure. The new layout has one PETS for 4 TWS structures. Taking the TWS with the highest efficiency (see above), and accounting for the physical element lengths, a high beam current of 207 A is needed.
Due to the eightfold symmetry of the PETS, the RF power can be extracted into 8 individual waveguides, so that 2 feed each TWS without any RF splitters.
Decreasing the PETS aperture from 25 to 22.5 mm would reduce the current to 157 A, leaving the wakefields scaled with the current about the same. In addition, the input load of the PETS might not be needed. This would further reduced the current to 140 A, for a beam energy of 1.79 GeV.
copy of Igor's transparencies (pdf format)
Hans presented permissible trip rates for the 30 GHz structures in CLIC. From the energy management point-of-view, about 1 trip per hour would be permissible with a 3% structure reserve. But an eventual vertical deflection of the beam by a breakdown (by a field direction change of 2°) could bring the beams out of collision. If a distortion of this magnitude occurred, a trip rate of 0.1trip/hour would result in a 2% luminosity loss.
copy of Hans' transparencies (pdf format)
 

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Frank Tecker  - Last updated  26-02-2004