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TUP113 |
Emittance Exchange at the Fermilab A0 Photoinjector
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667 |
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- T.W. Koeth
Rutgers University, The State University of New Jersey, Piscataway, New Jersey
- L. Bellantoni, H.T. Edwards, R.P. Fliller, A.S. Johnson, A.H. Lumpkin, J. Ruan, R. Thurman-Keup
Fermilab, Batavia
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Funding: This manuscript has been authored by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy.
An experiment has been developed at the Fermilab A0 Photoinjector Lab to demonstrate the exchange of longitudinal emittance with the horizontal emittance. Our apparatus consists of a 3.9 GHz TM110 deflecting rf cavity placed between two magnetic dogleg channels. The first dogleg generates the needed dispersion to appropriately position the off-momentum electrons in the TM110 cavity. The TM110 cavity reduces the momentum spread and imparts a time dependent transverse kick. The second dogleg finishes the exchange and yields the exchange of the emittances. We report on the measurement of the exchange beamline matrix elements as well as an inital report on measuring the exchange emittances directly.
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Slides
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THP023 |
Crab Cavities for Linear Colliders
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830 |
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- G. Burt, P.K. Ambattu, R.G. Carter, A.C. Dexter, M.I. Tahir
Cockcroft Institute, Lancaster University, Lancaster
- C. Adolphsen, Z. Li, A. Seryi, L. Xiao
SLAC, Menlo Park, California
- C.D. Beard, D.M. Dykes, P. Goudket, A. Kalinin, L. Ma, P.A. McIntosh
STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
- L. Bellantoni, B. Chase, M. Church, T.N. Khabiboulline
Fermilab, Batavia
- R.M. Jones
UMAN, Manchester
- A. Latina, D. Schulte
CERN, Geneva
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Crab cavities have been proposed for a wide number of accelerators and interest in crab cavities has recently increased after the successful operation of a pair of crab cavities in KEK-B. In particular crab cavities are required for both the ILC and CLIC linear colliders for bunch alignment. Consideration of bunch structure and size constraints favours a 3.9 GHz superconducting, multi-cell cavity as the ILC solution, whilst bunch structure and beam-loading considerations suggest an X-band copper travelling wave structure for CLIC. These two cavity solutions are very different in design but share complex design issues. Phase stabilisation, beam loading, wakefields and mode damping are special issues for these crab cavities. Requirements and potential design solutions will be discussed for both colliders.
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