DocumentCode
2131521
Title
Dispersion and betatron matching into the linac
Author
Decker, F.J. ; Adolphsen, C. ; Corbett, W.J. ; Emma, P. ; Hsu, I. ; Moshammer, H. ; Seeman, J.T. ; Spence, W.L.
Author_Institution
SLAC, CA, USA
fYear
1991
fDate
6-9 May 1991
Firstpage
905
Abstract
In high-energy linear colliders, the low-emittance beam from a damping ring has to be preserved all the way to the linear accelerator (LINAC), in the LINAC and to the interaction point. In particular, the ring-to-LINAC (RTL) section of the SLAC Linear Collider (SLC) should provide an exact betatron and dispersion match from the damping ring to the LINAC. A beam with a nonzero dispersion shows up immediately as an increased emittance, while with a betatron mismatch the beam forms filaments in the LINAC. Experimental tests and tuning procedures have shown that the linearized beta matching algorithms are insufficient if the actual transport line has some unknown errors not included in the model. Also, adjusting quadrupole strengths steers the beam if it is offset in the quadrupole magnets. These and other effects have led to a lengthy tuning process, which in the end improves the matching, but is not optimal. Different ideas are discussed to improve this matching procedure and make it a more reliable, faster, and simpler process.<>
Keywords
beam handling equipment; linear accelerators; SLAC Linear Collider; betatron matching; damping ring; dispersion match; high-energy linear colliders; linac; linear accelerator; linearized beta matching algorithms; low-emittance beam; nonzero dispersion; quadrupole strengths; tuning; Acceleration; Colliding beam devices; Damping; Dispersion; Linear accelerators; Linear particle accelerator; Magnets; Reliability theory; Testing; Wire;
fLanguage
English
Publisher
ieee
Conference_Titel
Particle Accelerator Conference, 1991. Accelerator Science and Technology., Conference Record of the 1991 IEEE
Conference_Location
San Francisco, CA, USA
Print_ISBN
0-7803-0135-8
Type
conf
DOI
10.1109/PAC.1991.164485
Filename
164485
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