Abstract
In storage rings, horizontal dispersion in the rf cavities introduces horizontal-longitudinal ($xz$) coupling, contributing to beam tilt in the $xz$ plane. This coupling can be characterized by a ``crabbing'' dispersion term ${\ensuremath{\zeta}}_{a}$ that appears in the normal mode decomposition of the 1-turn transfer matrix. ${\ensuremath{\zeta}}_{a}$ is proportional to the rf cavity voltage and the horizontal dispersion in the cavity. We report experiments at the Cornell Electron Storage Ring Test Accelerator where $xz$ coupling was explored using three lattices with distinct crabbing properties. We characterize the $xz$ coupling for each case by measuring the horizontal projection of the beam with a beam size monitor. The three lattice configurations correspond to (i) 16 mrad $xz$ tilt at the beam size monitor source point, (ii) compensation of the ${\ensuremath{\zeta}}_{a}$ introduced by one of two pairs of rf cavities with the second, and (iii) zero dispersion in rf cavities, eliminating ${\ensuremath{\zeta}}_{a}$ entirely. Additionally, intrabeam scattering is evident in our measurements of beam size vs rf voltage.
Highlights
Just as coupling of horizontal and vertical motion can result in a bunch profile that is tilted in the transverse plane, coupling of horizontal and longitudinal motion will in general produce a tilt in the horizontal-longitudinal plane
Studies of xz tilt have been done at the Cornell Electron Storage Ring Test Accelerator (CesrTA)
We describe recent experiments at CesrTA to measure and correct the xz tilt, and the theoretical basis for our correction techniques
Summary
Just as coupling of horizontal and vertical motion can result in a bunch profile that is tilted in the transverse plane, coupling of horizontal and longitudinal motion will in general produce a tilt in the horizontal-longitudinal (xz) plane. III, we develop a parametrization of the one-turn matrix and a numerical method for obtaining it From this parametrization, we extract the tilt and projected size of beams in arbitrary coupling conditions. IV, we present two methods for eliminating the tilt: (i) canceling the crabbing dispersion ζa by adjusting the horizontal phase advance between the two pairs of rf cavities; (ii) constraining the optics so that the dispersion is zero in the rf straights This necessarily results in nonzero dispersion in the wiggler straight, for operation in these optics, 6 of the 12 damping wigglers must be turned off
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More From: Physical Review Special Topics - Accelerators and Beams
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