Impedance Calculations for the Improved Slc Damping Rings*
نویسندگان
چکیده
A longitudinal, single bunch instability is observed in the damping rings of the Stanford Linear Collider (SLC).[l] Beyond a threshold bunch population of 3 x 10” particles the bunch energy spread increases and a “saw-tooth” variation in bunch length and synchronous phase as functions of time is observed. Although the relative amplitude of the saw-tooth variation is small-only on the order of lO%the resulting unpredictability of the beam properties in the rest of the SLC accelerator makes it difficult, if not impossible, to operate the machine above the threshold current. An additional problem at higher currents is that the bunch length is greatly increased: according to earlier measurements the rms length is increased by 60% at 3 x 10”.[2] When the bunch is very long in the ring it becomes difficult or impossible to properly compress it after extraction. We want to solve both of these problems so that the SLC can run at higher currents to increase the luminosity. In order to solve these problems the vacuum chambers of both damping rings are being rebuilt with the aim of reducing their impedance.[3] According to previous calculations the impedance of the SLC damping rings is dominated by the many small discontinuities that are located in the socalled QD and QF vacuum chamber segments-elements such as transitions, masks, bellows-that are inductive to the beam.[4] Since these earlier calculations were performed the bellows of the QD segments have been sleeved, yielding a factor of 2 increase in the instability threshold.[l] In this paper we begin by discussing the gains that might be achieved if we can reduce the impedance of the rings even further. Then we estimate the effect on the total impedance of the actual design changes that are being proposed. Three important elements-the bend-to-quad transitions, the distributed ion pump slots, and the beam position monitor (BPM) electrodes are fully 3-dimensional and will be studied using T3 of the MAFIA computer programs.[5]
منابع مشابه
The Calculated Longitudinal Impedance of the Slc Damping Rings*
A high level of current dependent bunch lengthening has been observed in the north damping ring of the Stanford Linear Collider (SLC), I indicating that the ring’s impedance is very inductive. This level of bunch lengthening will limit the performance of the SLC. In order to study the problem of bunch lengthening in the damping rings and the possibility of reducing their inductance we compute, ...
متن کاملBunch Lengthening Calculations for the Slc Damping Rings’
The problem of bunch lengthening in electron storage rings has been treated by many people, and there have been many experiments. In the typical experiment, the theory is used to determine the impedance of the ring. What has been lacking thus far, however, is a calculation of bunch lengthening that uses a carefully calculated ring impedance (or wakefield). In this paper we begin by finding the ...
متن کاملImpedance Calculation and Verification in Storage Rings
For both the SLC damping rings and the DAΦNE collider a systematic approach to understanding single bunch, longitudinal, current dependent behavior was taken: First, using a bunch significantly shorter than nominal, a careful calculation of the wakefield of the entire vacuum chamber was obtained. This “pseudo-Green” function was then used in bunch lengthening and instability calculations. We re...
متن کاملAn Improved Empirical Equation for Bunch Lengthening in Electron Storage Rings
In this paper we propose an improved empirical equation for the bunch lengthening in electron storage rings. The comparisons are made between the analytical and experimental results, and the agreements are quite well. This improved equation can be equally applied to the case where a storage ring is very resistive (such as the improved SLC damping rings) instead of inductive as usual.
متن کاملA Possible Redesign of the SLAC SLC Damping Rings ’
We describe a possible replacement for the SLC damping rings that would generate beams with normalized horizontal emittances of rcz = 9 x 10B6 m-rad when uncoupled; this is more than three times smaller than that generated by the current rings. The primary difference between the new design and the current ring is the arc cell structure; the insertion regions, the kickers, and the RF are essenti...
متن کامل