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Abstracts Brochure - CERN

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THPLS078<br />

THPLS079<br />

THPLS080<br />

THPLS081<br />

29-Jun-06 16:00 - 18:00 THPLS — Poster Session<br />

Tests of a New Bunch Cleaning Technique for the Advanced Light Source<br />

The Advanced Light Source at the Lawrence<br />

F. Sannibale, W. Barry, M.J. Chin (LBNL)<br />

Berkeley National Laboratory is a third generation<br />

synchrotron light source operating at<br />

1.9 GeV and optimized for the production of soft x-rays. The machine usually operates with 400 mA of stored electrons<br />

equally distributed among 276 contiguous buckets over the total of 328 available. The main reason for having this gap<br />

is for allowing users to perform experiments where a long relaxation time for their sample is required. For such users,<br />

a higher current bunch the "camshaft" is placed in the middle of the gap. Due to imperfect injection and to particle<br />

diffusion from different bunches, the "empty" buckets present a level of purity of the order of 0.1% respect to the<br />

camshaft current. This situation represent a signficant limitation for some users. In order to improve this situation,<br />

we are testing a bunch cleaning technique that allows for the cleaning the gap to much better purity levels without<br />

affecting either the camshaft or the other 276 bunches. In this paper we report on the results obtained so far.<br />

Bunch Diffusion Measuments at the Adavanced Light Source<br />

The Advanced Light Source (ALS) at the<br />

F. Sannibale, W.E. Byrne, J. Guo (LBNL) A.S. Tremsin (UCB) Lawrence Berkeley National Laboratory is a<br />

third generation synchrotron light source operating<br />

at 1.9 GeV and optimized for the production of soft x-rays. Twice per years a special user operation shift of 2<br />

weeks, is done dedicated to experiments where a long relaxation time for the samples is required. During these shifts,<br />

the storage ring is injected with a two opposite bunches pattern with about 30 mA of stored current per bunch. Most<br />

of the experiments require that all the other 326 remaining buckets must be clean from particles at a level of purity of<br />

better than 0.01% of the total stored current. For this reason after the injection, we use a special procedure that cleans<br />

the "empty" buckets to the required purity level. Particle diffusion from the main bunches must be avoided otherwise<br />

the purity level will get progressively worst and an additional cleaning could be required after some time. In this<br />

paper we present the measurements we did for the characterization of particle diffusion in the present ALS lattice.<br />

Progress on Diagnostics Upgrades for ALS Top-off Mode<br />

T. Scarvie, W. Barry, F. Sannibale (LBNL)<br />

In preparation for top-off mode at the Advanced<br />

Light Source, some old diagnostics<br />

systems are being refurbished and several<br />

new ones created. This paper catalogs the progress made on these top-off related upgrades. In particular, results<br />

from our first booster-to-storage-ring transfer line synchrotron radiation monitor are shown, and progress on<br />

the future storage ring bunch-by-bunch current monitor is presented.<br />

Operational Experience with the Undulator Based Fs-slicing Source at the ALS<br />

To improve the flux and brightness of the fs-<br />

C. Steier, D. Robin, W. Wan, W. Wittmer, A. Zholents (LBNL) slicing source at the ALS, an upgrade project<br />

has been completed. The new beamline uses<br />

an in-vacuum undulator as a radiator, a high repetition rate fs laser and other upgrades to provide several orders<br />

of magnitude higher flux than the original bend magnet beamline. In order to separate the fs-slices of the electron<br />

470

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