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Abstracts Brochure - CERN

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THOAFI01<br />

THOAFI02<br />

THOAFI03<br />

29-Jun-06 09:30 - 10:30 THOAFI — Beam Dynamics and Electromagnetic . . .<br />

THOAFI — Beam Dynamics and Electromagnetic<br />

Fields<br />

The Development of Computational Tools for Halo Analysis and Study of Halo Growth in<br />

the Spallation Neutron Source Linear Accelerator<br />

D.A. Bartkoski, A.V. Aleksandrov, S.M. Cousineau, S. Henderson,<br />

J.A. Holmes (ORNL)<br />

Computational tools have been developed to<br />

quantify the halo in a beam by analyzing<br />

beam profiles and identifying the halo particles<br />

using the Gaussian area ratio and kurto-<br />

sis methods. Simulations of various injection quadrupole magnet configurations using three types of initial simulated<br />

distributions, along with an analysis of their phase space and rms properties, provides insight into the development<br />

of halo in the Spallation Neurton Source linear accelerator. Finally, comparisons with machine beam profile data,<br />

taken at the same conditions as that of the simulated data, show how accurately the simulations model the beam and<br />

its halo development and provide a better understanding of the best machine configuration with which to minimize<br />

beam halo and losses.<br />

Ion Instability Observed in PLS Revolver In-vacuum Undulator<br />

Revolver In-Vacuum X-ray Undulator which<br />

H.-S. Kang, J. Choi, M. Kim, T.-Y. Koo, T.-Y. Lee, P.C.D. Park (PAL) was designed and fabricated at Spring-8 is<br />

under commissioning at PLS. This planar undulator<br />

whose permanent magnet array structure is a revolving type with 90-degree step provides 4 different undulator<br />

wavelengths of 10, 15, 20, and 24 mm. The minimum gap of the undulator is as small as 5 mm. It was observed that<br />

the trailing part of a long bunch train was scraped due to ion instability when the undulator gap was closed below<br />

6 mm. At that time the vacuum pressure in the undulator, which is estimated to be about one order of magnitude<br />

lower than that of the undulator gap, increased from 1.4 x 10 -10 (gap 20 mm) to 7.9 x 10 -10 Torr (gap 6 mm) at the<br />

stored beam current of 100 mA. This high vacuum pressure causes fast beam-ion instability: trailing part of a long<br />

bunch train oscillates vertically. It was also confirmed that adjusting the orbit along the undulator has improved the<br />

situation to some extent. The ion instability measured with a pico-second streak camera and a one-turn BPM as well<br />

as the result of orbit adjustment and chromaticity control will be described in this paper.<br />

Global and Local Coupling Compensation Experiments in RHIC using AC Dipoles<br />

Compensation of transverse coupling during<br />

R. Calaga (BNL) F. Franchi (GSI) R. Tomas (<strong>CERN</strong>)<br />

the RHIC energy ramp has been proven to be<br />

non-trivial and tedious. The lack of accurate<br />

knowledge of the coupling sources has initiated several efforts to develop fast techique using turn-by-turn BPM data<br />

to identify and compensate these sources. This paper aims to summarize the beam experiments performed to measure<br />

the coupling matrix and resonance driving terms with the aid of RHIC ac dipoles.<br />

382 Chair: T. Weiland (TEMF, Darmstadt)

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