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Abstracts Brochure - CERN

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WEPCH064<br />

WEPCH065<br />

WEPCH066<br />

28-Jun-06 16:00 - 18:00 WEPCH — Poster Session<br />

to negate the effect of the induced eddy currents. In this report results from measurements of these effects will be<br />

presented. Results from modeling and comparisons to the measurements will also be presented.<br />

Fast Compensation of Global Linear Coupling in RHIC Using AC Dipoles<br />

Global linear coupling has been extensively<br />

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

studied in accelerators and several methods<br />

have been developed to compensate the coupling<br />

vector C using skew quadrupole families scans. However, scanning techniques can become very time consuming<br />

especially during the commissioning of an energy ramp. In this paper we illustrate a new technique to measure and<br />

compensate, in a single machine cycle, global linear coupling from turn-by-turn BPM data without the need of a<br />

skew quadrupole scan. The algorithm is applied to RHIC BPM data using AC dipoles and compared with traditional<br />

methods.<br />

Lattices for High-power Proton Beam Acceleration and Secondary Beam Collection, Cooling,<br />

and Deceleration<br />

S. Wang (IHEP Beijing) K.A. Brown, C.J. Gardner, Y.Y. Lee, D.I.<br />

Lowenstein, S. Peggs, N. Simos, J. Wei (BNL)<br />

290<br />

Rapid-cycling synchrotrons are used to accelerate<br />

high-intensity proton beams to energies<br />

of tens of GeV for secondary beam production.<br />

After primary beam collision with a<br />

target, the secondary beam can be collected, cooled, accelerated or decelerated by ancillary synchrotrons for various<br />

applications. In this paper, we first present a lattice for the main synchrotron. This lattice has: a) flexible momentum<br />

compaction to avoid transition and to facilitate RF gymnastics b) long straight sections for low-loss injection,<br />

extraction, and high-efficiency collimation c) dispersion-free straights to avoid longitudinal-transverse coupling, and<br />

d) momentum cleaning at locations of large dispersion with missing dipoles. Then, we present a lattice for a cooler<br />

ring for the secondary beam. The momentum compaction across half of this ring is near zero, while for the other half<br />

it is normal. Thus, bad mixing is minimized while good mixing is maintained for stochastic beam cooling.<br />

Space Charge Tune Shift and Quantum Lifetime<br />

D.K. Kalantaryan (YSU) Y.L. Martirosyan, V.M. Tsakanov (CAN-<br />

DLE)<br />

The impact of the nonlinear resonance to<br />

electron beam distribution is conditioned by<br />

the proximity to the resonance and resonance<br />

strength. The space charge caused tune shift<br />

modifies the beam distribution. In this paper the equilibrium distribution of the electron beam near the nonlinear<br />

resonance is evaluated, taking into account the space charge caused betatron tune shift. The reduction of the beam<br />

quantum lifetime is calculated. The numerical example for the CANDLE synchrotron light source project is given.

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