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Abstracts Brochure - CERN

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TUPLS024<br />

TUPLS025<br />

TUPLS026<br />

27-Jun-06 16:00 - 18:00 TUPLS — Poster Session<br />

resonance crossings during acceleration. It is now essential to build at least one to study them in detail and learn how<br />

to optimise them for a variety of applications. It is currently planned to build two in the UK: (1) an electron FFAG<br />

(EMMA) to model muon acceleration and do a detailed study of non-scaling optics; (2) a proton FFAG as a prototype<br />

for hadron therapy. This contribution will discuss both of these projects.<br />

FFAG as a Muon Accelerator for Neutrino Factory<br />

The FFAG accelerator is a solution for rapid<br />

S. Machida (CCLRC/RAL/ASTeC)<br />

acceleration of muons because of its large<br />

aperture and no need of magnet ramping.<br />

Its particle dynamics is, however, peculiar due to high energy gain per turn and large transverse amplitude, which<br />

has not been seen in other types of circular accelerators. One variation of FFAG, called non-scaling FFAG, employs<br />

quite new scheme, namely, out of bucket acceleration. We studied emittance distortion, coupled motions among 3-D<br />

planes, effects of resonance lines, etc., based on a newly developed tracking code. In this paper, we will emphasize<br />

new regime of particle dynamics as well as a modeling technique of FFAG.<br />

Muon Acceleration with a Combination of the Non-scaling FFAG and Superconducting<br />

Linac<br />

The non-scaling Fixed-Field Alternating Gra-<br />

D. Trbojevic, J.S. Berg (BNL) S.A. Bogacz (Jefferson Lab)<br />

dient (FFAG) machines have very strong focusing,<br />

large momentum acceptance, and<br />

small dispersion and betatron functions. This report is a study of using a compact non-scaling FFAG in combination<br />

with the superconducting linac to accelerate the muons. The drift space between two kinds of combined<br />

function magnets in the previous non-scaling FFAG is removed. The time of flight in the non-scaling FFAG has a<br />

parabolic dependence on momentum. The large energy acceptance of the machine requires matching between the<br />

linac and the non-scaling FFAG arcs for both the betatron and dispersion functions over the entire energy range.<br />

A Design of a Combination of Energy Recovery Linac and the Non-scaling FFAG for e-<br />

RHIC<br />

D. Trbojevic, J.S. Berg, M. Blaskiewicz, V. Litvinenko, V. Ptitsyn, T.<br />

Roser, A.G. Ruggiero (BNL)<br />

226<br />

The future relativistic electron heavy ion or<br />

proton collider e-RHIC requires acceleration<br />

of electrons to 10 GeV. In the case that the<br />

super conducting linac is selected for accel-<br />

eration, an energy recovery scheme is required. We propose to study a possibility of using the non-scaling Fixed-<br />

Field Gradient-Accelerator (FFAG) for different energies. The beam will be accelerated by the superconducting linac<br />

at the top of the sine function, brought back to the front of the linac by the non-scaling FFAG and repeating this a<br />

few times until the total energy of 10 GeV is reached. After collisions the beam is brought back by the non-scaling<br />

FFAG and decelerated (on the lower RF phase) in the same sequence but in the reverse order. Conventional and<br />

non-conventional beam dynamic issues will be discussed, like the transit time matching effect and the time of flight<br />

adjustments.

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