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Abstracts Brochure - CERN

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TUPLS005<br />

TUPLS006<br />

TUPLS007<br />

TUPLS008<br />

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

Preliminary Study of Using "Pipetron"-type Magnets for a Pre-accelerator for the LHC Collider<br />

One of the luminosity limitations of the LHC<br />

G. De Rijk, L. Rossi (<strong>CERN</strong>) H. Piekarz (Fermilab)<br />

is the rather low injection energy (0.45 TeV)<br />

with respect to the collision energy (7 TeV).<br />

The magnetic multipoles in the main dipoles at low field and their dynamic behaviour are considered to limit the<br />

achievable bunch intensity and emittance. We report on a preliminary study to increase the injection energy to 1.5 TeV<br />

using a two beam pre-accelerator (LHCI) in the LHC tunnel. The LHCI is based on "Pipetron" magnets as originally<br />

proposed for the VLHC. The aim of the study is to assess the feasibility and to identify the critical processes or systems<br />

that need to be investigated and developed to render such a machine possible.<br />

Optics of a 1.5 TeV Injector for the LHC<br />

A concept is being developed to install a sec-<br />

J.A. Johnstone (Fermilab)<br />

ond ring above the LHC to accelerate protons<br />

from 450 GeV to 1.5 TeV prior to injection into<br />

the LHC. The arc and dispersion suppressor optics of the LHC would be replicated in the injector using combined<br />

function ’transmission line’ magnets orginally proposed for the VLHC. To avoid costly civil construction, in the<br />

straight sections housing detectors at least, the injector and LHC must share beampipes and some magnets through<br />

the detector portion of the straights. Creating the appropriate optics for these injector-LHC transition regions is very<br />

challenging: In addition to matching to the nominal LHC lattice functions at these locations, the changes in altitude<br />

of 1.1 m between the injector and LHC must be accomplished achromatically to avoid emittance blowup when the<br />

beams are transferred to the LHC.<br />

Fermilab Recycler Performance with a Dual Cooling System<br />

In 2005 the 8.9-GeV/c Fermilab Recycler an-<br />

S. Nagaitsev (Fermilab)<br />

tiproton storage ring was equipped with an<br />

electron cooling system, capable of cooling<br />

a record number of particles. The electron cooling system complements the existing stochastic cooling system –<br />

the two systems operate concurrently. This paper will describe the performance of the Recycler ring with a dual<br />

cooling system, its limitations (instabilities and beam lifetime) and future plans to store and cool a larger number of<br />

antiprotons.<br />

A Design for a HOM Water Cooled Absorber for the PEP-II B-factory Low Energy Ring<br />

M. Kosovsky, N. Kurita, A. Novokhatski, J. Seeman, S.P. Weathersby<br />

(SLAC)<br />

220<br />

At high currents and small bunch lengths<br />

beam line components in the PEP-II B-factory<br />

experience RF induced heating from higher<br />

order RF modes (HOMs) produced by scat-<br />

tered intense beam fields. A design for a passive HOM water cooled absorber for the PEP-II low energy ring is<br />

presented. This device is to be situated near HOM producing beamline components such as collimators and provide<br />

HOM damping for dipole and quadrupole modes while minimizing impedance to the beam. We present a method

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