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Abstracts Brochure - CERN

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WEPCH118<br />

WEPCH119<br />

WEPCH120<br />

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

LORASR Code Development<br />

R. Tiede, G. Clemente, H. Podlech, U. Ratzinger, A.C. Sauer (IAP)<br />

S. Minaev (ITEP)<br />

306<br />

LORASR is specialized on the beam dynamics<br />

design of Separate Function DTL’s<br />

based on the ’Combined 0 Degree Structure<br />

(KONUS)’ beam dynamics concept. The<br />

code has been used for the beam dynamics design of several linacs already in operation (GSI-HLI, GSI-HSI, <strong>CERN</strong><br />

Linac 3, TRIUMF ISAC-I) or scheduled for the near future (Heidelberg Therapy Injector, GSI Proton Linac). Recent<br />

code development was focused on the implementation of a new PIC 3D FFT space charge routine, facilitating timeefficient<br />

simulations with up to 1 million macro particles routinely, as well as of tools for error study and loss profile<br />

investigations. The LORASR code was successfully validated within the European HIPPI Project activities: It is the<br />

Poisson solver benchmarking and the GSI UNILAC Alvarez section tracking comparison programme. The error study<br />

tools are a stringent necessity for the design of future high intensity linacs. The new LORASR release will have a<br />

strong impact on the design of the GSI FAIR Facility Proton Linac, as well as the transmission investigations on the<br />

IFMIF Accelerator. This paper presents the status of the LORASR code development and the benchmarking results.<br />

Beam Performance with Internal Targets in the High-energy Storage Ring (HESR)<br />

A. Lehrach, R. Maier, D. Prasuhn (FZJ) O. Boine-Frankenheim, R.W.<br />

Hasse (GSI) F. Hinterberger (Universität Bonn, Helmholtz-Institut<br />

für Strahlen- und Kernphysik)<br />

The High-energy Storage Ring of the future<br />

International Facility for Antiproton and<br />

Ion Research (FAIR) at GSI in Darmstadt is<br />

planned as an antiproton synchrotron storage<br />

ring in the momentum range of 1.5 to 15<br />

GeV/c. An important feature of HESR is the combination of phase space cooled beams and dense internal targets<br />

(e.g., pellet targets), which results in demanding beam parameter requirements for two operation modes: high luminosity<br />

mode with peak luminosities of up to 2·10 32 cm-2 s-1, and high resolution mode with a momentum spread<br />

down to 10-5, respectively. The beam cooling equilibrium and beam loss with internal target interaction is analyzed.<br />

Rate equations are used to predict the rms equilibrium beam parameters. The cooling and intra-beam scattering<br />

rate coefficients are obtained from simplified models. Energy loss straggling in the target and the associated beam<br />

loss are analyzed analytically assuming a thin target. A longitudinal kinetic simulation code is used to study the<br />

evolution of the momentum distribution in coasting and bunched beam. The analytic expressions for the target<br />

induced momentum tail are found in good agreement with the simulation results.<br />

*A. Lehrach et al. Beam Performance and Luminosity Limitations in the High-Energy Storage Ring (HESR), Nuclear<br />

Inst. and Methods in Physics Research, A44704 (2006).<br />

Simulation of 3D Space-charge Fields of Bunches in a Beam Pipe<br />

A. Markovik, G. Pöplau, U. van Rienen (Rostock University, Faculty<br />

of Computer Science and Electrical Engineering) K. Floettmann<br />

(DESY)<br />

Recent applications in accelerator design require<br />

precise 3D calculations of space-charge<br />

fields of bunches of charged particles additionally<br />

taking into account the shape of the<br />

beam pipe. An actual problem of this kind is<br />

the simulation of e-clouds in damping rings. In this paper a simulation tool for 3D space-charge fields is presented<br />

where a beam pipe with an arbitrary elliptical shape is assumed. The discretization of the Poisson equation by<br />

the method of finite differences on a Cartesian grid is performed having the space charge field solved only in the

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