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Abstracts Brochure - CERN

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MOPLS — Poster Session 26-Jun-06 16:00 - 18:00<br />

Magnetic Modelling of a Short Period Superconducting Helical Undulator for the ILC<br />

Positron Source<br />

A positron source utilising undulators is now<br />

defined as the baseline option for the International<br />

Linear Collider (ILC). The ILC requires<br />

a short period undulator, as close to 10mm<br />

as possible, that is capable of producing 10<br />

MeV photons. The HeliCal collaboration in<br />

the UK has undertaken a programme to design,<br />

develop and produce a prototype un-<br />

J. Rochford, E. Baynham, T.W. Bradshaw, F.S. Carr, Y. Ivanyushenkov<br />

(CCLRC/RAL/ASTeC) I.R. Bailey, L.I. Malysheva (Cockcroft Institute)<br />

D.P. Barber (DESY) A.J. Brummitt (CCLRC/RAL) J.A. Clarke,<br />

O.B. Malyshev, D.J. Scott (CCLRC/DL/ASTeC) P. Cooke, J.B. Dainton<br />

(Liverpool University, Science Faculty) G.A. Moortgat-Pick<br />

(Durham University)<br />

dulator. As part of the programme, the group has used the OPERA software package to perform the magnetic design<br />

of the undulator. The design has addressed several issues, including the effect of magnetic material for the undulator<br />

former, optimal winding geometry, the magnetic flux inside the superconductor and its variation with undulator<br />

period and the winding bore. This paper summarizes the results of both the 2d and the 3d magnetic simulations.<br />

Higher Band Dipole Wake Field Simulations for the Main Linacs of the ILC<br />

The main superconducting L-band linacs of<br />

the ILC (International Linear Collider) will R.M. Jones, R.M. Jones (UMAN)<br />

consist of two sets of approximately 10,000<br />

nine-cell accelerating cavities, which will accelerate electrons and positrons up to a center of mass energy of initially<br />

500 GeV and 1 TeV in a future projected upgrade. During acceleration, it is important to preserve the emittance of the<br />

beam as any dilution thereof will degrade the luminosity of the beams at the collision point. Transverse wake fields<br />

excited by multiple bunches with the beam train can cause the emittance to be diluted and in the worst case can give<br />

rise to a beam break up instability. Here we report on detailed wake field simulations for TESLA-like cavities and<br />

on recently designed LL (Low Loss) and re-entrant cavities; the latter cavities are reshaped with a view to achieving<br />

higher gradients. The impact on beam dynamics is taken into account by tracking the particles down the complete<br />

linac and recording the emittance.<br />

Mitigation of Emittance Dilution due to Transverse Mode Coupling in the L-band Linacs<br />

of the ILC<br />

The main L-band linacs of the ILC accelerate<br />

2820 bunches from a center of mass of 10 R.M. Jones, R.M. Jones (UMAN) R.H. Miller (SLAC)<br />

GeV to 500 GeV (and in the proposed later<br />

upgrade, to 1 TeV). The emittance of the vertical plane is approximately 400 times less than that of the horizontal<br />

plane. Provided the vertical and horizontal mode dipole frequencies are degenerate, then the motion in each plane<br />

is not coupled. However, in reality the degeneracy will more than likely be removed with the eigen modes lying<br />

in planes rotated from the x and y planes due to inevitable manufacturing errors introduced in fabricating 20,000<br />

cavities. This gives rise to a transverse coupling in the horizontal-vertical motion and can readily lead to a dilution<br />

in the emittance in the vertical plane. We investigate means to ameliorate this emittance dilution by splitting the<br />

horizontal-vertical tune of the lattice.<br />

141<br />

MOPLS118<br />

MOPLS119<br />

MOPLS120

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