09.12.2012 Views

Abstracts Brochure - CERN

Abstracts Brochure - CERN

Abstracts Brochure - CERN

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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

Development of a Prototype Superconducting CW Cavity and Cryomodule for Energy Recovery<br />

Energy Recovery LINAC (ERL) and LINACdriven<br />

FEL proposals and developments are<br />

now widespread around the world. Superconducting<br />

RF (SRF) cavity advances made<br />

over the last 10 years for TESLA/TTF at 1.3<br />

GHz, in reliably achieving accelerating gra-<br />

P.A. McIntosh, C.D. Beard, D.M. Dykes, B. Todd (CCLRC/DL/<br />

ASTeC) J.M. Byrd, J.N. Corlett, D. Li (LBNL) M. Liepe, V. Medjidzade,<br />

H. Padamsee, J. Sears, V.D. Shemelin (Cornell University)<br />

P. Michel, J. Teichert (FZR)<br />

dients >20 MV/m, suggest their suitability for these ERL and FEL accelerators. Typically however, photon fluxes<br />

are maximised from the associated insertion devices when the electron bunch repetition rate is as high as possible,<br />

making CW-mode operation at high average current a fundamental requirement for these light sources. Challenges<br />

arise in controlling the substantial HOM power and in minimizing the power dissipated at cryogenic temperatures<br />

during acceleration and energy recovery, requiring novel techniques to be employed. This paper details a collaborative<br />

development for an advanced high-Qo cavity and cryomodule system, based on a modified TESLA cavity, housed<br />

in a Stanford/Rossendorf cryomodule. The cavity incorporates a Cornell developed resistive-wall HOM damping<br />

scheme, capable of providing the improved level of HOM damping and reduced thermal load required.<br />

RF Requirements for the 4GLS LINAC Systems<br />

The 4GLS facility at Daresbury will combine<br />

energy recovery linac (ERL) and free<br />

electron laser (FEL) technologies to deliver a<br />

suite of naturally synchronised state-of-the-<br />

P.A. McIntosh, C.D. Beard, D.M. Dykes, A.J. Moss (CCLRC/DL/<br />

ASTeC)<br />

art sources of synchrotron radiation and FEL radiation covering the terahertz (THz) to soft X-ray regimes. CWmode<br />

operation at high acceleration gradients are needed for the various 4GLS accelerator systems and here is where<br />

Superconducting Radio Frequency (SRF) cavities excel. Since resistive losses in the cavity walls increase as the square<br />

of the accelerating voltage, conventional copper cavities become uneconomical when the demand for high CW voltage<br />

grows with particle energy requirements. After accounting for the refrigeration power needed to provide the liquid<br />

helium operating temperature, a net power gain of several hundred remains for SRF over conventional copper cavities.<br />

This paper details the RF requirements for each of the SRF accelerating stages of the 4GLS facility, outlining techniques<br />

necessary to cope with CW-mode operation and HOM power generation.<br />

Analysis of Wakefields in the ILC Crab Cavity<br />

The large crossing angle schemes of the ILC<br />

need a correction of bunch orientation at the<br />

IP in order to recover a luminosity loss of up<br />

to 80%. The orientation of bunches can be<br />

G. Burt (Microwave Research Group, Lancaster University) C.D.<br />

Beard, P. Goudket (CCLRC/DL/ASTeC) L. Bellantoni (Fermilab)<br />

changed using a transverse deflecting cavity. The location of the crab cavity would be close to the final focus, and<br />

small deflections caused by wakefields in the cavities could cause misalignments of the bunches at the IP. Wakefields in<br />

the FNAL CKM cavities have been analysed and their effects studied in view of use as the ILC crab cavity. Numerical<br />

simulations have been performed to analyse the transverse wakepotentials of up to quadrupole order modes in this<br />

cavity and the effect upon bunches passing through this cavity. Trapped modes within the CKM cavity have been<br />

95<br />

MOPCH161<br />

MOPCH162<br />

MOPCH163

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!