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Abstracts Brochure - CERN

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

with this cavity. An initial experiment with copper benchmarked our apparatus. It afforded an opportunity to refine<br />

our technique of determining Q0 from the reflected frequency response and revealed the behavior of copper down to<br />

4.2 K. This was followed by a test of a niobium sample. A test is also planned for MgB2. In addition to characterizing<br />

the onset of superconductivity with temperature, our cavity can be resonated with a high power klystron to determine<br />

the surface magnetic field level sustainable by the material in the superconducting state.<br />

*C. Nantista et al. “Test Bed for Superconducting Materials,” presented at the 2005 Particle Accelerator Conference,<br />

Knoxville, Tennessee, May 16-20, 2005; SLAC-PUB-11246.<br />

1.3 GHz Electrically Controlled Fast Ferroelectric Tuner<br />

A fast, electrically-controlled tuner is described<br />

with parameters suitable for operation<br />

with the 9-cell SC accelerator structure<br />

of ILC. The tuner is based on a magic tee and<br />

V.P. Yakovlev (Omega-P, Inc.) J.L. Hirshfield (Yale University,<br />

Physics Department) S. Kazakov (KEK)<br />

two phase shifters that contain ferroelectric rings. The dielectric constant of the ferroelectric ring is altered by applying<br />

a 4.2 kV DC pulse that provides an RF phase shift from 0 deg to 180 deg. This, in turn allows a change of the input<br />

signal amplitude from zero to its maximum value, or a change in phase from 0 deg to 360 deg during the RF pulse. It<br />

is shown that the possibility of changing the cavity coupling to the input line during the RF pulse allows significant<br />

RF power savings, up to 12.5 MW for the 800 GeV ILC option. In addition, fast electrically-tuned amplitude and<br />

phase control with a feed-back system should be useful to compensate for possible phase deviations of the input RF<br />

fields in each cavity of ILC to match the cavity with the feeding transmission line as the beam load varies.<br />

The JLAB Ampere-class Cryomodule Conceptual Design<br />

For the next generation of compact highpower<br />

FELs a new cryomodule is required<br />

that is capable of accelerating up to Ampere<br />

levels of beam current. Challenges include<br />

R.A. Rimmer, E. Daly, J. Henry, W.R. Hicks, J.P. Preble, M. Stirbet,<br />

H. Wang, K. Wilson, G. Wu (Jefferson Lab)<br />

strong HOM damping, high HOM power and high fundamental-mode power (in operating scenarios without full<br />

energy recovery). For efficient use of space a high real-estate gradient is desirable and for economic operation good<br />

fundamental-mode efficiency is important. The technology must also be robust and should be based on well-proven<br />

and reliable technologies. For Ampere-class levels of beam current both halo interception and beam break-up (BBU)<br />

are important considerations. These factors tend to drive the designs to lower frequencies where the apertures are<br />

larger and the transverse impedances are lower. To achieve these goals we propose to use a compact waveguidedamped<br />

multi-cell cavity packaged in an SNS-style cryomodule.<br />

Compact Waveguide Fundamental Power Coupler Design for 1-Ampere Cryomodule<br />

Development of a new CW cryomodule capable<br />

of transporting Ampere-level beam currents<br />

in a compact FEL is currently underway<br />

at JLAB. The 748.5 MHz cavities will operate<br />

M. Stirbet, E. Daly, J. Henry, W.R. Hicks, R.A. Rimmer, K. Wilson<br />

(Jefferson Lab)<br />

with at least 16 MV/m acceleration gradients at forward RF power up to 200 kW. In this paper we propose a compact<br />

waveguide fundamental power coupler, based on the robust, pre-stressed planar window concept developed and<br />

101<br />

MOPCH181<br />

MOPCH182<br />

MOPCH183

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