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Abstracts Brochure - CERN

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

High Power Coaxial FEM Based on Surface Photonic Band Gap Structures<br />

High frequency (26.5GHz to 40GHz), high<br />

power (tens of MW) microwave sources are<br />

required for cavity testing and conditioning<br />

applications in accelerators such as CLIC.<br />

I.V. Konoplev, A.W. Cross, W. He, P. MacInnes, A. Phelps, C.W.<br />

Robertson, K. Ronald, C.G. Whyte (USTRAT/SUPA)<br />

The first study of microwave radiation from a co-axial Free-Electron Maser (FEM) based on a two-mirror cavity<br />

formed by a 2D Surface Photonic Band Gap (SPBG) structure (input mirror 10.4cm) and 1D SPBG structure (output<br />

mirror 10cm) is presented. The electron beam source consisted of a magnetically insulated plasma flare emission<br />

carbon cathode. Application of a 450kV voltage pulse of duration ∼250ns across the cathode and grounded anode<br />

resulted in the production of a 7.0cm diameter annular electron beam of current ∼1500A. The output radiation power<br />

from the FEM was measured using a Ka-band horn with 60dB of attenuation in front of a microwave detector located<br />

at a distance of 1.5m from the output window. By integrating the microwave power measured at the detector over the<br />

radiation pattern a total power of 50 (±10) MW corresponding to an efficiency of ∼9% was calculated. The location<br />

of the operating frequency was found to lie between 35GHz and 39GHz, which agrees with theoretically predicted<br />

frequency of 37.2GHz.<br />

Design and Simulation of a Cusp Gun for Gyro-amplifier Application in High Frequency<br />

RF Accelerators<br />

Gyro-amplifiers have potential as the high<br />

frequency RF drivers for particle accelerators.<br />

They require relativistic electron beams<br />

with low velocity spread and with a high<br />

fraction of the electron energy associated<br />

D.H. Rowlands, A.W. Cross, W. He, A. Phelps, E.G. Rafferty, C.W.<br />

Robertson, K. Ronald, J. Thomson, C.G. Whyte, A.R. Young (US-<br />

TRAT/SUPA)<br />

with the cyclotron motion. For harmonic operation and mode control an axis-encircling beam is desirable. The<br />

passage of an electron beam through a non-adiabatic magnetic field reversal (cusp) converts part of the electron<br />

beam’s axial velocity into axis-encircling transverse velocity. A cusp-based electron beam forming system, yielding<br />

a 10MW, 150kV, 70A axis-encircling beam will be presented. This cusp gun is being designed as the electron beam<br />

source for a microwave gyro-amplifier that is relevant for high frequency accelerator applications. The latest results<br />

from numerical simulations and experiments will be presented and compared.<br />

Installation and Commissioning of the High Power, IOT Based, 300 KW CW Amplifier at<br />

Diamond<br />

The Diamond Light Source requires up to 900<br />

kW of RF power at 500 MHz to make up for<br />

radiation losses. This power will be supplied<br />

from three high power amplifiers provided<br />

by Thales. Each amplifier is capable of deliv-<br />

M. Jensen, M. Maddock, S.A. Pande, S. Rains, A. F. Rankin, D. Spink,<br />

A.V. Watkins (Diamond) J. Alex, M. Mueller (Thomson Broadcast<br />

& Multimedia AG)<br />

ering 300 kW through the combination of four 80 kW broadcast type IOTs. This paper provides an overview of the<br />

measurements of the key parameters following installation at Diamond, as well as the operating experience during<br />

initial storage ring beam commissioning.<br />

205<br />

TUPCH155<br />

TUPCH156<br />

TUPCH157

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