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Abstracts Brochure - CERN

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THPCH088<br />

THPCH089<br />

THPCH090<br />

29-Jun-06 16:00 - 18:00 THPCH — Poster Session<br />

this cavity lies in the simple geometry with no need for vacuum inside the cavity and high shunt impedance despite<br />

an internal ferrite load. The ferrite load is succesfully used to dampen higher order modes down to Q < 50 while the<br />

fundamental mode is damped by less than 2 dB. While nominal input power is rated at 60 dBm the cavity is prepared<br />

to handle beam loading. In spite of power requirements and ferrite load the cavity needs no active cooling. It can be<br />

tuned in center frequency and bandwidth over a range of 96..105 MHz and 4..7 MHz respectively and in consequence<br />

provides an optimal actuator for the particle beam control system. Presented will be the design details, all relevant<br />

parameters, the design of the internal ferrite load and operational experience.<br />

A Possibility of Constant Energy Extraction at the KEK ATF<br />

Beam energy oscillations of the order of<br />

A. Kalinin (CCLRC/DL/ASTeC)<br />

0.02% take place at the KEK ATF. With extractions,<br />

the synchrotron oscillation amplitude<br />

and phase at the extraction turn randomly fluctuates. The energy jitter causes a position/angle jitter in the<br />

Diagnostic section of the Extraction Line. To reduce it, a feed forward energy stabilisation can be used done by<br />

extraction of the beam at the turn next to that turn at which the energy passes the equilibrium value. For this,<br />

the synchrotron oscillation is measured by a turn-by-turn BPM as a horizontal position oscillation. A fast turn-byturn<br />

processor detects the turn where the oscillation passes zero, and generates an extraction permission signal that<br />

triggers the existing ATF Extraction system. Stability improvement by factor of 10 can be obtained even when the<br />

extraction is done with uncertainty up to three turns after the trigger.<br />

The Electromagnetic Background Environment for the Interaction-point Beam Feedback<br />

System at the International Linear Collider<br />

The Interaction Point (IP) feedback system is<br />

G.B. Christian (JAI)<br />

essential for maintaining the luminosity at<br />

the International Linear Collider (ILC). It is<br />

necessary to demonstrate the performance of the feedback beam position monitor (BPM) in an electron-positron<br />

pair background similar to that expected in the ILC interaction region (IR). We have simulated the ILC beam-beam<br />

interactions and used a GEANT model of the IR to evaluate the pair and photon flux incident on the BPM, for both the<br />

2 mrad and 20 mrad crossing angle geometries. We present results as a function of the proposed machine parameter<br />

schemes, as well as for various system layouts within the IR. We plan to study the degradation of BPM resolution,<br />

and the long term survivability, in beam tests at End Station A at SLAC. To simulate the background environment of<br />

the ILC a ’spray beam’ will be produced, which will scatter from a mechanical mock-up of the forward region of the<br />

IR, and irradiate the BPM with realistic flux of secondary pairs. We present the proposed experimental layout and<br />

planned beam tests.<br />

Stabilization of the ILC Final Focus Using Interferometers<br />

We are developing a system of interferom-<br />

D. Urner, P.A. Coe, A. Reichold (OXFORDphysics)<br />

eters that can measure the relative motion<br />

between two objects (such as the two final<br />

focus quadrupoles) to a few nanometers using interferometric methods. Two instruments are developed at the John<br />

Adams Institute at University of Oxford: A distance meter to measure length changes and a straightness monitor to<br />

412

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