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Abstracts Brochure - CERN

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

Characterization of the PEP-II Colliding-beam Phase Space by the Boost Method<br />

We present a novel approach to characterize<br />

the colliding-beam phase space at the inter- M. Weaver (SLAC) W. Kozanecki (CEA)<br />

action point of the energy-asymmetric PEP-II<br />

B-Factory. The method exploits the fact that the transverse-boost distribution of e + e − –> mu+ mu- events reconstructed<br />

in the BaBar tracking system, reflects that of the colliding electrons & positrons. The average boost direction,<br />

when combined with the measured orientation of the luminous ellipsoid, determines the e + e − crossing angles.<br />

Varying the horizontal direction of one beam with respect to the other in a controlled fashion allows to estimate<br />

the individual e + and e − horizontal IP beam sizes. The angular spread of the transverse boost vector provides an<br />

accurate measure of the angular spread of the incoming high-energy beam, confirming the presence of a significant<br />

beam-beam induced increase of this angular spread. In addition, the longitudinal dependence of the angular spread<br />

of the boost vector in the y-z plane allows to extract from the continuously-monitored boost distributions, a weighted<br />

average of the vertical IP beta-functions & emittances of the two beams representative of routine high-luminosity<br />

operation.<br />

Ion-related Phenomenon in UVSOR/UVSOR-II Electron Storage Ring<br />

A vertical betatron tune shift depending on<br />

beam current under multibunch condition<br />

was observed in the UVSOR storage ring.<br />

Vertical tune increased as beam current de-<br />

A. Mochihashi, M. Hosaka, M. Katoh (UVSOR) Y. Hori (KEK) Y.<br />

Takashima (Nagoya University)<br />

creased, and the slope of the tune shift depended on the condition of the vacuum in the ring. Such a change in vertical<br />

tune was explained by a change in the stability condition of trapped ions*/** with the beam current. Based on a<br />

theoretical model*** that gives density of the trapped ions the experimental results were discussed via analytic and<br />

tracking calculations. Both the effect from the residual gas ions generated by scattering between high energy electrons<br />

and molecules and that from dissociated ions that come from secondary ionization processes have been discussed. In<br />

quest of the ion-related phenomenon in single-bunch condition, precise tune measurement has been also performed<br />

in the UVSOR-II storage ring. The experimental results in the single-bunch condition have been discussed. Precise<br />

measurement of vacuum pressure in the beam duct is a key issue of the ion-related phenomenon. A design of vacuum<br />

pressure measurement system via detecting residual gas fluorescence will be introduced in the presentation.<br />

*R. D. Kohaupt. DESY Internal. Bericht No.H1-71/2 (1971). **Y. Baconnier and G. Brianti. <strong>CERN</strong> Internal Report<br />

No.<strong>CERN</strong>/SPS/80-2(DI) (1980). ***A. Mochihashi et al. Jpn. J. Appl. Phys. 44 (2005) 430.<br />

Upgrade of Main RF Cavity in UVSOR-II Electron Storage Ring<br />

The UVSOR electron storage ring, which is<br />

dedicated to a synchrotron radiation (SR)<br />

light source especially for VUV and Soft Xray,<br />

has been improved at the beginning of<br />

A. Mochihashi, K. Hayashi, M. Hosaka, M. Katoh, J. Yamazaki<br />

(UVSOR) H. Suzuki (Toshiba) Y. Takashima (Nagoya University)<br />

2003, and transverse emittance in the improved ring (UVSOR-II)* has been decreased from 165nm-rad to 60 and/or<br />

27nm-rad. Users runs have been performed since September 2003 with 60nm-rad mode, and since then high brilliant<br />

SR beams have been supplied routinely for users. The 27nm-rad mode, however, was difficult to introduce to daily<br />

operation initially because Touschek lifetime was insufficient in such small emittance condition. To improve the beam<br />

lifetime and make full use of the SR beams, we have built new main RF cavity. The aim of the improvement was<br />

191<br />

TUPCH108<br />

TUPCH109<br />

TUPCH110

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