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Abstracts Brochure - CERN

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

device sources and for damping wigglers to reduce emittance. The dispersive regions can be designed to minimize<br />

the strength of the chromatic correction sextupoles. A key constraint is the imposition of a limit on circumference<br />

which is closely tied to cost. We discuss optimization of the dynamic aperture by minimizing the non-linear driving<br />

terms using high-order achromatic cancellation in the non-linear lattice.<br />

Control of Dynamic Aperture with Insertion Devices<br />

It is well known that insertion devices (IDs)<br />

perturb the linear optics in the vertical plane. T.V. Shaftan, J. Bengtsson, S.L. Kramer (BNL)<br />

In particular, that the effect can be corrected<br />

locally by a symmetric arrangement of four quadrupoles on each side of the IDs. We show how to control an arbitrary<br />

set of IDs in this configuration with the response matrix for the beta-beat and perturbation of the phase advance and<br />

SVD, i.e., to maintain the dynamic aperture. We also evaluate the residual impact on the dynamic aperture from the<br />

nonlinear terms and outline how to control these. As an example, we discuss an impact of some ID models on the<br />

NSLS-2 dynamic aperture. Results for a single ID and a set of 20 IDs with random field strengths are presented.<br />

Nb-Pb Superconducting RF Gun<br />

We report on the status of an electron RF-gun<br />

made of two superconductors: niobium and<br />

lead. The presented design combines the advantages<br />

of the RF performance of bulk niobium<br />

superconducting cavities and the reasonably<br />

high quantum efficiency of lead, as<br />

compared to other superconducting metals.<br />

The concept, mentioned in a previous paper,<br />

J.S. Sekutowicz, J.I. Iversen, D. Klinke, D. Kostin, W.-D. Möller<br />

(DESY) I. Ben-Zvi, T. Rao, J. Smedley (BNL) M. Ferrario (INFN/<br />

LNF) P. Kneisel (Jefferson Lab) K. Ko, L. Xiao (SLAC) J. Langner,<br />

P.S. Strzyzewski (The Andrzej Soltan Institute for Nuclear Studies,<br />

Centre Swierk) A.R. Lipski (SBUNSL) J.B. Rosenzweig (UCLA) K.<br />

Szalowski (University of Lodz)<br />

follows the attractive approach of all niobium superconducting RF-gun as it has been proposed by the BNL group.<br />

Measured values of quantum efficiency for lead at various photon energies, analysis of recombination time of photonbroken<br />

Cooper pairs for lead and niobium, and preliminary cold test results are discussed in this paper.<br />

Status of the Photocathode RF Gun System at Tsinghua University<br />

An S-band high gradient photocathode RF<br />

gun test stand is in construction process at<br />

Tsinghua University. The photocathode RF<br />

gun test stand is a primary step of a femtosec-<br />

X. He, Cheng. Cheng. Cheng, Q. Du, Du.Taibin. Du, Y.-C. Du,<br />

W.-H. Huang, Y. Lin, C.-X. Tang, S. Zheng (TUB)<br />

ond hard x-ray source based on Thomson scattering. The photocathode RF gun system adopts Ti:Sap laser, BNL IV<br />

type 1.6 cell RF gun, compact compensation solenoid. We foresee to conduct investigations on the thermal emittance<br />

contribution of surface roughness, the emittance compensation technique under various laser shape and its application<br />

to Thomson scattering x-ray source. Except for the transportation of laser, correction of laser front for glazing<br />

incidence and laser pulse shaping system, other parts of the photocathode RF gun test stand have been constructed,<br />

and we can start very primary experiment on the RF gun test stand, such as measurements of dark current, QE and<br />

energy of the beam. The experimental results are reported.<br />

473<br />

THPLS091<br />

THPLS092<br />

THPLS093

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