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Wednesda , May 6

utomatic Frequency Matching for Cavity Warming-up in J- P RC Linac Digital LLRF Control T. Kobayashi (JAEA/J- PARC) S. Anami, Z. Fang, S. Michizono, S. Yamaguchi (KEK) H. Suzuki (JAEA)

Direct Sampling of rf Signal for 1.3 GHz Cavity Y. Okada (NETS) S. Fukuda, H. Katagiri, T. Matsumoto, S. Michizono, T. Miura, Y. Yano (KEK)

Study of Direct RF Feedback with the Pedersen Model L.- H. Chang, M.-C. Lin, Y.-H. Lin, C.H. Lo, Ch. Wang, M.-S. Yeh (NSRRC)

Energy Saving for Booster RF System in NSRRC M.-S. Yeh (NSRRC)

Status of the Spallation Neutron Source Prototype lator Ring LLRF System M.T. Crofford (ORNL)

ccumu-

SNS LLRF Control System Temperature Sensitivity Charac- terization M.F. Piller, M.T. Crofford, T.W. Hardek (ORNL) J.A.

Ball, T.L. Davidson, S.L. Jones (ORNL RAD)

High Intensity Beam Performance of the SNS

ccumulator

Ring LLRF Control System M.F. Piller, M.T. Crofford, T.W.

Hardek (ORNL) K. Smith (BNL)

Phase

mplitude

Detection

(P

D)

and

Phase

mplitude

Control (P C) for PXFEL W.H. Hwang, M.-H. Chun, K.M. Ha, Y.J. Han, D.T. Kim, S.H. Kim (PAL) R. Akre (SLAC)

pplication of Non-Linear Time-Domain RF Simulations to Longitudinal Emittance Studies for the LHC T. Mastorides, J.D. Fox, C.H. Rivetta, D. Van Winkle (SLAC)

Damping Effect Studies for X-Band High Gradient Structures

  • S. Pei, V.A. Dolgashe , Z. Li, S.G. Tantawi, J.W. Wang (SLAC)

Data

nalysis of

FL

SH S. Pei, C.

LLRF Measurement with Beam Off at Adolphsen (SLAC) J. Carwardine (ANL) N.J.

Walker (DESY)

Feedback Configuration Tools for LHC Low Level RF System

  • D. Van Winkle, J.D. Fox, T. Mastorides, C.H. Rivetta (SLAC) P.

Baudrenghien, A.C. Butterworth, J.C. Molendijk (CERN)

TRIUMF e-Linac RF Control System Design K. Fong, Q. Zheng (TRIUMF)

  • M.P. Laverty,

Beam Loading Effects on the RF Control Loops of a Double- Harmonic Cavity System for F IR D. Lens (TU Darmstadt, RTR) P. Hülsmann, H. Klingbeil (GSI)

RF System Modeling for the CEB F Energy Upgrade T. E. Plawski, C. Hovater (JLAB)

Vancouver BC, May 4 – 8

145

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