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booster

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TUPSM009 Operational Use of Ionization Profile Monitors at Fermilab proton, injection, emittance, lattice 111
 
  • J.R. Zagel, A. Jansson, T. Meyer, D.K. Morris, D. Slimmer, T. Todd, M.-J. Yang
    Fermilab, Batavia
 
 

Ionization profile monitors (IPMs) are installed in the Fermilab Booster, Main Injector and Tevatron. They are used routinely for injection matching measurements. For emittance measurements the IPMs have played a secondary role to the Flying Wires, with the exception of the Booster (where it is the only profile diagnostics). As Fermilab is refocusing its attention on the intensity frontier, non-intercepting diagnostics such as IPMs are expected to become even more important. This paper gives an overview of the operational use of IPMs for emittance and injection matching measurements at Fermilab, and summarizes the future plans.

 
TUPSM065 Injection Beam Dynamics in SPEAR3 injection, synchrotron, betatron, storage-ring 318
 
  • W.J. Corbett, A.S. Fisher
    SLAC, Menlo Park, California
  • W.X. Cheng
    BNL, Upton, Long Island, New York
  • W.Y. Mok
    Life Imaging Technology, Palo Alto, California
 
 

For top-up injection it is important to understand the time evolution of the incident charge in the transverse and longitudinal coordinate systems. In SPEAR3, the injection system has a vertically-deflecting Lambertson septum with the injected beam entering ~13mm to the inside. The resulting large-amplitude betatron oscillations give rise to rapid filamentation followed by nominal radiation damping and in some cases non-linear x-y coupling. Similarly, in the longitudinal dimension, a mis-match in beam arrival time or energy can result non-linear beam dynamics and damped synchrotron motion. To the next order, any betatron, bunch length or energy spread mismatch will generate damped ‘quadrupole’ oscillations or even higher-order motion. In this paper we report on measurements of injection beam dynamics in the transverse and longitudinal coordinate systems using a fast-gated, image-intensified CCD camera and a Hamamatsu C5680 streak camera, respectively. The injection beam dynamics are shown to contain relatively complicated evolution in the x-y-z beam distributions that change with injection conditions and storage ring lattice configuration.

 
TUPSM073 Tune Measurement System at the ALBA Booster synchrotron 350
 
  • U. Iriso, F. Peréz, A. Salom
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The ALBA Booster synchrotron is designed to ramp an electron beam of up to 4 mA from 100 MeV to 3 GeV in a 3 Hz cycle. The Booster is equipped with two common λ/4 striplines for tune excitation and precise beam position measurement. Beam excitation along the cycle requires the amplitude kick to increase synchronously with the energy ramp. This paper shows the excitation and measurement system at ALBA, including both mechanical and hardware instrumentation as well as control system functionalities.

 
TUPSM074 Diagnostics During the ALBA Booster Commissioning linac, dipole, synchrotron, diagnostics 353
 
  • U. Iriso, M. Alvarez, R. Muñoz, A. Olmos, F. Peréz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The ALBA Booster is a synchrotron designed to accelerate electron beam from 100 MeV to 3 GeV in a 3 Hz cycle. The maximum pulse coming from the ALBA Linac provides 4 mA in the Booster. In order to check all the Booster sub-systems, a Booster pre-commissioning took place during two weeks between December 2009 and January 2010. This paper presents the Diagnostics elements installed in the ALBA Booster and our experience during the Booster pre-commissioning.

 
TUPSM075 Beam Position Monitors Characterization for ALBA storage-ring, vacuum, monitoring, synchrotron 356
 
  • A. Olmos, M. Alvarez, F. Peréz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

Beam position monitors (BPM) characterization has been widely studied at ALBA Synchrotron Light Source. Special care has been taken on the analysis of their electrical offset in order to achieve submicron beam stabilities. This paper shows the results of the BPMs offset study for Booster and Storage Ring. The electrical effect of the different vacuum vessels housings the BPMs is also reported.

 
TUPSM085 Microwave Link Phase Compensation for Longitudinal Stochastic Cooling in RHIC pick-up, kicker, cavity, controls 389
 
  • K. Mernick, M. Blaskiewicz, J.M. Brennan, B.R. Johnson, F. Severino
    BNL, Upton, Long Island, New York
 
 

A new microwave link has been developed for the longitudinal stochastic cooling system, replacing the fiber optic link used for the transmission of the beam signal from the pickup to the kicker. This new link reduces the pickup to kicker delay from 2/3 of a turn to 1/6 of a turn, which greatly improves the phase margin of the system and allows operation at higher frequencies. The microwave link also introduces phase modulation on the transmitted signal due to variations in the local oscillators and time of flight. A phase locked loop tracks a pilot tone generated at a frequency outside the bandwidth of the cooling system. Information from the PLL is used to calculate real-time corrections to the cooling system at a 10 kHz rate. The design of the pilot tone system is discussed and results from commissioning are described.

 

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Poster

 
TUPSM098 NSLS-II Injector System Diagnostics diagnostics, linac, controls, injection 437
 
  • D. Padrazo, R.P. Fliller, Y. Hu, B.N. Kosciuk, R. Meier, I. Pinayev, T.V. Shaftan, O. Singh
    BNL, Upton, Long Island, New York
 
 

The NSLS-II Injector System Diagnostics will provide instrumentation in the Linac, Booster, transfer lines and beam dumps for measuring key beam parameters. These instruments will be adequate in providing staged commissioning of NSLS-II injectors, as well as allowing sufficient beam diagnostics for tune-up and top up operations. This paper will summarize the progress and implementation status of the NSLS-II injector system diagnostics.

 

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Poster

 
TUPSM103 Recent Upgrade of the PITZ Facility laser, gun, electron, cavity 459
 
  • J.W. Bähr, A. Brinkmann, K. Flöttmann, S. Lederer, F. Obier, D. Reschke, S. Schreiber
    DESY, Hamburg
  • W. Ackermann, W.F.O. Müller, S. Schnepp, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
  • H.M. Al-Juboori, A. Donat, U. Gensch, H.-J. Grabosch, L. Hakobyan, R. Heller, M. Hänel, Ye. Ivanisenko, L. Jachmann, M.A. Khojoyan, G. Klemz, W. Köhler, G. Koss, M. Krasilnikov, A. Kretzschmann, H. Leich, M. Mahgoub, J. Meissner, D. Melkumyan, M. Otevrel, M. Penno, B. Petrosyan, M. Pohl, S. Rimjaem, C. Rueger, M. Sachwitz, B. Schoeneich, J. Schultze, A. Shapovalov, F. Stephan, M. Tanha, G. Trowitzsch, G. Vashchenko, L.V. Vu, T. Walther, X.H. Wang, S. Weisse, R.W. Wenndorff, M. Winde
    DESY Zeuthen, Zeuthen
  • G. Asova, A. Bonev, I.I. Tsakov
    INRNE, Sofia
  • D.J. Holder, B.L. Militsyn, B.D. Muratori
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • P.M. Michelato, L. Monaco, C. Pagani, D. Sertore
    INFN/LASA, Segrate (MI)
  • V.V. Paramonov
    RAS/INR, Moscow
  • D. Richter
    Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Berlin
  • J. Roßbach, J. Rönsch-Schulenburg
    Uni HH, Hamburg
  • J. Saisut
    FNRF, Chiang Mai
  • W. Sandner, I. Will
    MBI, Berlin
 
 

The Photo Injector Test facility at DESY Zeuthen site (PITZ) is dedicated to developing and optimizing high brightness electron sources for short wavelength Free-Electron Lasers (FELs) like FLASH and the European XFEL, both in Hamburg (Germany). Since October 2009 a major upgrade has been ongoing with the goal of improving the accelerating components, the photocathode drive laser system, and the beam diagnostics. The previously operated and fully characterized gun was brought to FLASH and will go into operation soon. A gun of the same type is installed now in PITZ. The conditioning has started and the gun will be characterized throughout 2010. A new booster cavity, Cut Disk Structure (CDS), was developed and will be mounted at PITZ in spring 2010. The booster cavity will be able to accelerate electrons above 20 MeV/c and will be suitable for long RF pulses. The most important upgrade of the diagnostics system will be the implementation of a phase space tomography module (PST) consisting of three FODO cells each surrounded by two screen stations. The results of commissioning, gun and booster conditioning and the very first measurements will be reported.

 
TUPSM110 Synchrotron Light Monitor System for NSLS-II radiation, synchrotron, diagnostics, synchrotron-radiation 478
 
  • W.X. Cheng
    BNL, Upton, Long Island, New York
 
 

A synchrotron light diagnostic beamline has been designed at the NSLS-II storage ring, using the dipole radiations. A "cold-finger" configuration has been selected to block the central x-rays. Beam power on the first mirror is less than 1 W, so no water cooling was required for this in-vacuum mirrors. The beamline layout and major applications will be discussed in this paper. Two vacuum ports are reserved in the NSLS2 booster ring to monitor the transverse profile as well as bunch length measurement during ramping. There will be a synchrotron light port in the BTS transport line for observing the injecting beam behavior during top-up operation.