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storage-ring

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MOP014 Observation of Sub-THz Coherent Radiation from the Linac Beam Injected in the NewSUBARU Storage Ring linac, injection, synchrotron, radiation 76
 
  • Y. Shoji
    LASTI, Hyogo
 
 

 Sub-THz coherent synchrotron radiation (CSR) from the SPing-8 linac beam was observed after the injection into the NewSUBARU storage ring. The beam from the linac has much sorter bunch length than the stationary stored bunch in the ring. It had been reported that the injected linac beam emits CSR at just after the injection until it diluted to a longer bunch by its energy spread. However we observed CSR at after more revolutions. At some tens of microseconds after the injection we observed CSR produced by a fine time structure in a bunch. At after more revolutions, a half of the synchrotron oscillation period (0.1 ms), CSR was back because the bunch length became shorter again. At this timing we also expect CSR emitted from a structure produced by longitudinal and transverse coupling, which should depend on the chromaticity. We report results of CSR observation through these periods.

 
WE202 Upgrade of Pohang Light Source (PLS) Linac for PLS-II* linac, klystron, gun, cavity 698
 
  • S.J. Park, W.H. Hwang, H.-G. Kim, J.M. Kim, K.R. Kim, M. Kim, S.H. Kim, S.-C. Kim, E.H. Lee, S.H. Nam, B.R. Park, S.S. Park, Y.J. Park, Y.G. Son
    PAL, Pohang, Kyungbuk
 
 

Since its completion in 1993, the PLS (Pohang Light Source) linear accelerator has been operated as the full energy injector to the PLS storage ring - a 2.5-GeV 3rd generation light source in Korea. After successful services for more than 15 years to the Korean synchrotron radiation users' community, the PLS is now being upgraded to meet ever-increasing user demands for brighter lights. The PLS-II, the major upgrade program to the PLS, is to increase the beam energy to 3 GeV, changing the storage ring lattice to accommodate large number of insertion devices with lower emittance, and to have the top-up injection as the default operating mode. In order to achieve high injection efficiency (> 80%), beam qualities including the energy spread, pulse length, and jitters in bunch arrival times to the storage ring rf bucket have to be reduced. After successful upgrade of the PLS linac one could further exploit its potential by, for example, implementing high-brightness electron source, which would open up new possibilities with the facility

 

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THP090 Modeling A Table Top Storage Ring For A Compact Light Source Using Electromagnetic Field Simulation Tools injection, synchrotron, electron, cavity 953
 
  • T. Roggen, H. De Gersem, J.P. Locquet, B. Masschaele
    KU Leuven, Kortrijk
  • M. Zhukova
    Tomsk Polytechnic University, Nuclear Physics Institute, Tomsk
 
 

Large synchrotron radiation facilities have become one of the most powerful instruments for research today. All over the world new facilities are being constructed or designed. The biggest disadvantage of a large synchrotron facility is that the scientific experiments, which are often very sensitive and complex, have to be performed in a dedicated place, sometimes far away from the researcher's home laboratory. Promising compact synchrotron radiation sources, that fit in a typical research lab, have been proposed recently. In this paper results are presented of an initial study of a single body magnet, low electron energy storage ring, performed with the Finite Element (FE) and Finite Difference Time-Domain (FDTD) modeling possibilities in the CST Studio Suite 2010 software package. Insights were obtained for the most crucial components: the magnet yoke, the internal RF cavity and the resonance injection component. Finally, the model of the storage ring was verified using the particle tracker solver which tracks the injected electrons along the ring.