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Koseki, K.

Paper Title Page
WEPLT110 Specific Beam Dynamics in Super-bunch Acceleration 2107
 
  • Y. Shimosaki, E. Nakamura, K. Takayama, T. Toyama
    KEK, Ibaraki
  • K. Horioka, M. Nakajima
    TIT, Yokohama
  • K. Koseki
    GUAS/AS, Ibaraki
  • K. Torikai
    Kyushu University, Fukuoka
  • M. Watanabe
    RIKEN, Saitama
 
  Proof-of-principle experiments on the induction synchrotron concept using the KEK 12-GeV PS makes progress, in which RF bunches and a super-bunch will be accelerated with a long step voltage generated in the induction accelerating gaps. In order to give a guide for super-bunch acceleration, the beam stabilities against a droop and a fluctuation of the accelerating voltage have been examined by using a simulation. The droop voltage gives an additional focusing or defocusing force in the longitudinal direction, which leads the mismatching beyond the transition energy. Furthermore, the extremely slow fluctuation of the accelerating voltage causes a lowest-order resonance near the transition. These induce a serious emittance blow-up in the longitudinal, so that the compensating manners will be presented. Moreover, the other issues such as head-tail instability and intra beam scattering will be discussed.  
MOPLT066 Induction Accelerating Cavity for a Circular Ring Accelerator 704
 
  • K. Torikai, Y.A. Arakida, T. Kono, K. Koseki, E. Nakamura, Y. Shimosaki, K. Takayama, T. Toyama, M. Wake
    KEK, Ibaraki
  • J. Kishiro
    JAERI/LINAC, Ibaraki-ken
 
  This paper reports details of an induction accelerating cavity employed for induction synchrotron POP experiments [*] using the KEK 12GeV PS. This cavity is the first induction cavity in the history of accelerator that is used in a circular ring. We focus our attention on crucial aspects distinguished from well-know properties of RF cavity. The single cavity is capable of generating an acceleration voltage of 2.5kV with a pulse width of 250ns, which is operated at a repetition rate in the range of 667kHz - 882kHz. The cavity is driven by its own pulse modulator through a 25m long transmission cable of 125W, the end of which is connected with a matching resistance so as to minimize reflection in a wide range of frequency. Accelerating field characteristics are discussed and matching features of the cavity as a one-to-one transformer are presented. A longitudinal and transverse coupling impedance have been measured using a net-work analyzer.

* K.Takayama et al., 'POP Experiments of the Induction Synchrotron' in this conference