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Shevchenko, O. A.

Paper Title Page
MOCAU02 Numerical Solution of the FEL Correlation Function Equation 188
 
  • N. Vinokurov, O. A. Shevchenko
    BINP SB RAS, Novosibirsk
 
  The equation for two-particle correlation function in FEL was derived recently to provide a new way of noise calculations in FELs*. In this paper this equation is solved numerically for the simplest case of narrow electron beam. Time independent solution with saturation is obtained. It is compared with the results of quasilinear theory and results of previous SASE linewidth estimates.

* O. A. Shevchenko, N. A. Vinokurov, NIM A507 (2003) 84-88

 
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TUAAU02 Electron Outcoupling Scheme for the Novosibirsk FEL 204
 
  • O. A. Shevchenko, V. G. Tcheskidov, N. Vinokurov, A. N. Matveenko
    BINP SB RAS, Novosibirsk
 
  One of the main problems of contemporary high power FELs is the mirror heating. One of the possible solutions of this problem is the use of electron outcoupling*. In this case the mirrors of optical resonator are not transparent and the coherent radiation from an additional undulator in the FEL magnetic system is used. To provide the output of this radiation the electron beam in the auxiliary undulator is deflected from the optical resonator axis. To save bunching it is preferable to use the achromatic deflecting bend. The project of electron outcoupling for the Novosibirsk FEL is described. Simulation results are presented.

* N. G. Gavrilov et al., NIM A304 (1991) 63-65

 
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TUPPH014 Generation of X-ray FEL Light Using Laser Wakefield Accelerated Electron Beams 252
 
  • A. Rousse, K. Ta Phuoc
    LOA, Palaiseau
  • N. Vinokurov, O. A. Shevchenko
    BINP SB RAS, Novosibirsk
 
  We consider a new class of high gain FELs based on femtosecond electron bunches with extra high current density produced by Laser Wake Field Acceleration (LWFA). The FELs of this kind can be used for generation of high power femtosecond x-ray pulses. We present the results of simulations of FEL operation with some reasonable beam parameters which will be obtained in future. We focus our attention on the advantages which can be gained from the unique possibility of the use of femtosecond hundred-kiloamperes bunches, generated by LWFA. We also consider the impact of the relatively poor electron beam properties on FEL characteristics.  
MOPPH044 Status of Novosibirsk ERL and FEL  
 
  • N. Gavrilov, B. A. Knyazev, E. I. Kolobanov, V. V. Kotenkov, V. V. Kubarev, G. N. Kulipanov, A. N. Matveenko, L. E. Medvedev, S. V. Miginsky, L. A. Mironenko, V. Ovchar, V. M. Popik, T. V. Salikova, M. A. Scheglov, S. S. Serednyakov, O. A. Shevchenko, A. N. Skrinsky, V. G. Tcheskidov, N. Vinokurov
    BINP SB RAS, Novosibirsk
 
  The Novosibirsk terahertz free electron laser is based on the energy recovery linac (ERL) with room-temperature radiofrequency system. Some features of the ERL are discussed. The results of emittance measurements and electron optics tests are presented. The first stage of Novosibirsk high power free electron laser (FEL) was commissioned in 2003. Now the FEL provides electromagnetic radiation in the wavelength range 110 - 230 micron. The average power is 400 W. The minimum measured linewidth is 0.3%, which is close to the Fourier-transform limit. Four user stations are in operation. The second stage of the ERL, which has four orbits, is under construction.  
FRAAU03 Compact Ring FEL as a Source of High Power Infrared Radiation 517
 
  • A. N. Matveenko, N. Vinokurov, O. A. Shevchenko
    BINP SB RAS, Novosibirsk
 
  Ring FELs* were proposed mainly to improve the quality of radiation of x-ray FELs. Their main advantage is the absence of mirrors. It appears that this advantage is also useful for high power FELs. Another reason to build infrared ring FEL is the proof-of-principle for shorter wavelength FELs. Therefore we considered the scheme of infrared ring FEL which requires ERL with beam energy 50 MeV. Using extensive simulations we developed requirements for electron beam parameters and magnetic system of ring FEL. In spite of rather compact design such FEL may provide more than 10 kW average power.

* N. A. Vinokurov, O. A. Shevchenko, NIM A528 (2004) 491-496

 
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