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Liang, Z , and Hirschfield, J. L. (1982). Phys. Rev. Lett. 49, 1556. Elias, L. R, Fairbank, W. M , Madey, J. M. , Schwettman, H. , and Smith, T. I. (1976). Phys. Rev. Lett. 36, 717. Fleischmann, H. (1975). Today May, 35. Fly agin, V. , Luchinin, A. , and Nusinovich, G. S. (1982). Int. J. Infrared Millimeter Waves 3, 765. Freund, H. (1983). Phys. Rev. A 27, 1977. Goldstein, C, and Colson, W. B. (1982). Int. Conf. Lasers, New Orleans, Dec. 13-17. Granatstein, V. , Read, M. , and Barnett, L. R. (1982).
Pavelyev, V. E. (1983a). Rep. All-Union Conf. , 10th Minsk, Sept. 1, 182. Zapevalov, V. , Malygin, S. , and Sokolov, E. V. (1983b). Rep. All-Union Conf. , 10th, Minsk, Sept. 1, 189. Zarnitsyna, I. , and Nusinovich, G. S. (1974). Radiophys. Quantum Electron. 17, 1418. This page intentionally left blank INFRARED AND MILLIMETER WAVES, VOL. 13 CHAPTER 2 New High-Power Coherent Radiation Sources P. Sprangle and T. C. I. II. III. IV. V. GENERAL INTRODUCTION 19 FREE-ELECTRON LASERS 20 A. B. C. D. E.
COFFEY injection point the electrons are randomly phased and, in the absence of a force to bunch them, they would radiate incoherently, generating spontaneous magnetic bremsstrahlung radiation. The essential feature of the FEL mechanism is that the electrons undergo axial bunching in the combined wiggler and radiation fields. , Sprangle et al, and Colson and Ride). , 1980). To understand better the origin and central role played by the ponderomotive wave, we shall represent the wiggler magnetic field by B w = Bw cos(kwz)ey and the radiation electric and magnetic fields by (E R , BR) = ER cos(kz — cot)(ex, ey).