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As a result of the CSR kick, transverse emittance in the bending plane dilutes (Fig. 32). Note that the emittance growth by coherent synchrotron radiation is mainly a growth of the projection emittance; the growth of the slice emittance is not so large. Fig. 3 mm, p = 2 m, 0 = 20°, Q = 1 nC. (center) Deviation of bunch slices after bending due to CSR. (right) Emittance growth by CSR kick. 52 Femtosecond Beam Science As we have seen in Fig. 31, the power of coherent synchrotron radiation does not depend on the electron energy and is determined by geometrical conditions, such as curvature radius, bunch length and electron density.
1 RF cavity and laser The device called a photoinjector is a fascinating element of linear accelerators (linacs). The number of photoinjectors around the world is large and growing fast, and there is a large body of research on its many aspects. In this Section we will explore the science and technology of photoinjectors. 6-cell device developed at Brookhaven National Laboratory (BNL). We will start by explaining why a discussion of photoinjectors is relevant in a book dedicated to ultrashort pulses.
53) where z is the longitudinal coordinate of the electron, zo is the center of the bunch, w is the RF frequency and c is the speed of light. 54) and 7-70 70 - - Cc +1- C co c 2 2 co + -coc . 55) Eqs. 55) express the nonlinear energy modulation of the acceleration RF wave in an acceleration tube. Substituting Eq. 55) into Eq. 61) mainly conMaking 5’ zero gives perfect compression. Since [ is small, tributes to We choose the parameters of the chicane (D,Ro, L, L c ) and C1, C2, C3) so as to minimize [I.