Download Laser Handbook by M.L. Stitch (Eds.) PDF
By M.L. Stitch (Eds.)
Quantity four of the Laser instruction manual maintains the excessive commonplace set by means of the 1st 3 volumes that have been greatly acclaimed by way of a variety of reviewers in technology, Optical Spectra and Laser expertise, as offering a superb contribution to the sector of laser know-how
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10) By inserting eqs. 10) in the rhs of eq. , Blewett and Chasman 1977). **This is the typical configuration of a permanent magnet linear Undulator. 33 The free-electron laser derivatives (x\ y') with respect to the longitudinal one (z). 13) A"" Let us assume that the energy radiated by the electrons is a small fraction of the total energy. 11) is constant during the trip of the particle through the UM. 12) is constant because we have neglected the energy variation due to synchrotron emission. , Dattoli et al.
Therefore it is worthwhile to dedicate this full section to a detailed description of that device (an overview of the features relevant to the other FEL experiments will be given in §§ 9 and 10). 1 we briefly describe the experimental layout (both for the amplifier and the oscillator). e. the accelerator and the undulator magnet. 5. 1 The experimental layout The Stanford experiment has been developed in two main steps. In the first one (Elias et al. 6μιη), in small-signal regime, was performed.
23, bottom). From fig. 19 we can derive the following interesting features: (a) The power scale of the upper (above threshold) spectrum is 10 8 times larger than the lower (below threshold) one. This fact indicates a clear lasing action. (b) The laser linewidth is Fourier-transform limited by the length of the lasing medium pulses (the electron bunches). 3 ps, which corresponds to a linewidth Δω = 7r/Tb = 730 GHz which agrees very well with the experimental data (AX ~ 6nm => Δω ~ 1 0 3 GHz). 48 G.