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Additional info for The Scientific Papers of James Clerk Maxwell [Vol I]
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Baltuska, M. Uiberacker, E. Goulielmakis, R. Kienberger, V. Yakovlev, T. Udem, T. Hänsch, F. Krausz, Phase-controlled amplification of few-cycle laser pulses. IEEE J. Sel. Top. Quantum Electron. 9, 972 (2003) 15. L. Xu, C. Spielmann, A. Poppe, T. Brabec, F. W. Hänsch, Route to phase control of ultrashort light pulses. Opt. Lett. 21, 2008 (1996) 16. T. Brabec, Strong Field Laser Physics (Springer, Cambridge, 2008) 9 For shorter pulses, the saturation intensity is higher, allowing to drive HHG at higher intensities.
In a stable resonator, in which the beam lies in a single plane, this difference is caused by the difference of the effective radius of curvature of the (de)focusing mirrors thus, indicating the angles of incidence on these mirrors. g. be used to adjust the angles of incidence on the curved mirrors so that the Gouy parameters in both directions are equal. In this case all peaks corresponding to modes with the same sum of x and y indices coincide. In particular, this could be used to adjust quasi-imaging in both directions, see Sect.
Here, an octave-spanning frequency comb is employed to generate a beat signal between the mode with the number N and the one with the number 2N . g. by self-phase modulation in a nonlinear crystal. e. ω2N − ω N = ωCE . Controlling ωCE can be done in manifold ways. g. [31]. Recently, a related method was demonstrated in which a composite plate is used to vary this ratio without affecting the repetition rate [32]. g. [19, 20, 33] or by shifting the pumping beam with respect to the cavity mode [34].