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Extra resources for The Supercontinuum Laser Source: Fundamentals with Updated References

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2c ˚ (5) The main physics behind the supercontinuum generation by self-phase modulation is contained in Eq. 1. 1a, the index change becomes time dependent and, therefore, the phase of a pulse propagating in a distorted medium becomes time dependent, resulting in self-phase modulation. 1c) in time. This process is most important in the generation of femtosecond pulses (see Chapter 10 by Johnson and Shank). 1. A simple mechanism for SPM for a non-linear index following the envelope of a symmetrical laser pulse: (a) time-dependent nonlinear index change; (b) time rate of change of index change; (c) time distribution of SPM-shifted frequencies w(t) - w 0.

Phys. Lett. 8, 276. T. R. Shen (1973) Study of self-focusing and small-scale filaments of light in nonlinear media. IEEE J. Quantum Electron. QE-9, 409. R. Shapiro, and M. Mustafa (1985) Spectral distribution of an ultrashort supercontinuum laser source. Phys. Lett. A107, 305. A. R. P. Ho (1986) Spectral extent and pulse shape of the supercontinuum for ultrashort laser pulse. IEEE J. Quantum Electron. QE-22, 197. H. (1975) Self-focusing: theory. Prog. Quantum Electron. 4, 35. Nakatsuka, H. and D.

Q. Wang, T. P. Ho (1987) Induced spectral broadening about a second harmonic generated by an intense primary ultrashort laser pulse in ZuSe. Phys. Rev. A 35, 459. Bloembergen N. and P. Lallemand (1966) Complex intensity-dependent index of refraction, frequency broadening of stimulated Raman lines, and stimulated Rayleigh scattering. Phys. Rev. Lett. 16, 81. G. (1967) Frequency shifts in self-focusing light. Phys. Rev. Lett. 19, 8. P. M. Rentzepis (1973) Picosecond spectroscopy using a picosecond continuum.

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