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Extra resources for The Supercontinuum Laser Source: Fundamentals with Updated References
27, 488. J. P. Stoicheff (1964) Induced absorption at optical frequencies. Phys. Rev. Lett. 13, 657. Lallemand, P. (1996) Temperature variation of the width of stimulated Raman lines in liquids. Appl. 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.
Lett. 6, 411. L. (1967) Molecular Scattering of Light. Plenum, New York, Chapter VIII. A. and W. Bischel (1975) Numerical studies of the interplay between selfphase modulation and dispersion for intense plane-wave light pulses. J. App. Phys. 46, 4921. , B. Suydam, and D. Yevich (1983) Optical phase conjugation for time domain undoing of dispersive self-phase modulation effects. Opt. Lett. 8, 611. V. Shank, C. Hirliman, and R. Yen (1983) Femtosecond white-light continuum pulses. Opt. Lett. 8, 1.
Maximum Stokes (Dw- < 0) and anti-Stokes (Dw+ > 0) shifts calculated with different models: simple theory of self-phase modulation (---); more rigorous theory without the self-steepening effect on the intensity pulse (–·–); more rigorous theory with the self-steepening effect (—). ) Dw w 0 Ӎ - Q sinh x cosh 2 x, (29) which is identical to the result one would ﬁnd from the simple theory of SPM. For Q տ 1, we expect spectral superbroadening with appreciable Stokes–antiStokes asymmetry and a maximum anti-Stokes shift Dw+ տ w 0.