1993
DOI: 10.1070/qe1993v023n06abeh003105
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Two-photon Raman processes in spectral ultrabroadening of intense ultrashort light pulses

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Cited by 5 publications
(14 citation statements)
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“…These properties are an instantaneous intensity-dependent cross section, continuous frequency-modulating and pulse reshaping. It has been shown that the 2π pulse RSIT in conditions of stimulated Raman self-scattering (SRSS)permit to generate a spectral supercontinuum [17][18][19][20]. First a breakup of a few-cycle 4π pulse into two 2π pulse was observed in our simulation on SRSS [21] with pulses containing three and four optical cycles (full width at half maximum (FWHM)).…”
Section: Introductionmentioning
confidence: 87%
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“…These properties are an instantaneous intensity-dependent cross section, continuous frequency-modulating and pulse reshaping. It has been shown that the 2π pulse RSIT in conditions of stimulated Raman self-scattering (SRSS)permit to generate a spectral supercontinuum [17][18][19][20]. First a breakup of a few-cycle 4π pulse into two 2π pulse was observed in our simulation on SRSS [21] with pulses containing three and four optical cycles (full width at half maximum (FWHM)).…”
Section: Introductionmentioning
confidence: 87%
“…We will consider the propagation of a laser pulse with duration τ which satisfies the condition SRSS [16][17][18][19][20][21][22]…”
Section: Basic Equationsmentioning
confidence: 99%
“…Continuous Stokes frequency shift with spectral broadening of femtosecond pulses under the condition of SRSS, in vibrational transitions, was experimentally observed in different media [14], when initial laser pulse duration τ o was below 100 fs. In [13,15] it was shown theoretically that under the condition of SRSS the continuous spectral broadening to Stokes direction occurred when the two-photon Rabi frequency Ω (2) , that corresponded to this stimulated Raman process, was less π/τ o . But for pulses with more intensity, when the two-photon Rabi frequency was more π/τ o (especially ∼ 2π/τ o ), the superbroadening to both anti-Stokes and Stokes direction, and the generation of spectral supercontinuum occurred [13,15].…”
Section: Introductionmentioning
confidence: 98%
“…In [13,15] it was shown theoretically that under the condition of SRSS the continuous spectral broadening to Stokes direction occurred when the two-photon Rabi frequency Ω (2) , that corresponded to this stimulated Raman process, was less π/τ o . But for pulses with more intensity, when the two-photon Rabi frequency was more π/τ o (especially ∼ 2π/τ o ), the superbroadening to both anti-Stokes and Stokes direction, and the generation of spectral supercontinuum occurred [13,15]. In addition, for some conditions a two-photon self-induced transparency (SIT) at SRSS for few-cycle laser pulses had been predicted and an equation for the change in the total energy had been derived [16].…”
Section: Introductionmentioning
confidence: 98%
“…For further consideration, it is convenient to introduce an angle of rotation of material variable [17][18][19]:…”
Section: Introductionmentioning
confidence: 99%