2010
DOI: 10.1364/josab.27.001751
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Conical emission in β-barium borate under femtosecond pumping with phase matching angles away from second harmonic generation

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Cited by 12 publications
(6 citation statements)
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“…Filamentation under the conditions of phasematched second-order nonlinear effects has led to SC generation, which is accompanied by simultaneous wavelength-tunable second harmonic or sum frequency generation, as experimentally observed in basic nonlinear crystals, such as KDP [229,230] and β-barium borate (β-BBO) [231,232].…”
Section: Birefringent Crystalsmentioning
confidence: 97%
“…Filamentation under the conditions of phasematched second-order nonlinear effects has led to SC generation, which is accompanied by simultaneous wavelength-tunable second harmonic or sum frequency generation, as experimentally observed in basic nonlinear crystals, such as KDP [229,230] and β-barium borate (β-BBO) [231,232].…”
Section: Birefringent Crystalsmentioning
confidence: 97%
“…A similar treatment was given to the study of parametric down and up conversion [24,25]. For related experiments involving the process of parametric up conversion of the vacuum, see the work in [26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, the SPDC under a strongly focused pump has been studied, and a broadening effect of the far-field SPDC ring has been found, which is explained as a result of the transverse momentum spreading, making the phase-matching range extend beyond that for the initial focused pump beam [37,38]. In our experiment, the generated SPDC peak intensity is estimated to be on the order of 100 GW/cm 2 , exceeding the critical intensity for self-focusing in the BBO crystal or even approaching the minimum intensity required for WLSC generation [12]. It is thus expected that in our experiment, the intense femtosecond pulses are subject to self-focusing from optical Kerr nonlinearity [23].…”
Section: Resultsmentioning
confidence: 59%
“…Meanwhile, when intense light propagates in a transparent medium including quadratic nonlinear crystals, modulation instability usually occurs due to the interplay of optical Kerr nonlinearity and group velocity dispersion or diffraction, producing an exponential growth of perturbations during photon-medium interactions [10]. For example, away from phase-matching conditions of second-harmonic generation (SHG), BBO and KDP crystals could produce white-light supercontinuum (WLSC) in the center of the beam and colored conical emission (CCE) rings surrounding the white core [11,12]. Interestingly, when the phase-matching condition for SHG is satisfied, the spatiotemporally coupled modulation instability in a quadratic crystal can result in a series of bright cyan rings [13][14][15].…”
Section: Introductionmentioning
confidence: 99%