2012
DOI: 10.1364/ol.37.002709
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Parametrically shaped femtosecond pulses in the nonlinear regime obtained by reverse propagation in an optical fiber

Abstract: We present the experimental realization of a method to generate predetermined, arbitrary pulse shapes after transmission through an optical fiber in the nonlinear regime. The method is based on simulating the reverse propagation of the desired pulse shape in the fiber. First, linear and nonlinear parameters of a single-mode step-index fiber required for the simulation are determined. The calculated pulse shapes are then generated in a pulse shaper.

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Cited by 9 publications
(5 citation statements)
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“…The inverse problem at hand is much more complex: from a pulse shape and spectrum that are generated after propagation in the fiber, the properly trained network should be able to retrieve the parameters , N as well as the regime of dispersion of the fiber. One could tackle this inverse problem by using reverse propagation, that is, solving the NLSE to the backward direction [22,23]. However, this method would require knowledge of the peak power (or energy) of the pulse at the fiber output, whereas we only consider here the pulse shape characteristics.…”
Section: B/ Retrieval Of the Propagation Characteristicsmentioning
confidence: 99%
“…The inverse problem at hand is much more complex: from a pulse shape and spectrum that are generated after propagation in the fiber, the properly trained network should be able to retrieve the parameters , N as well as the regime of dispersion of the fiber. One could tackle this inverse problem by using reverse propagation, that is, solving the NLSE to the backward direction [22,23]. However, this method would require knowledge of the peak power (or energy) of the pulse at the fiber output, whereas we only consider here the pulse shape characteristics.…”
Section: B/ Retrieval Of the Propagation Characteristicsmentioning
confidence: 99%
“…Due to the unbalanced higher-order dispersion and unmatched propagation power in the SMF and in the DCF, such a pulse shaper is suboptimal. Other pulse shaper implementations that lend themselves to a more efficient fiber delivery of femtosecond laser pulses deserve future investigation [35].…”
Section: Discussionmentioning
confidence: 99%
“…As we noted in [24], the use of a reverse propagation method [39,40] to solve this problem would require proper knowledge of the peak power (or energy) of the pulse at the fibre output, whereas we only consider here the pulse shape characteristics.…”
Section: Retrieval Of the Propagation Characteristicsmentioning
confidence: 99%