2015
DOI: 10.1364/oe.23.029660
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Effect of narrow spectral filter position on the characteristics of active similariton mode-locked femtosecond fiber laser

Abstract: A significant change in active similariton characteristics, both numerically and experimentally, is observed as a function of the location of the lumped spectral filter. The closer the spectral filter is to the input of the Yb(3+)-doped fiber, the shorter the de-chirped pulse width. The peak power of the de-chirped pulse has its maximum value at a certain location of the spectral filter. Four different positions of the spectral filter inside the laser cavity have been theoretically studied and two of them have… Show more

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Cited by 10 publications
(5 citation statements)
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“…The model was used to study the effect of the input pulse parameters on the output pulse shape after propagating through the normal dispersion gain medium. The excess kurtosis factor 𝐾 is used to indicate the output pulse shape [13], [28], [29], where the values of -1.2, -1, -0.86, −0.594, 0, and 1.2 are for rectangular, semicircle, parabolic, raised cosine, Gaussian and sech squared > REPLACE THIS LINE WITH YOUR MANUSCRIPT ID NUMBER (DOUBLE-CLICK HERE TO EDIT) < pulse shapes, respectively. The excess kurtosis for the pulse in the time domain is calculated as [30]:…”
Section: Resultsmentioning
confidence: 99%
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“…The model was used to study the effect of the input pulse parameters on the output pulse shape after propagating through the normal dispersion gain medium. The excess kurtosis factor 𝐾 is used to indicate the output pulse shape [13], [28], [29], where the values of -1.2, -1, -0.86, −0.594, 0, and 1.2 are for rectangular, semicircle, parabolic, raised cosine, Gaussian and sech squared > REPLACE THIS LINE WITH YOUR MANUSCRIPT ID NUMBER (DOUBLE-CLICK HERE TO EDIT) < pulse shapes, respectively. The excess kurtosis for the pulse in the time domain is calculated as [30]:…”
Section: Resultsmentioning
confidence: 99%
“…The forward direction ASE is calculated using the same numerical method as that of the backward direction (solving (5) with a positive sign). The electric field envelopes are calculated by using the fourth-order Runge-Kutta split-step Fourier transform algorithm [13], [23]- [25] to solve the coupled nonlinear Schrödinger's equations (CNLSEs) given by [15], [26], [27]:…”
Section: Numerical Modelmentioning
confidence: 99%
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“…Then, we have followed the derivation of the nonlinear Schrödinger equation (NLSE), a PDE that describes the propagation in dispersive and nonlinear mediums [27]. It has been solved numerically before by using the split-step Fourier method (SSFM) [27,44] and this solution is developed and considered in RONST too [45][46][47][48][49][50]. The SSFM is a numerical technique that behaves much faster when compared to the conventional finite-difference methods [44].…”
Section: Numerical Modeling Approachmentioning
confidence: 99%
“…Solitons, which are the localized formations in nonlinear systems 1 , appear in various physical settings 2 3 4 5 6 7 8 9 10 11 12 13 14 15 . The soliton on a water surface was first described by John Scott Russell and the fundamental concept of soliton in mathematical physics was first introduced by Norman Zabusky and Martin Kruskal 10 11 .…”
mentioning
confidence: 99%