2016
DOI: 10.1364/josab.34.002721
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Pulse train uniformity and nonlinear dynamics of soliton crystals in mode-locked fiber ring lasers

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Cited by 7 publications
(4 citation statements)
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“…Such growth is driven by an instability-induced dynamical transition of the cw laser propagating in nonlinear optical media. The instability-induced dynamical transition, so-called modulational instability [13][14][15][16][17][18][19], involves the cw instability and its breakup into a high-power laser field leading ultimately to a pulse via a regime dominated by pulse-train structures [20][21][22]. Hence operating lasers in micromachining processings requires a good understanding of its characteristic dynamics.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Such growth is driven by an instability-induced dynamical transition of the cw laser propagating in nonlinear optical media. The instability-induced dynamical transition, so-called modulational instability [13][14][15][16][17][18][19], involves the cw instability and its breakup into a high-power laser field leading ultimately to a pulse via a regime dominated by pulse-train structures [20][21][22]. Hence operating lasers in micromachining processings requires a good understanding of its characteristic dynamics.…”
Section: Introductionmentioning
confidence: 99%
“…In nonlinear optical materials in particular the problem can be translated into the issue of laser self-starting dynamics [16][17][18][19], where it is assumed that the optical pump is a cw field whose amplitude can grow upon propagation until a critical amplitude. Beyond this amplitude the cw mode will become modulationally unstable, typically this instability will first generate weakly nonlinear pulse trains [20][21][22][23] which decay subsequently into high-intensity temporal pulses.…”
Section: Introductionmentioning
confidence: 99%
“…Passively mode-locked lasers have been the subject of intensive research [1][2][3][4][5][6][7][8][9][10][11] because of their ability to produce pulses of very short durations (of the order of sub-picoseconds as well as femtoseconds). Fiber lasers with saturable absorbers in particular have attracted a great deal of attention; in the specific context of their standard setup where the gain medium is an optical fiber with weak nonlinearity, the propagation of the pump field is commonly described by the complex Ginzburg-Landau equation (CGLE) with cubic nonlinearity [1,6,12,13].…”
Section: Introductionmentioning
confidence: 99%
“…Passively mode-locked fiber lasers can display a wealth of operation regimes, including continuous-wave (cw), soliton, period-doubling, multi-pulse, and chaotic [5,[8][9][10][11][24][25][26][27][28][29]. However, in most applications, there is a desire that the laser operate in the pulse regime.…”
Section: Introductionmentioning
confidence: 99%