2012
DOI: 10.1109/lpt.2012.2208100
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Multiwavelength Dissipative-Soliton Generation in Yb-Fiber Laser Using Graphene-Deposited Fiber-Taper

Abstract: We propose and demonstrate multiwavelength dissipative soliton (DS) generation in an all-normal-dispersion ytterbium-doped fiber laser based on a graphene-deposited tapered fiber (GDTF) device. Due to the interaction of the graphene with the evanescent field on the taper, the GDTF device possesses the characteristics of both saturable absorption and polarizing effect. Therefore, this device not only initiates the mode-locking operation based on the saturable absorption, but also induces both the special spectr… Show more

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Cited by 59 publications
(21 citation statements)
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“…Due to the simultaneous generation of pulses at different wavelengths, multiwavelength pulsed fiber lasers possess versatile applications in wavelength division multiplexing systems, fiber-optic sensors, and optical spectroscopy. To date, several passively mode-locked techniques such as semiconductor saturable absorber (SESAM) [1], [2], nonlinear polarization rotation (NPR) [3], [4], nonlinear amplifying loop mirror (NALM) [5], carbon nanotubes (CNT) [6], [7], graphene [8] and topological insulator [9] have been used to achieve multiwavelength passively mode-locked pulses in fiber lasers. However, all the multiwavelength pulses mentioned above are hyperbolic secant pulses.…”
Section: Introductionmentioning
confidence: 99%
“…Due to the simultaneous generation of pulses at different wavelengths, multiwavelength pulsed fiber lasers possess versatile applications in wavelength division multiplexing systems, fiber-optic sensors, and optical spectroscopy. To date, several passively mode-locked techniques such as semiconductor saturable absorber (SESAM) [1], [2], nonlinear polarization rotation (NPR) [3], [4], nonlinear amplifying loop mirror (NALM) [5], carbon nanotubes (CNT) [6], [7], graphene [8] and topological insulator [9] have been used to achieve multiwavelength passively mode-locked pulses in fiber lasers. However, all the multiwavelength pulses mentioned above are hyperbolic secant pulses.…”
Section: Introductionmentioning
confidence: 99%
“…The waist diameter and the length of the taper is ~4 μm and 8 mm, respectively. Compared with the reported taper length [17][18][19], the 8 mm taper waist in our laser cavity provides enough interacting length between the rGO and the transmission light, guaranteeing excellent saturable absorption and high nonlinearity. As shown in Fig.…”
Section: System Configuration and Signal Processingmentioning
confidence: 99%
“…In order to decrease the threshold of MI, we enhance the nonlinearity in a fiber laser cavity via long evanescent-field interaction length and strong mode confinement. To realize this, we use a long fiber taper deposited with reduced graphene oxide (reGO) [18][19][20][21][22]. The spontaneous XPMI is observed when pump power is set at 185 mW.…”
Section: Introductionmentioning
confidence: 99%