2015
DOI: 10.1364/oe.23.004369
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Tunable and switchable dual-wavelength Tm-doped mode-locked fiber laser by nonlinear polarization evolution

Abstract: We propose and demonstrate a tunable and switchable dual-wavelength ultra-fast Tm-doped fiber laser. The tunability is based on nonlinear polarization evolution (NPE) technique in a passively mode-locked laser cavity. The NPE effect induces wavelength-dependent loss in the cavity to effectively alleviate mode competition and enables the multiwavelength mode locking. The laser exhibits tunable dual-wavelength mode locking over a wide range from 1852 to 1886 nm. The system has compact structure and both the wave… Show more

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Cited by 151 publications
(56 citation statements)
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“…Recently, Z. Yan et al . have presented a switchable and tuneable single-longitudinal-mode multi-wavelength Tm-doped fibre laser, based on NPE2223, resulting in limited progress in the field.…”
mentioning
confidence: 99%
“…Recently, Z. Yan et al . have presented a switchable and tuneable single-longitudinal-mode multi-wavelength Tm-doped fibre laser, based on NPE2223, resulting in limited progress in the field.…”
mentioning
confidence: 99%
“…Compared to conventional mode-locked lasers, a tunable-mode-locked laser with flexibly adjustable mode-locked laser parameters, such as output wavelength, pulse repetition frequency, and pulse width, obviously has a wider application potential [4][5][6][7][8]. Graphene and other two-dimensional (2D) noncarbon materials, including topological insulators (TIs), transition metal dichalcogenides (TMDCs), phosphorene, bismuthene, and antimonene, have witnessed a very fast development of both fundamental and practical aspects in mode-locked fiber lasers [9].Several approaches have been proposed to achieve tunable wavelength mode-locked operation, based on a nonlinear optical loop mirror (NOLM) [10] or on polarization-maintaining fiber (PMF) [11]. However, these techniques require a few kilometers of fiber to achieve the desired non-linear effect, which increase the length of the fiber required for the constitution of the laser, resulting in a significant reduction in the stability of the laser output.…”
Section: Introductionmentioning
confidence: 99%
“…Different from active mode-locking techniques, passive mode-locking is simple, compact and low-cost without using active modulator in the laser cavity. Generally, passively mode-locked thulium-doped fiber lasers (TDFLs) can be implemented by nonlinear polarization rotation (NPR) [3], nonlinear amplifying loop mirror (NALM) [4], nonlinear optical loop mirror (NOLM) [5], semiconductor saturable absorber mirror (SESAM) [6], graphene [7], topological insulator [8], and the combination of saturable absorber (SA) with nonlinear switching based techniques [9]. As carbon allotropes draw much attention recently, single-wall carbon nanotube (SWNT) has been demonstrated to possess ultrafast nonlinear optical responses [10].…”
Section: Introductionmentioning
confidence: 99%
“…However, such additional optical filter extends the cavity length and increases the implementation cost. NALM and NPR techniques, on the other hand, are good alternatives to obtain both mode-locking and filtering effect within the laser cavity to realize multi-wavelength mode-locking [3], [16]. Nevertheless, NALM-based and NPR-based mode-locking generally need high pump power and careful adjustment, in order to realize stable mode-locking operation.…”
Section: Introductionmentioning
confidence: 99%