2011
DOI: 10.1134/s1054660x11150369
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Tunable high energy giant chirped passively mode-locked Yb-doped fiber laser

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Cited by 9 publications
(3 citation statements)
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“…Tunable ranges of 1024-1070 nm, 1015-1050 nm, and 1032-1052 nm were obtained by use of tunable intra-cavity filters, i.e., birefringent filter, tilting interference filter, and hibi-fiber sagnac loop filter, respectively. Tunable ANDi laser with giant chirped pulse output was also obtained by long period fiber grating filter and the tunable spectral range was 1028-1039 nm [8]. The wavelength tunable range and bandwidth of above lasers are different.…”
Section: Introductionmentioning
confidence: 98%
“…Tunable ranges of 1024-1070 nm, 1015-1050 nm, and 1032-1052 nm were obtained by use of tunable intra-cavity filters, i.e., birefringent filter, tilting interference filter, and hibi-fiber sagnac loop filter, respectively. Tunable ANDi laser with giant chirped pulse output was also obtained by long period fiber grating filter and the tunable spectral range was 1028-1039 nm [8]. The wavelength tunable range and bandwidth of above lasers are different.…”
Section: Introductionmentioning
confidence: 98%
“…Passive mode locking is the introduction of a nonlinear effect device with a saturated absorption response to the light intensity in the cavity to saturate the absorber, and the use of nonlinear Kerr effect or saturable absorption effect to achieve phase lock between each longitudinal mode. Common passive mode-locking technologies include nonlinear polarization rotation (NPR) mode-clamping [6], semiconductor saturable absorber mirror (SESAM) mode-clamping [7], nonlinear optical (magnification) loop mirror (NOLM/NALM) mode-clamping [8], and hybrid mode-clamping technology based on the above three mode-clamping mechanisms. In order to achieve the mode-locked output of wavelength tuning and switching, it is usually necessary to add tuning optical components [9][10][11][12] in the resonant cavity, such as wavelength selectors, tunable filters, polarization maintaining fibers, fiber gratings, etc., and can also introduce dispersive media in the cavity to increase the dispersion in the cavity and achieve wavelength tuning.…”
Section: Introductionmentioning
confidence: 99%
“…In 2007, A. Chong et al reported a mode-locked all-normal-dispersion giant chirped passively fiber laser system [11], in which the energy of the DSs is above 20nJ. Various ANDi systems such as switchable dual-wavelength laser system [12], tunable high energy giant chirped passively mode-locked fiber laser [13] have also been reported in recently years. In an ANDi system, multi pulses have been observed in the cavity when the pump power is increased to a certain level.…”
Section: Introductionmentioning
confidence: 99%