2013
DOI: 10.1007/s00340-013-5616-x
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Mode-locked L-band bismuth–erbium fiber laser using carbon nanotubes

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Cited by 24 publications
(14 citation statements)
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“…In addition, compared with traditional SAs, including semiconductor saturable absorber mirrors or carbon nanotubes, graphene does not require bandgap optimization and diameter or chiral adjustment, thus greatly simplifying the preparation process. With these advantages, graphene and its derivatives, such as graphene oxide, reduced graphene oxide, and graphene composite materials, have been widely developed in mode‐locked fiber lasers, as shown in Table . In terms of the performance of these mode‐locked lasers, some exciting results have been obtained, including minimum pulse‐width, maximum output power, and repetition rates of 29 fs, 520 mW, and 162 GHz, respectively.…”
Section: Versatile Pulsed Lasers Using 2d Layered Materialsmentioning
confidence: 99%
“…In addition, compared with traditional SAs, including semiconductor saturable absorber mirrors or carbon nanotubes, graphene does not require bandgap optimization and diameter or chiral adjustment, thus greatly simplifying the preparation process. With these advantages, graphene and its derivatives, such as graphene oxide, reduced graphene oxide, and graphene composite materials, have been widely developed in mode‐locked fiber lasers, as shown in Table . In terms of the performance of these mode‐locked lasers, some exciting results have been obtained, including minimum pulse‐width, maximum output power, and repetition rates of 29 fs, 520 mW, and 162 GHz, respectively.…”
Section: Versatile Pulsed Lasers Using 2d Layered Materialsmentioning
confidence: 99%
“…For this, Bi-Er co-doped optical fibres were used as an active gain [60]. In this work Ahmad et al suggested the application of the dualpumping configuration at 980 and 1480 nm to achieve amplified spontaneous emission spectrum with a bandwidth of more than 100 nm, from 1520 to 1625 nm.…”
Section: Bismuth (Bi)-doped Fibre Lasersmentioning
confidence: 99%
“…There are numerous reports in the literature [50][51][52][53][54][55][56][57][58][59][60][61][62][63][64][65][66][67] on the use of SWNTs as mode lockers and Q-switches for ultrafast lasers in the broad wavelength band, which are summarised in Table 1. One of the main advantages of SWNT-based SAs, apart from ultrashort relaxation time and high nonlinearity, is the ease of their fabrication and implementation into the laser setup.…”
Section: Introductionmentioning
confidence: 99%
“…Additionally, at 1560 nm, the saturation fluence of graphene is not much below the material damage threshold, which can lead to problems if the laser Q-switches at start up. Nevertheless, mode-locked fiber lasers have been demonstrated with CNTs [90,105,[126][127][128][129] as well as with graphene saturable absorbers [130][131][132]. A fully stabilized frequency comb system using CNTs deposited on a fiber tip has been reported [105], while only offset frequency stabilization has been demonstrated using a CNT embedded fiber taper [106].…”
Section: Carbon Nanotube and Graphene Saturable Absorber Lasersmentioning
confidence: 99%