2015
DOI: 10.1080/09500340.2015.1100339
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Generation of soliton and bound soliton pulses in mode-locked erbium-doped fiber laser using graphene film as saturable absorber

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Cited by 32 publications
(13 citation statements)
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“…It is anticipated that the soliton fiber lasers could serve as an ideal testbed for the study on bound solitons. So far, there have been plenty of reports on bound solitons 72,75,80,86,100,110,130,134,187,348,371,374, or claimed as soliton molecules 70,74,78,96,131,189,209,214,354, in mode locked fiber lasers. The bound states of solitons were first experimentally observed in a fiber laser mode locked with the nonlinear polarization rotation technique.…”
Section: A Multiple Soliton Interactionsmentioning
confidence: 99%
See 1 more Smart Citation
“…It is anticipated that the soliton fiber lasers could serve as an ideal testbed for the study on bound solitons. So far, there have been plenty of reports on bound solitons 72,75,80,86,100,110,130,134,187,348,371,374, or claimed as soliton molecules 70,74,78,96,131,189,209,214,354, in mode locked fiber lasers. The bound states of solitons were first experimentally observed in a fiber laser mode locked with the nonlinear polarization rotation technique.…”
Section: A Multiple Soliton Interactionsmentioning
confidence: 99%
“…The bound states of solitons were first experimentally observed in a fiber laser mode locked with the nonlinear polarization rotation technique. 374,385 Later, with the development of novel material based real saturable absorber (SA) mode locking techniques, such as the carbon nanotube mode locking and 2D-nano-materials mode locking, formation of bound states of solitons has also been observed in fiber lasers mode locked with the carbon nanotubes, 410,421,423,464,465 graphene, 70,72,74,75,78,80,86,96,100 MoS 2 , 130,131,134 black phosphorus, 109,110 and so on. As these saturable absorbers may be polarization independent, bound states of vector solitons were also reported in fiber lasers.…”
Section: A Multiple Soliton Interactionsmentioning
confidence: 99%
“…Compared with the actively Q-switched and mode-locked lasers, which frequently depend on an acousto-optic modulator (AOM) [10] or an electro-optic modulator (EOM) [11] for pulsed operation, the passive ones that use low-dimensional nanomaterials as saturable absorbers (SAs) possess the merits of cost effectiveness, low optical loss, simplicity, and ease of integration into a laser system [12][13][14][15]. As deeply studied SAs, low-dimensional nanomaterials such as graphene [16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31], topological insulators (TIs) [32][33][34][35][36][37][38][39][40], MXenes [41][42][43][44][45][46], transition-metal dichalcogenides (TMDs) [47][48][49][50][51][52][53][54][55]…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, graphene based materials such as graphene (G), 14 graphene oxide (GO), 15 reduced graphene oxide (rGO) 16 have been widely used for pulsed laser generation due to their unique nonlinear optical property. Graphene, with zero bandgap energy, readily absorbs all photons at all wavelengths, putting this graphene material forward as a broadband saturable absorber 17‐20 . On another note, graphene is also explored for wearable temperature sensor for personalized health care and human‐machine interface systems 21,22 .…”
Section: Introductionmentioning
confidence: 99%
“…Graphene, with zero bandgap energy, readily absorbs all photons at all wavelengths, putting this graphene material forward as a broadband saturable absorber. [17][18][19][20] On another note, graphene is also explored for wearable temperature sensor for personalized health care and human-machine interface systems. 21,22 Apart from all the properties mentioned above, graphene based materials are also known for its exceptional thermal conductivity, which allows it to be used as sensing element.…”
Section: Introductionmentioning
confidence: 99%