Observation of soliton bound states in a graphene mode locked erbium-doped fiber laser

We report on the experimental observation of bound states of solitons in a graphene mode locked erbium-doped fiber laser. By using graphene as a saturable absorber, we have obtained stable, single and bound soliton pulses, the latter with a full width at half maximum (FWHM) of 1.49 ps and a fixed pulse separation of 2.46 ps. Our results once again show that bound soliton pulses is an intrinsic feature of fiber lasers independent of the exact mode locking mechanism.

[1]  Y. G. Wang,et al.  Diode end-pumped passively mode-locked Nd:YLF laser at 1047 nm using single-wall carbon nanotubes based saturable absorber , 2011 .

[2]  Konstantin Golant,et al.  Bismuth fiber integrated laser mode-locked by carbon nanotubes , 2010 .

[3]  Yonggang Wang,et al.  Diode-pumped passively Q-switched Nd:Lu0.33Y0.37Gd0.3VO4 laser using a single-walled carbon nanotube saturable absorber , 2011 .

[4]  Bound solitons in the nonlinear Schrödinger-Ginzburg-Landau equation. , 1991 .

[5]  Zhi-Chao Luo,et al.  Graphene-based, 50 nm wide-band tunable passively Q-switched fiber laser , 2011 .

[6]  Zhipei Sun,et al.  A stable, wideband tunable, near transform-limited, graphene-mode-locked, ultrafast laser , 2010 .

[7]  Jing Kong,et al.  Transferring and Identification of Single- and Few-Layer Graphene on Arbitrary Substrates , 2008 .

[8]  D. Basko,et al.  Graphene mode-locked ultrafast laser. , 2009, ACS nano.

[9]  X. Wu,et al.  Bound states of solitons in a fiber laser mode locked with carbon nanotube saturable absorber , 2011 .

[10]  Malomed Bound solitons in coupled nonlinear Schrödinger equations. , 1992, Physical review. A, Atomic, molecular, and optical physics.

[11]  A. Voronin,et al.  Dynamics of high-power self-similar light pulses in a fiber laser with a carbon-nanotube saturable absorber , 2008 .

[12]  Swee Chuan Tjin,et al.  Compact graphene mode-locked wavelength-tunable erbium-doped fiber lasers: from all anomalous dispersion to all normal dispersion , 2010, 1003.5096.

[13]  P. Grelu,et al.  Phase-locked soliton pairs in a stretched-pulse fiber laser. , 2002, Optics letters.

[14]  Valery M. Mashinsky,et al.  Tunable and switchable dual-wavelength passively mode-locked Bi-doped all-fiber ring laser based on nonlinear polarization rotation , 2011 .

[15]  Boris A. Malomed,et al.  STABILITY OF BOUND STATES OF PULSES IN THE GINZBURG-LANDAU EQUATIONS , 1997 .

[16]  Wei Zhao,et al.  All-normal dispersion, figure-eight, tunable passively mode-locked fiber laser with an invisible and changeable intracavity bandpass filter , 2011 .

[17]  V. Konov,et al.  Femtosecond reflectometer with saturable absorber based on single-walled carbon nanotubes , 2009 .

[18]  J. Hernández-García,et al.  Generation of long broadband pulses with a figure-eight fiber laser , 2011 .

[19]  Yong-Won Song,et al.  Graphene mode-lockers for fiber lasers functioned with evanescent field interaction , 2010 .

[20]  S. Kobtsev,et al.  Mode-locked Yb-fiber laser with saturable absorber based on carbon nanotubes , 2011 .

[21]  Malomed Bound states of envelope solitons. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[22]  Elena D. Obraztsova,et al.  Using the E22 transition of carbon nanotubes for fiber laser mode-locking , 2011 .

[23]  Yong-Won Song,et al.  Deformation-immunized optical deposition of graphene for ultrafast pulsed lasers , 2011 .

[24]  H. Tam,et al.  Bound twin-pulse solitons in a fiber ring laser. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[25]  Zhenhua Ni,et al.  Atomic‐Layer Graphene as a Saturable Absorber for Ultrafast Pulsed Lasers , 2009, 0910.5820.

[26]  A. Reina,et al.  Large area, few-layer graphene films on arbitrary substrates by chemical vapor deposition. , 2009, Nano letters.