IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 28, NO. 11, JUNE 1, 2016 1193
Dual-Wavelength 2-μm Fiber Laser With Coupled
Fiber Bragg Grating Cavities
Yao Wang, Yan Zhou, Shuo Yan, Yulong Tang, and Jianqiu Xu
Abstract—We develop dual-wavelength 2-µm fiber lasers with
coupled cavity configurations based on fiber Bragg gratings and
study their output performance and emission dynamics. Efficient
cavity-coupling management leads to different dual-wavelength
operation regimes. Over 3 W of output power is realized at
both 1942 and 2020 nm, and a power ratio of the 1942 nm
to the 2020 nm laser emissions can be tuned from 24.9%
to 237.6%. This first achieved 2-µm fiber laser system with
binary-wavelength emission and flexible power ratios can find
applications in various areas.
Index Terms—Fiber lasers, thulium, dual-wavelength, fiber
gratings.
I. INTRODUCTION
T
M-DOPED fiber lasers (TDFLs) have been advanced
rapidly in recent years due to their ability to generate effi-
cient, high power, and diffraction-limited laser emission in the
1900-2100 nm wavelength range and have found significant
applications in various areas, including atmospheric lidar mea-
surement, remote sensing, medical surgery, industry machin-
ing, etc. [1]–[3]. A large variety of TDFLs have been reported,
such as high power continuous wave (CW) mode [4]–[7],
pulsed mode [8]–[10], wavelength tunable [11]–[13], just to
name a few.
For some applications, such as division multiplexing
communication, optical signal processing, optical sensing,
and precision spectroscopy, multi-wavelength fiber
lasers (MWFLs) are required and shaping up as an important
area of research. There are a number of methods to realize
MWFL operation [14]–[21]. So far, a few papers have reported
MWFLs in the 2-μm regime [16]–[21]. For CW operation, the
2-μm MWFLs are generally constructed by using four-wave
mixing [16], [17], nonlinear loop mirror [18], [19], and
high-birefringence fiber Bragg gratings (FBGs) [20]. For
pulsed operation, the 2-μm MWFLs are primarily based on
nonlinear polarization evolution [21]. All these 2-μmMWFLs
Manuscript received October 8, 2015; revised December 9, 2015; accepted
February 25, 2016. Date of publication February 29, 2016; date of current
version April 5, 2016. This work was supported in part by the Research
Fund for the Doctoral Program of Higher Education of China under
Grant 20120073120085 and in part by the National Natural Science Founda-
tion of China under Grant 11121504, Grant 61138006, and Grant 61275136.
The authors are with the Key Laboratory for Laser Plasmas, Department
of Physics and Astronomy, Ministry of Education, Shanghai Jiao Tong Uni-
versity, Shanghai 200240, China, and also with the Collaborative Innovation
Center of Inertial Fusion Science and Application (CIC IFSA), Shanghai
Jiao Tong University, Shanghai 200240, China (e-mail: ywang001@yeah.net;
luguozhe@sjtu.edu.cn; yanssjtu@163.com; yulong@sjtu.edu.cn; jqxu09@
sjtu.edu.cn).
Color versions of one or more of the figures in this letter are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LPT.2016.2536101
Fig. 1. Experimental setup of the coupled-cavity TDFL. LD: laser diode;
HR: highly reflective fiber Bragg grating; PR: partially reflective fiber Bragg
grating; TDF: Tm-doped fiber.
mentioned above, either CW or pulsed, feature low output
power and small wavelength spacing. However in some
particular applications, multi-wavelength laser beams with
moderate power and large wavelength spacing are required.
In this letter, dual-wavelength 2-μm fiber lasers with cou-
pled FBG cavities are reported. By changing both the laser
cavity parameters (cavity coupling, etc.) and the pumping
level, we obtain binary-wavelength output modes and different
output power ratios of the 1942 nm to the 2020 nm laser
emissions. Over 3 W of output power is realized at both
1942 nm and 2020 nm, and power ratio of the 1942 nm to the
2020 nm laser emissions can be tuned from 24.9% to 237.6%.
II. E
XPERIMENT AND RESULTS
In order to achieve dual-wavelength operation from a single
fiber laser system, we have designed a coupled-cavity con-
figuration, as shown in Fig. 1. The 1942 nm laser cavity
includes the 2020 nm laser cavity. At the same time, these
two cavities are coupled due to pump depletion and laser light
reabsorption (the 1942 nm signal light can be reabsorbed in the
2020 nm laser cavity [7]). The active fiber used is a double-
clad TDF (Nufern, PLMA-TDF-25P/400-HE) with a 25 μm
diameter, 0.09 numerical aperture (NA) core doped with Tm
3+
of ∼4 wt. % concentration. The pure-silica inner cladding,
coated with a low-index polymer, has a 400 μm diameter and
a NA of 0.46. The absorption of this fiber at 793 nm with
cladding-pump (at 1942 nm with core-pump) was measured
to be ∼3dB/m(∼1.2 dB/m) with the cut-back method.
A ∼2.1 m TDF and a ∼2.6 m TDF are used here. The
pump source is a 793 nm high power laser diode (LD). The
LD has a maximum output power of 75 W and a 220 μm
(0.22 NA) pigtail fiber, which matches to the pump fiber of a
(6+ 1)×1 high power fiber combiner (ITF, MMC0611C4090).
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