High Power Laser Science and Engineering, (2018), Vol. 6, e16, 5 pages.
© The Author(s) 2018. This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/
licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
doi:10.1017/hpl.2018.9
kW-class high power fiber laser enabled by active long
tapered fiber
Chen Shi
1,2
, Hanwei Zhang
1,2
, Xiaolin Wang
1,2
, Pu Zhou
1,2
, and Xiaojun Xu
1,2
1
College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
2
Hunan Provincial Collaborative Innovation Center of High Power Fiber Laser, Changsha 410073, China
(Received 29 November 2017; revised 17 January 2018; accepted 27 February 2018)
Abstract
Compared with traditional uniform fibers, tapered fiber has numerous unique advantages, such as larger mode area,
higher pump absorption, suppression to nonlinear effects, and maintaining good beam quality. In this manuscript, we
have constructed an all-fiberized fiber amplifier which is based on a piece of ytterbium-doped tapered double-clad fiber
(T-DCF). The fiber amplifier is operated under continuous wave (CW) regime at 1080 nm wavelength. The M
2
factor of
the amplifier at 1.39 kW output power is ∼1.8. The maximum output power of the system reached 1.47 kW, which, to the
best of our knowledge, is the highest output power of long tapered fiber based fiber laser system. Our result successfully
verifies the potential of power scalability and all-fiberized capability of long tapered fiber, and the performance of our
system can be further enhanced by fiber design optimization.
Keywords: fiber lasers and applications; laser amplifiers
1. Introduction
For the advantage of high slope efficiency, good beam qual-
ity, superior thermal management property and compactness,
fiber lasers are widely used in the field of laser marking,
material processing, medicine, communication and many
other industrial applications
[1]
. In the past decade, output
power of fiber lasers experienced a rapid boost with the
development of large mode area (LMA) double-clad fibers
(DCF) and cladding pump technology
[2, 3]
. Among them,
ytterbium-doped fiber lasers and amplifiers at 1 µm have
shown excellent optical efficiency
[4, 5]
and have reached over
100 kW output power by combining tens of kW-level single
mode fiber lasers.
Compared with traditional fiber laser oscillator, the main
oscillator power amplifier (MOPA) system, which can
boost the progress of fiber laser power scaling, offers an
effective way to acquire high power fiber laser source with
excellent beam quality by employing cascaded structure.
However, further power scaling of MOPA system requires a
considerable effort to suppress nonlinearities, which usually
has contradiction in fiber type selection with the requirement
of good beam quality. Compared to uniform LMA active
fiber, T-DCF shows numerous unique advantages when
Correspondence to: X. Wang, College of Advanced Interdisciplinary
Studies, National University of Defense Technology, Changsha 410073,
China. Email: chinawxllin@163.com
being employed as gain medium of optical amplifier, such
as larger mode area, higher pump absorption, suppression
to nonlinear effects, maintaining good beam quality and
so on
[6–8]
. A number of applications using T-DCF have
already been reported. T-DCF has been applied in CW
fiber laser oscillator
[9]
, Q-switched pulsed oscillator
[10]
, CW
fiber laser amplifier
[11, 12]
and ultrafast laser systems
[13]
.
However, all of the systems in Refs. [9–13] were constructed
based on the bulk optical component, which lack stability
and compactness. Comparatively speaking, the all-fiberized
structure has better performance in stability, compactness,
thermal management and so on. Few researchers have
reported their experimental results based on all-fiberized
T-DCF structures. Zhou et al. has constructed an all-
fiberized fiber amplifier using active T-DCF
[14]
, and 53 W
single frequency output at 1064 nm wavelength with
M
2
∼ 1.28 beam quality was obtained. Zhang et al. and
Lou et al. have individually reported their passive T-DCF
based random fiber laser system
[15, 16]
. Up to present, the
maximum output power of fiber laser based on long tapered
fiber is 750 W with a beam quality of M
2
∼ 1.7
[9]
. A kW-
level, all-fiberized fiber laser using tapered fiber has not yet
been reported.
In this manuscript, we have constructed an all-fiberized
fiber amplifier, which is based on a piece of ytterbium-
doped T-DCF. The fiber amplifier was operated at 1080 nm
wavelength under CW regime. The maximum output power
1