Saturable and reverse saturable absorption in
molybdenum disulfide dispersion and film by
defect engineering
CHUNHUI LU,
1
HONGWEN XUAN,
1,
*YIXUAN ZHOU,
1
XINLONG XU,
1
QIYI ZHAO,
2
AND JINTAO BAI
1
1
Shaanxi Joint Laboratory of Graphene, State Key Laboratory of Photoelectric Technology and Functional Materials, International Collaborative
Center on Photoelectric Technology and Nano Functional Materials, Institute of Photonics & Photon-Technology, School of Physics,
Northwest University, Xi’an 710069, China
2
School of Science, Xi’an University of Posts and Telecommunications, Xi’an 710121, China
*Corresponding author: hwxuan@nwu.edu.cn
Received 22 April 2020; revised 14 June 2020; accepted 23 June 2020; posted 24 June 2020 (Doc. ID 395870); published 27 August 2020
Understanding and controlling defect in two-dimensional materials is important for both linear and nonlinear
optoelectronic devices, especially in terms of tuning nonlinear optical absorption. Taking advantage of an atomic
defect formed easily by smaller size, molybdenum disulfide nanosheet is prepared successfully with a different size
by gradient centrifugation. Interestingly, size-dependent sulfur vacancies are observed by high-resolution
X-ray photoelectron spectroscopy, atomic force microscopy, and transmission electron microscopy. The defect
effect on nonlinear absorption is investigated by Z-scan measurement at the wavelength of 800 nm. The results
suggest the transition from saturable absorption to reverse saturable absorption can be observed in both disper-
sions and films. First principle calculations suggest that sulfur vacancies act as the trap state to capture the
excited electrons. Moreover, an energy-level model with the trap state is put forward to explain the role of
the sulfur vacancy defect in nonlinear optical absorption. The results suggest that saturable absorption and reverse
saturable absorption originate from the competition between the excited, defect state and ground state absorp-
tion. Our finding provides a way to tune the nonlinear optical performance of optoelectronic devices by defect
engineering.
© 2020 Chinese Laser Press
https://doi.org/10.1364/PRJ.395870
1. INTRODUCTION
Unavoidable defects in the growth process of two-dimensional
(2D) materials can dramatically affect the performance of the
corresponding device. Defect-associated nonradiative recombi-
nation will lead to low quantum efficiency (<0.6%)[1], and
structure defects will result in lower carrier mobility [2].
Defects can also be a source of merit; for instance, photolumi-
nescence enhancement induced by sulfur (S) vacancy [3] and
oxygen bonding at the defect sites [4] in monolayer molybde-
num disulfide (MoS
2
) and catalytic efficiency in hydrogen evo-
lution reaction improved by S vacancies [5] at edge defects [6].
However, the contribution of these defects to the nonlinear op-
tical (NLO) properties, such as saturable absorption (SA) and
reverse saturable absorption (RSA), is not completely clear so
far. Recently, different defect types, including effective two-
photon absorption (TPA) from zinc (Zn) vacancy [7], tunable
NLO absorption derived from the concentration of manganese
doping [8], and enhanced modulation depth [9] from localized
defect states at grain boundaries, have been introduced to im-
prove the performance of nonlinear photonic devices. Actually,
these defects act as different trap centers to capture electrons
[10], holes [11], or excitons [12,13], which make it crucial
to confirm the type of defect-induced localized states in 2D
materials.
MoS
2
is a typical 2D material to design linear optoelectronic
devices due to its excellent optical and electronic properties,
including high current on/off ratio (∼10
8
), high electron
mobility (10
2
cm
2
· V
−1
· s
−1
)[14], strong catalytic activity [15],
and photoluminescence [16,17]. Importantly, a size-dependent
few-layer MoS
2
can be achieved easily using ultrasonic exfolia-
tion [18] combined with the gradient centrifugation method
[19]. On the other hand, nonlinear photonic applications in-
cluding Q-switching [20], mode-locking [21,22], and an op-
tical limiter [23] have also been designed based on SA and
RSA behavior. For example, MoS
2
and graphene were reported
with stronger SA [24] than those of MoTe
2
and MoSe
2
, while
BN exhibited a strong RSA effect [25]. SA and RSA can be
interpreted as a transmission increasing and decreasing accord-
ing to pump intensity, respectively. It is determined by a smaller
absorption cross section in excited state compared with that in
1512
Vol. 8, No. 9 / September 2020 / Photonics Research
Research Article
2327-9125/20/091512-10 Journal © 2020 Chinese Laser Press