Shouqian Tang's research while affiliated with Shandong University of Technology and other places

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Publications (10)


Generation of Bright Pulses, Dark–Bright–Dark Pulses, and H-Shaped Pulse Rains in Fiber Lasers with CoTe 2 Nanosheets as Saturable Absorbers for Ultrafast Photonics
  • Article

March 2024

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25 Reads

ACS Applied Nano Materials

Qi Li

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Siyuan Xiong

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Qiuyan Sheng

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[...]

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Preparation processes of few-layer ZrTe2 nanosheets and ZrTe2 SA.
ZrTe2 powder. (a) SEM images; (b) XRD; (c) Raman spectrum; (d) EDS spectrum.
ZrTe2 nanosheets. (a) AFM images; (b) Corresponding to the thickness at the marked line in (a); (c) TEM images; (d) HR-TEM images.
(a) Nonlinear transmission properties of the ZeTe2 SA. Insert of Fig. 4(a). The experimental setup used for testing nonlinear transmission properties. (b) Linear transmission of the ZrTe2-PVA film versus wavelength.
Schematic diagram of experimental device for passively mode-locked EDFL.

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Generation of vector soliton mode-locked Er-doped fiber laser using ZrTe₂ as saturable absorber
  • Article
  • Full-text available

February 2024

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24 Reads

Optical Materials Express

Optical Materials Express

We demonstrate a passively mode-locked fiber laser employing zirconium telluride (ZrTe 2 ) as saturable absorber and illustrate its application for vector soliton generation in erbium-doped fiber lasers. By tuning the pump power and polarization controller, stable mode-locked operations in different operations are obtained with different cavity lengths. In addition, we also further research on characteristics of the vector solitons formed in fiber laser. The vector features of the obtained solitons are experimentally explored, and these solitons are proved to be group velocity locked vector solitons. Our research results indicate that ZrTe 2 nanosheets could be available saturable absorber for ultrashort pulse fiber lasers, especially for generating vector soliton pulses in fiber lasers.

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Figure 7. The relationship between the average output power and the pump power of the pulsed laser with different output ratios.
The output performance of the laser at different coupling ratios.
Comparison of high energy mode-locked lasers based on different SAs.
High-Energy Mode-Locked Pulse Er-Doped Fiber Laser-Based GeTe as Saturable Absorber

August 2023

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50 Reads

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1 Citation

High-energy Er-doped fiber laser with high conversion efficiency is reported, which is mode-locked by a germanium telluride (GeTe)-based saturable absorber (SA). By adjusting the direction of the polarization controller (PC), a high-energy pulse with a central wavelength of 1533.1 nm and a fundamental repetition frequency of 1.58 MHz is achieved. Under the pump power of 450.1 mW, the maximum average output power is 50.48 mW, and the single-pulse energy is 32 nJ. It is worth noting that the optical-to-optical conversion efficiency has reached about 11.2%. The experimental results indicate that GeTe performs excellently as SAs for obtaining mode-locked fiber lasers and plays an extremely important role in high-energy fiber lasers.


Evolution between bright and dark pulses in a Mo x W1-xTe2 based fiber laser

July 2023

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36 Reads

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4 Citations

We proposed an erbium-doped fiber laser mode-locked with a Mo x W1-xTe2-based nonlinear optical modulator for the first time to our best knowledge. This fiber laser can deliver bright pulses, bright-dark pulse pairs, dark pulses, bright-dark-bright pulses, and dark-dark-bright pulses. The modulation depth and saturation intensity of the Mo x W1-xTe2-based saturable absorber were about 7.8% and 8.6 MW/cm², respectively. When 10% of the laser in the cavity was output, conventional soliton pulses with central wavelength of 1560.1 nm can be obtained in the cavity. When 70% of the laser was output, dual-wavelength domain-wall dark pulses appeared in the laser cavity. This experiment revealed that an appropriate increase in the ratio of output energy can improve the chance of dark pulses in fiber lasers. The mode-locking states in this fiber laser can evolve with each other between bright pulses, bright-dark pulse pairs and dark pulses by adjusting the polarization controller. The results indicated that the Mo x W1-xTe2 can be used to make modulators for generating dark pulses. Furthermore, our work will be of great help to improve the chance of the generation of dark pulse in fiber lasers.



Generation of bright–dark solitons in an Er-doped fiber laser employing InSb as a saturable absorber

February 2023

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40 Reads

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2 Citations

In this paper, an indium antimonide (InSb) saturable absorber (SA) was successfully fabricated. The saturable absorption properties of the InSb SA were studied, and they show a modulation depth and a saturable intensity of 5.17% and ${9.23}\;{\rm{MW/c}}{{\rm{m}}^2}$ 9.23 M W / c m 2 , respectively. By employing the InSb SA and building the ring cavity laser structure, the bright–dark soliton operations were successfully obtained by increasing the pump power to 100.4 mW and adjusting the polarization controller. As the pump power increased from 100.4 to 180.3 mW, the average output power increased from 4.69 to 9.42 mW, the corresponding fundamental repetition rate was 2.85 MHz, and the signal-to-noise ratio was 68 dB. The experimental results show that InSb with excellent saturable absorption characteristics can be used as a SA to obtain pulse lasers. Therefore, InSb has important potential in fiber laser generation, further applications in optoelectronics, laser distance ranging, and optical fiber communication, and it can be widely developed.


Passively mode-locked fiber laser based on GeTe as a saturable absorber

November 2022

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29 Reads

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1 Citation

Applied Optics

Applied Optics

In this work, we fabricate a saturable absorber based on GeTe with saturation intensity and modulation depth of ${12.6}\;{{\rm MW/cm}^2}$ 12.6 M W / c m 2 and 7%, respectively. We obtain stable conventional soliton and stretched soliton mode-locking operation. For the conventional soliton state, the average output power increased from 0.93 to 8.70 mW with the increase of pump power, and the fundamental repetition rate was 7.8351 MHz. Its central wavelength and 3 dB bandwidth were 1564.72 and 4.78 nm, respectively. For the stretched soliton state, when the pump power was increased from 87.4 to 420.3 mW, the average output power increased from 2.05 to 10.46 mW. When the maximum average output power reached 10.46 mW, the maximum average single-pulse energy was 0.86 nJ. The experimental results show that GeTe nanosheets will have broad application potential in the field of ultrafast photonics.


Passively mode-locked Er-doped fiber laser based on a ferromagnetic insulator Cr2Si2Te6 as a saturable absorber

January 2022

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38 Reads

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13 Citations

Applied Optics

Applied Optics

In our work, a new-type, to the best of our knowledge, ferromagnetic insulator and its nonlinear optical absorption characteristics and related ultrafast modulation applications were investigated. ${{\rm Cr}_2}{{\rm Si}_2}{{\rm Te}_6}$ C r 2 S i 2 T e 6 saturable absorbers (SAs) with a modulation depth and a saturable intensity of 9.7% and ${3.5}\;{{\rm MW/cm}^2}$ 3.5 M W / c m 2 were fabricated. By adjusting the pump power to 120 mW and optimizing the polarization state, traditional soliton operations were obtained successfully; the corresponding duration of pulse and the fundamental repetition rate were ${\sim} {1.33}\;{\rm ps}$ ∼ 1.33 p s and 6.70 MHz, and the signal-to-noise ratio was 50 dB. The experimental results reveal that ${{\rm Cr}_2}{{\rm Si}_2}{{\rm Te}_6}$ C r 2 S i 2 T e 6 with excellent saturable absorption characteristics can be used as a SA to obtain ultrafast pulse lasers.

Citations (6)


... In addition, ZrTe 2 is high quality topological material among the layered 2D TMDs, and the material may perform particular nonlinear optical features and excellent properties in the field of ultrashort optics [37][38][39]. In September 2023, Sheng et al. report on the generation of dual large energy pulses in a passively mode-locked Er-doped fiber laser based on ZrTe 2 as SA [40]. They obtained mode-locked soliton pulses with maximum pulse energy of 42.6 nJ and 45.7 nJ, respectively. ...

Reference:

Generation of vector soliton mode-locked Er-doped fiber laser using ZrTe₂ as saturable absorber
Generation of dual large energy pulses in Er3+-doped fiber lasers based on ZrTe2 saturable absorber via polarization manipulation
  • Citing Article
  • February 2024

Optics & Laser Technology

... To the best of our knowledge, our method has enabled, for the first time, the stationary generation of nanosecond pulses with an energy of up to 180 nJ to be obtained at a wavelength of about 1.53 µm in Er all-fiber lasers without the employment of any active intracavity modulators or saturable absorbers (neither artificial nor material [25,26]). The use of these devices for high-energy pulse Photonics 2024, 11, 37 8 of 10 generation via Q-switching [27] or mode-locking [28] not only complicates the design of fiber lasers, but also reduces their reliability and may impose additional limits on the laser performance. The known approaches to pulse generation through intracavity instabilities in Er fiber lasers [5,7] do not result in the same high pulse energy and pulse train stability as our method. ...

High-Energy Mode-Locked Pulse Er-Doped Fiber Laser-Based GeTe as Saturable Absorber
Nanomaterials

Nanomaterials

... The absence of Kelly sidebands in Fig. 5(b) may be attributed to the spectrum filtration effect caused by polarization of the PC and intracavity birefringence of the SMF. Notably, the spectrum exhibits an M-shape with two wavelength components centered at 1568.26 nm and 1569.20 nm, which is similar to earlier reports, [47][48][49][50] sug-gesting that it may also be influenced by cavity feedback and competition for gain. When the pump power is maintained at a fixed value of 63 mW, a stable bright-dark soliton pair is generated by adjusting the PC. Figure 6 displays the pulse train of a bright-dark soliton pair, with a distance of 34 ns between the solitons, which corresponds to the cavity's return time. ...

Evolution between bright and dark pulses in a Mo x W1-xTe2 based fiber laser
Optics Express

Optics Express

... The single-pulse energy shows a gradually increasing trend, with a slight decrease in peak power. The increase in pulse width with pump power causes this change [42,43]. ...

Generation of dissipative soliton resonance and soliton rain in passively mode-locked fiber laser based on GeTe saturable absorber
  • Citing Article
  • March 2023

Infrared Physics & Technology

... It can be seen that Ge and Te existed in the measured sample. Therefore, it confirms the high purity of the GeTe nanosheets [44,45]. In the Raman spectrum, as provided in Figure 2c, there are three obvious peaks located at 91.71, 122.83, and 141.21 cm −1 , respectively. ...

Passively mode-locked fiber laser based on GeTe as a saturable absorber
Applied Optics

Applied Optics

... In the future, we will solve the problem of instruments and further explore more details of the bound state soliton output from ZrGeTe 4 -SA based ring lasers. Table 1 summarizes the results of mode-locked fiber lasers based on SAs of different 2D materials [68][69][70][71][72][73][74]. This indicates that our designed ZrGeTe 4 -SA based TSFL is effective. ...

Passively mode-locked Er-doped fiber laser based on a ferromagnetic insulator Cr2Si2Te6 as a saturable absorber
Applied Optics

Applied Optics