| FUNDAMENTAL AREAS OF PHENOMENOLOGY(INCLUDING APPLICATIONS) |
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Femtosecond Fiber Laser Based on BiSbTeSe$_{2}$ Quaternary Material Saturable Absorber |
| Yue-Jia Xiao1, Xiao-Wei Xing1, Wen-Wen Cui1, Yue-Qian Chen1, Qin Zhou2, and Wen-Jun Liu1* |
1State Key Laboratory of Information Photonics and Optical Communications, School of Science, Beijing University of Posts and Telecommunications, Beijing 100876, China
2School of Mathematical and Physical Sciences, Wuhan Textile University, Wuhan 430200, China
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| Cite this article: |
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Yue-Jia Xiao, Xiao-Wei Xing, Wen-Wen Cui et al 2023 Chin. Phys. Lett. 40 054201 |
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Abstract Topological insulator materials, including Bi$_{2}$Te$_{3}$, Sb$_{2}$Te$_{3}$, Sb$_{2}$Te$_{3}$, and Bi$_{2}$Se$_{3}$, have attracted some attention due to their narrow band gaps, high carrier mobility, wide spectral absorption ranges and other characteristics. We report a new multi-compound topological insulator material BiSbTeSe$_{2}$ that, compared with the traditional topological insulator composed of two elements, can integrate the physical advantages of each element, helpful to build an experimental platform with rich physical properties. The nonlinear optical characteristics of the quaternary material BiSbTeSe$_{2}$ is obtained in the erbium-doped fiber laser. Using the BiSbTeSe$_{2}$ as a saturable absorber material, the passive Q-switched and mode-locked fiber lasers are achieved. The pulse duration and signal-to-noise ratio (SNR) of the Q-switched fiber laser are 854 ns and 70 dB, respectively. Meanwhile, the pulse duration and SNR of the mode-locked fiber laser are 259 fs and 87.75 dB, respectively. This work proves that the BiSbTeSe$_{2}$ has a considerable application prospect as a saturable absorber in fiber lasers, and provides a new reference for selection of high-performance saturable absorber materials.
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Received: 13 February 2023
Published: 18 April 2023
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| PACS: |
42.55.Wd
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(Fiber lasers)
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42.65.Sf
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(Dynamics of nonlinear optical systems; optical instabilities, optical chaos and complexity, and optical spatio-temporal dynamics)
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42.70.Hj
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(Laser materials)
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42.70.-a
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(Optical materials)
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