4.7 Article

Layered iron pyrite for ultrafast photonics application

期刊

NANOPHOTONICS
卷 9, 期 8, 页码 2515-2522

出版社

WALTER DE GRUYTER GMBH
DOI: 10.1515/nanoph-2020-0014

关键词

iron pyrite; ultrafast photonics; transition metal dichalcogenide; 2D materials

资金

  1. National Natural Science Foundation of China [61605106]
  2. projects for the Academic Leader and Academic Backbones, Shaanxi Normal University [18QNGG006]
  3. Shaanxi Normal University [1112010209, 1110010717]
  4. Fundamental Research Funds for the Central Universities [GK201802006, 2018CSLY005]
  5. Open Research Fund of State Key Laboratory of Transient Optics and Photonics, Chinese Academy of Sciences [SKLST201809, SKLST201401]
  6. Open Fund of State Key Laboratory of Information Photonics and Optical Communications (Beijing University of Posts and Telecommunications), P.R. China [IPOC2017B012]
  7. Open Research Fund of State Key Laboratory of Pulsed Power Laser Technology, Electronic Engineering Institute [SKL2017KF02]

向作者/读者索取更多资源

Two-dimensional (2D) transition metal dichalcogenide materials have attracted much attention in recent years due to their excellent electro-optical properties. FeS2, the ideal composition of iron pyrite, is a 2D transition metal dichalcogenide which has been potentially used in the electronic, optical, and chemical fields. On the other hand, the narrow band gap of FeS2 (approximate to 0.96 eV) makes it very suitable and promising for the ultrafast application in near-infrared regimes. However, the potential application of FeS2 in laser technology has not been explored till now. Ultrashort pulse lasers have great applications in industry and science because of its stability, ease of operation, and portability. Passively mode-locked fiber lasers using 2D materials (such as MoS2, CuS2, and WS) as saturable absorber are intensively investigated. Here, layered FeS2 has been characterized systematically. It is successfully applied in ultrafast photonics and plays a key component in the passively mode-locked laser for the first time. The single pulse can be obtained with 1.7-ps pulse duration, 1.89-nm spectral width, and fundamental repetition of 6.4 MHz at 1563 nm central wavelength. Through controlling the pump power, the evolution of the pulse train can be observed, which can be transformed from single pulse to bound states. Also, the harmonic mode-locked fiber laser is observed with the pump power high enough.

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