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Yao BC, Rao YJ, Wang ZN, Wu Y, Zhou JH, Wu H, Fan MQ, Cao XL, Zhang WL, Chen YF, Li YR, Churkin D, Turitsyn S, Wong CW. Graphene based widely-tunable and singly-polarized pulse generation with random fiber lasers. Sci Rep 2015; 5:18526. [PMID: 26687730 PMCID: PMC4685245 DOI: 10.1038/srep18526] [Citation(s) in RCA: 35] [Impact Index Per Article: 3.9] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/02/2015] [Accepted: 11/17/2015] [Indexed: 11/09/2022] Open
Abstract
Pulse generation often requires a stabilized cavity and its corresponding mode structure for initial phase-locking. Contrastingly, modeless cavity-free random lasers provide new possibilities for high quantum efficiency lasing that could potentially be widely tunable spectrally and temporally. Pulse generation in random lasers, however, has remained elusive since the discovery of modeless gain lasing. Here we report coherent pulse generation with modeless random lasers based on the unique polarization selectivity and broadband saturable absorption of monolayer graphene. Simultaneous temporal compression of cavity-free pulses are observed with such a polarization modulation, along with a broadly-tunable pulsewidth across two orders of magnitude down to 900 ps, a broadly-tunable repetition rate across three orders of magnitude up to 3 MHz, and a singly-polarized pulse train at 41 dB extinction ratio, about an order of magnitude larger than conventional pulsed fiber lasers. Moreover, our graphene-based pulse formation also demonstrates robust pulse-to-pulse stability and wide-wavelength operation due to the cavity-less feature. Such a graphene-based architecture not only provides a tunable pulsed random laser for fiber-optic sensing, speckle-free imaging, and laser-material processing, but also a new way for the non-random CW fiber lasers to generate widely tunable and singly-polarized pulses.
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Affiliation(s)
- B C Yao
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China.,Mesoscopic Optics and Quantum Electronics Laboratory, University of California, Los Angeles, CA 90095, United States
| | - Y J Rao
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - Z N Wang
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - Y Wu
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - J H Zhou
- State Key Laboratory of Electronic Thin Films and Integrated Devices, University of Electronic Science and Technology of China, Chengdu 610054, China
| | - H Wu
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - M Q Fan
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - X L Cao
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - W L Zhang
- Key Laboratory of Optical Fiber Sensing and Communications (Education Ministry of China), University of Electronic Science and Technology of China, Chengdu 610054, China
| | - Y F Chen
- State Key Laboratory of Electronic Thin Films and Integrated Devices, University of Electronic Science and Technology of China, Chengdu 610054, China
| | - Y R Li
- State Key Laboratory of Electronic Thin Films and Integrated Devices, University of Electronic Science and Technology of China, Chengdu 610054, China
| | - D Churkin
- Aston Institute of Photonic Technologies, Aston University, Birmingham, B47ET, United Kingdom.,Laboratory of Nonlinear Photonics, Novosibirsk State University, Novosibirsk, 630090 Russia.,Institute of Automation and Electrometry, Siberian Branch of the Russian Academy of Sciences, Novosibirsk, 630090, Russia
| | - S Turitsyn
- Aston Institute of Photonic Technologies, Aston University, Birmingham, B47ET, United Kingdom.,Laboratory of Nonlinear Photonics, Novosibirsk State University, Novosibirsk, 630090 Russia
| | - C W Wong
- Mesoscopic Optics and Quantum Electronics Laboratory, University of California, Los Angeles, CA 90095, United States
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Turitsyn SK, Ania-Castañón JD, Babin SA, Karalekas V, Harper P, Churkin D, Kablukov SI, El-Taher AE, Podivilov EV, Mezentsev VK. 270-km ultralong Raman fiber laser. Phys Rev Lett 2009; 103:133901. [PMID: 19905514 DOI: 10.1103/physrevlett.103.133901] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/01/2009] [Indexed: 05/28/2023]
Abstract
We analyze the physical mechanisms limiting optical fiber resonator length and report on the longest ever laser cavity, reaching 270 km, which shows a clearly resolvable mode structure with a width of approximately 120 Hz and peak separation of approximately 380 Hz in the radio-frequency spectrum.
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Affiliation(s)
- S K Turitsyn
- Photonics Research Group, Aston University, Birmingham, B4 7ET, United Kingdom
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Babin S, Churkin D, Kablukov S, Podivilov E. Raman gain saturation at high pump and Stokes powers. Opt Express 2005; 13:6079-6084. [PMID: 19498616 DOI: 10.1364/opex.13.006079] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/27/2023]
Abstract
Raman gain spectral profile has been measured in a phosphosilicate fiber at high pump and Stokes (signal) wave powers. It has been shown that the profile saturates homogeneously. The main saturation mechanism is proved to be the pump depletion, i.e., Raman gain coefficient gR does not depend on the pump and signal wave power up to the level of ~ 3 W.
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