10) are 0.766L179.1" and 0.743L -171.9", respectively, while the measured reflection coefficient is 0.763L -172.6' . The inversion process with water as medium 1 and a conductor as medium 2 indicates even slower convergence with respect to that of methanol. In this case, the permittivity of water w
Analyzing longitudinal-mode of single-frequency ring fiber laser
✍ Scribed by T. S. Wang; Y. B. Guo; K. Wang
- Publisher
- John Wiley and Sons
- Year
- 2007
- Tongue
- English
- Weight
- 313 KB
- Volume
- 49
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
To realize single‐frequency of the fiber laser, a ring configuration is devised. The single‐frequency operation is realized at 1549.63 nm by using a fiber Bragg grating (FBG) as wavelength‐selective element and a unpumped 1.5 m‐long erbium‐doped fiber, which can produce standing‐wave saturation effects in the cavity. A measurement method based on fiber‐coupling scanning Fabry–Perot (F‐P) interferometer at 1.55 μm is designed. The laser longitudinal‐mode spacing is 11.1 MHz. The single‐frequency is observed by the interferometer with free spectrum range (FSR) of 7.5 GHz. The longitudinal‐mode fabric is analyzed by the interferometer with FSR of 1.5 GHz. As the cavity length increases, the longitudinal‐mode spacing changes to 3.7 MHz. The structures of longitudinal‐modes under different cavity lengths are compared. The longitudinal‐mode linewidth of 20 MHz is measured. Experimental results show that single‐frequency of the fiber laser can be approved accurately, and the effectiveness of the method, which can analyze longitudinal‐mode of the fiber laser with scanning Fabry–Perot (F‐P) interferometer, is improved. © 2007 Wiley Periodicals, Inc. Microwave Opt Technol Lett 49: 1494–1497, 2007; Published online in Wiley InterScience (www.interscience.wiley.com). DOI.10.1002/mop.22467
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