Polarization-dependent efficient Cherenkov radiation at visible wavelengths in hollow-core photonic crystal fiber cladding
Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber (HC-PCF). When the angle of the half-wave plate is rotated from 0° to 45°, the Raman soliton shifts from 2227 to 2300 nm, the output power of the CR...
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Published in | Chinese physics B Vol. 22; no. 1; pp. 222 - 225 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
2013
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Online Access | Get full text |
ISSN | 1674-1056 2058-3834 1741-4199 |
DOI | 10.1088/1674-1056/22/1/014102 |
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Abstract | Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber (HC-PCF). When the angle of the half-wave plate is rotated from 0° to 45°, the Raman soliton shifts from 2227 to 2300 nm, the output power of the CR increases 8.15 times, and the maximum output power ratio of the CR at 556 nm to the residual pump is estimated to be 20:1. The width of the output optical spectrum at visible wavelengths broadens from 25 to 45 nm, and the conversion efficiency of the CR can be above 28%. Moreover, the influences of the pump polarization and wavelength on the CR are studied, and the corresponding nonlinear processes are discussed. |
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AbstractList | Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber (HC-PCF). When the angle of the half-wave plate is rotated from 0° to 45°, the Raman soliton shifts from 2227 to 2300 nm, the output power of the CR increases 8.15 times, and the maximum output power ratio of the CR at 556 nm to the residual pump is estimated to be 20:1. The width of the output optical spectrum at visible wavelengths broadens from 25 to 45 nm, and the conversion efficiency of the CR can be above 28%. Moreover, the influences of the pump polarization and wavelength on the CR are studied, and the corresponding nonlinear processes are discussed. Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber (HC-PCF). When the angle of the half-wave plate is rotated from 0[degrees] to 45[degrees], the Raman soliton shifts from 2227 to 2300 nm, the output power of the CR increases 8.15 times, and the maximum output power ratio of the CR at 556 nm to the residual pump is estimated to be 20:1. The width of the output optical spectrum at visible wavelengths broadens from 25 to 45 nm, and the conversion efficiency of the CR can be above 28%. Moreover, the influences of the pump polarization and wavelength on the CR are studied, and the corresponding nonlinear processes are discussed. |
Author | 申向伟 苑金辉 桑新柱 余重秀 饶岚 夏民 韩颖 夏长明 侯蓝田 吴中超 何晓亮 |
AuthorAffiliation | The 26th Institute of China Electronics Technology Corporation, Chongqing 400060, China State Key Laboratory of Information Photonics and Optical Communications, Beijing University of Posts & Telecommunications, Beijing 100876, China Institute of Infrared Optical Fibers & Sensors, Qinhuangdao 066004, China |
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Cites_doi | 10.1109/LPT.2012.2186436 10.1103/PhysRevA.51.2602 10.1364/OE.19.004985 10.1364/OE.16.004858 10.1007/s00340-004-1650-z 10.7498/aps.61.044203 10.1126/science.285.5433.1537 10.1088/1674-1056/21/6/068404 10.1364/OL.35.002361 10.1364/OL.11.000464 10.1109/JQE.2009.2034754 10.1088/1674-1056/21/7/074209 10.1088/0256-307X/29/5/054208 10.1364/OE.17.013588 10.1364/OE.14.010645 10.1088/1674-1056/21/3/034217 10.1364/OE.17.009858 10.1109/LPT.2011.2136431 10.1364/OE.15.003729 10.1007/s00340-005-1881-7 10.1088/1674-1056/19/7/074218 10.1038/nature01849 |
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Notes | Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber (HC-PCF). When the angle of the half-wave plate is rotated from 0° to 45°, the Raman soliton shifts from 2227 to 2300 nm, the output power of the CR increases 8.15 times, and the maximum output power ratio of the CR at 556 nm to the residual pump is estimated to be 20:1. The width of the output optical spectrum at visible wavelengths broadens from 25 to 45 nm, and the conversion efficiency of the CR can be above 28%. Moreover, the influences of the pump polarization and wavelength on the CR are studied, and the corresponding nonlinear processes are discussed. 11-5639/O4 polarization-dependent Cherenkov radiation, hollow-core photonic crystal fiber (HC-PCF) ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
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References | 11 22 12 14 15 16 17 Shen X W (4) 2012; 61 18 19 Hadley G R (23) 1998; 46 Liu S (8) 2012; 21 Yuan J H (13) 2010; 19 Zhao H (7) 2012; 21 Shen X W (5) 2012; 21 1 2 3 6 Han Y (9) 2012; 29 20 10 21 |
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Snippet | Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber... Efficient Cherenkov radiation (CR) is experimentally generated by a soliton self-frequency shift (SSFS) in a knot of hollow-core photonic crystal fiber... |
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SubjectTerms | Conversion Crystal fibers Knots Nonlinearity Photonic crystals Polarization Pumps Solitons Wavelengths 偏振相关 光波长 切伦科夫辐射 包层 孤子自频移 最大输出功率 空心 空芯光子晶体光纤 |
Title | Polarization-dependent efficient Cherenkov radiation at visible wavelengths in hollow-core photonic crystal fiber cladding |
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