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All-Fiber-Integrated High-Power Supercontinuum Sources Based on Multi-Core Photonic Crystal Fibers
The obstacles of power scaling the supercontinuum (SC) source based on single-core photonic crystal fiber (PCF) are analyzed. The combination of high-power fiber lasers and multi-core PCFs would be a feasible method to obtain an all-fiber-integrated high-power broadband SC source (covering visible r...
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Published in: | IEEE journal of selected topics in quantum electronics 2014-09, Vol.20 (5), p.64-71 |
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creator | Chen, Hongwei Wei, Huifeng Liu, Tong Zhou, Xuanfeng Yan, Peiguang Chen, Zilun Chen, Shengping Li, Jinyan Hou, Jing Lu, Qisheng |
description | The obstacles of power scaling the supercontinuum (SC) source based on single-core photonic crystal fiber (PCF) are analyzed. The combination of high-power fiber lasers and multi-core PCFs would be a feasible method to obtain an all-fiber-integrated high-power broadband SC source (covering visible range). In this paper, we present a comprehensive study of high-power SC generation in multi-core PCFs. Comparative experiments are performed by using a high-power pulse-repetition-rate-tunable picosecond fiber laser to pump two kinds of home-made seven-core PCFs. The influences of PCF structure (fiber dispersion property) and pulse repetition rate (pulse peak power) on the SC generation in multi-core PCFs are investigated in detail. When the picosecond fiber laser at a pulse repetition rate of 1.9 GHz is adopted as the pump, 116 W SC spanning from 800 to 1700 nm is generated in 1# seven-core PCF. Also 64 W visible SC spanning at least 500-1700 nm is demonstrated in 2# seven-core PCF at a pump pulse repetition rate of 480 MHz. The potential of extending the spectral range and scaling the output power for the SC source based on multi-core PCFs are analyzed and discussed. |
doi_str_mv | 10.1109/JSTQE.2014.2304136 |
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The combination of high-power fiber lasers and multi-core PCFs would be a feasible method to obtain an all-fiber-integrated high-power broadband SC source (covering visible range). In this paper, we present a comprehensive study of high-power SC generation in multi-core PCFs. Comparative experiments are performed by using a high-power pulse-repetition-rate-tunable picosecond fiber laser to pump two kinds of home-made seven-core PCFs. The influences of PCF structure (fiber dispersion property) and pulse repetition rate (pulse peak power) on the SC generation in multi-core PCFs are investigated in detail. When the picosecond fiber laser at a pulse repetition rate of 1.9 GHz is adopted as the pump, 116 W SC spanning from 800 to 1700 nm is generated in 1# seven-core PCF. Also 64 W visible SC spanning at least 500-1700 nm is demonstrated in 2# seven-core PCF at a pump pulse repetition rate of 480 MHz. The potential of extending the spectral range and scaling the output power for the SC source based on multi-core PCFs are analyzed and discussed.</description><identifier>ISSN: 1077-260X</identifier><identifier>EISSN: 1558-4542</identifier><identifier>DOI: 10.1109/JSTQE.2014.2304136</identifier><identifier>CODEN: IJSQEN</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Broadband ; Crystal fibers ; Dispersions ; Fiber laser ; Fiber lasers ; fiber nonlinear optics ; Laser excitation ; multi-core photonic crystal fiber ; Optical fiber amplifiers ; Optical fiber dispersion ; optical fibers ; Photonic crystals ; Pulse repetition rate ; Pump lasers ; Pumps ; Spectra ; supercontinuum generation</subject><ispartof>IEEE journal of selected topics in quantum electronics, 2014-09, Vol.20 (5), p.64-71</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Sep/Oct 2014</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c377t-ad84d9b4dc4421364fd59c3578e3b4241f336592e96b9433394b3e5a14c2c38a3</citedby><cites>FETCH-LOGICAL-c377t-ad84d9b4dc4421364fd59c3578e3b4241f336592e96b9433394b3e5a14c2c38a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/6730666$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,54796</link.rule.ids></links><search><creatorcontrib>Chen, Hongwei</creatorcontrib><creatorcontrib>Wei, Huifeng</creatorcontrib><creatorcontrib>Liu, Tong</creatorcontrib><creatorcontrib>Zhou, Xuanfeng</creatorcontrib><creatorcontrib>Yan, Peiguang</creatorcontrib><creatorcontrib>Chen, Zilun</creatorcontrib><creatorcontrib>Chen, Shengping</creatorcontrib><creatorcontrib>Li, Jinyan</creatorcontrib><creatorcontrib>Hou, Jing</creatorcontrib><creatorcontrib>Lu, Qisheng</creatorcontrib><title>All-Fiber-Integrated High-Power Supercontinuum Sources Based on Multi-Core Photonic Crystal Fibers</title><title>IEEE journal of selected topics in quantum electronics</title><addtitle>JSTQE</addtitle><description>The obstacles of power scaling the supercontinuum (SC) source based on single-core photonic crystal fiber (PCF) are analyzed. The combination of high-power fiber lasers and multi-core PCFs would be a feasible method to obtain an all-fiber-integrated high-power broadband SC source (covering visible range). In this paper, we present a comprehensive study of high-power SC generation in multi-core PCFs. Comparative experiments are performed by using a high-power pulse-repetition-rate-tunable picosecond fiber laser to pump two kinds of home-made seven-core PCFs. The influences of PCF structure (fiber dispersion property) and pulse repetition rate (pulse peak power) on the SC generation in multi-core PCFs are investigated in detail. When the picosecond fiber laser at a pulse repetition rate of 1.9 GHz is adopted as the pump, 116 W SC spanning from 800 to 1700 nm is generated in 1# seven-core PCF. Also 64 W visible SC spanning at least 500-1700 nm is demonstrated in 2# seven-core PCF at a pump pulse repetition rate of 480 MHz. The potential of extending the spectral range and scaling the output power for the SC source based on multi-core PCFs are analyzed and discussed.</description><subject>Broadband</subject><subject>Crystal fibers</subject><subject>Dispersions</subject><subject>Fiber laser</subject><subject>Fiber lasers</subject><subject>fiber nonlinear optics</subject><subject>Laser excitation</subject><subject>multi-core photonic crystal fiber</subject><subject>Optical fiber amplifiers</subject><subject>Optical fiber dispersion</subject><subject>optical fibers</subject><subject>Photonic crystals</subject><subject>Pulse repetition rate</subject><subject>Pump lasers</subject><subject>Pumps</subject><subject>Spectra</subject><subject>supercontinuum generation</subject><issn>1077-260X</issn><issn>1558-4542</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNpdkMtOwzAQRSMEEuXxA7CJxIaNi-0ZO8kSKp4CUVSQ2EWOMy1BaVzsRIi_x6WIBauZxblXMydJjgQfC8GLs7vZ89PlWHKBYwkcBeitZCSUyhkqlNtx51nGpOavu8leCO-c8xxzPkqq87ZlV01Fnt12PS286alOb5rFG5u6T_LpbFiRt67rm24YlunMDd5SSC9MiJzr0oeh7Rs2cZ7S6ZvrXdfYdOK_Qm_a9Kc3HCQ7c9MGOvyd-8nL1eXz5IbdP17fTs7vmYUs65mpc6yLCmuLKOMDOK9VYUFlOUGFEsUcQKtCUqGrAgGgwApIGYFWWsgN7Cenm96Vdx8Dhb5cNsFS25qO3BBKoSQvEJXGiJ78Q9_jX128LlJcgeZcQKTkhrLeheBpXq58szT-qxS8XGsvf7SXa-3lr_YYOt6EGiL6C-gMuNYavgHLP31g</recordid><startdate>201409</startdate><enddate>201409</enddate><creator>Chen, Hongwei</creator><creator>Wei, Huifeng</creator><creator>Liu, Tong</creator><creator>Zhou, Xuanfeng</creator><creator>Yan, Peiguang</creator><creator>Chen, Zilun</creator><creator>Chen, Shengping</creator><creator>Li, Jinyan</creator><creator>Hou, Jing</creator><creator>Lu, Qisheng</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The combination of high-power fiber lasers and multi-core PCFs would be a feasible method to obtain an all-fiber-integrated high-power broadband SC source (covering visible range). In this paper, we present a comprehensive study of high-power SC generation in multi-core PCFs. Comparative experiments are performed by using a high-power pulse-repetition-rate-tunable picosecond fiber laser to pump two kinds of home-made seven-core PCFs. The influences of PCF structure (fiber dispersion property) and pulse repetition rate (pulse peak power) on the SC generation in multi-core PCFs are investigated in detail. When the picosecond fiber laser at a pulse repetition rate of 1.9 GHz is adopted as the pump, 116 W SC spanning from 800 to 1700 nm is generated in 1# seven-core PCF. Also 64 W visible SC spanning at least 500-1700 nm is demonstrated in 2# seven-core PCF at a pump pulse repetition rate of 480 MHz. The potential of extending the spectral range and scaling the output power for the SC source based on multi-core PCFs are analyzed and discussed.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JSTQE.2014.2304136</doi><tpages>8</tpages></addata></record> |
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subjects | Broadband Crystal fibers Dispersions Fiber laser Fiber lasers fiber nonlinear optics Laser excitation multi-core photonic crystal fiber Optical fiber amplifiers Optical fiber dispersion optical fibers Photonic crystals Pulse repetition rate Pump lasers Pumps Spectra supercontinuum generation |
title | All-Fiber-Integrated High-Power Supercontinuum Sources Based on Multi-Core Photonic Crystal Fibers |
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