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Effect of Cross-Sectional Structure on Optical Properties of Metal-Filled Side-Hole Fiber

The effect of the cross-sectional structure of metal-filled side-hole fiber on the birefringence and thermooptic properties was investigated by the fiber-optic Sagnac loop interferometry. The optical fibers having different cross-sectional structures filled with indium metal were fabricated by drawi...

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Published in:Journal of lightwave technology 2015-07, Vol.33 (14), p.2930-2937
Main Authors: Lee, Seung Ho, Kim, Bok Hyeon, Son, Dong Hoon, Jeong, Seongmook, Kim, Youngwoong, Han, Won-Taek
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container_issue 14
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container_title Journal of lightwave technology
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creator Lee, Seung Ho
Kim, Bok Hyeon
Son, Dong Hoon
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description The effect of the cross-sectional structure of metal-filled side-hole fiber on the birefringence and thermooptic properties was investigated by the fiber-optic Sagnac loop interferometry. The optical fibers having different cross-sectional structures filled with indium metal were fabricated by drawing a fiber preform with two side holes at different temperatures followed by metal infiltration. The original circular core and two identical holes in the fiber preform were deformed into the fiber core with various core ellipticities and different hole diameters after the drawing. It was found that the fiber birefringence ({\boldsymbol B} ) and the temperature dependence were strongly influenced by the deformation of the fiber cross section, the birefringence increased from 5.68 \,{\times}\, 10 ^{-5} to 1.16 \,{\times}\, 10^{-4} with the increase of the core ellipticity from 0.273 to 0.412. Additional birefringence was found to be induced after the infiltration of indium into holes due to the large thermal expansion mismatch between indium and silica glass of the fiber. The temperature sensitivities of the unfilled side-hole fibers ( d( δλ _{n} )/dT ) were almost the same and found to be constant of ∼−0.60 nm/K regardless of the fiber cross sections. On the other hand, the sensitivities of the indium-filled side-hole fibers ( d( δλ_{m} )/dT ) were enhanced 10-15 times larger than those of the unfilled side-hole fibers, increased from − 5.98 to −11.03  nm/K with the increase of the filler indium diameter from ∼ 18.5 to 24.1 μm, respectively.
doi_str_mv 10.1109/JLT.2015.2415795
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The optical fibers having different cross-sectional structures filled with indium metal were fabricated by drawing a fiber preform with two side holes at different temperatures followed by metal infiltration. The original circular core and two identical holes in the fiber preform were deformed into the fiber core with various core ellipticities and different hole diameters after the drawing. It was found that the fiber birefringence (<inline-formula><tex-math>{\boldsymbol B}</tex-math> </inline-formula>) and the temperature dependence were strongly influenced by the deformation of the fiber cross section, the birefringence increased from <inline-formula><tex-math>5.68 \,{\times}\, 10 ^{-5}</tex-math> </inline-formula> to <inline-formula><tex-math>1.16 \,{\times}\, 10^{-4}</tex-math></inline-formula> with the increase of the core ellipticity from <inline-formula><tex-math>0.273</tex-math></inline-formula> to <inline-formula> <tex-math>0.412</tex-math></inline-formula>. Additional birefringence was found to be induced after the infiltration of indium into holes due to the large thermal expansion mismatch between indium and silica glass of the fiber. The temperature sensitivities of the unfilled side-hole fibers ( d( δλ<inline-formula> <tex-math>_{n}</tex-math></inline-formula> )/dT ) were almost the same and found to be constant of ∼−<inline-formula><tex-math>0.60</tex-math></inline-formula> nm/K regardless of the fiber cross sections. On the other hand, the sensitivities of the indium-filled side-hole fibers ( d( δλ<inline-formula><tex-math>_{m}</tex-math></inline-formula> )/dT ) were enhanced 10-15 times larger than those of the unfilled side-hole fibers, increased from −<inline-formula><tex-math> 5.98</tex-math></inline-formula> to −<inline-formula><tex-math>11.03</tex-math></inline-formula>  nm/K with the increase of the filler indium diameter from ∼ <inline-formula><tex-math>18.5 </tex-math></inline-formula> to <inline-formula><tex-math>24.1</tex-math></inline-formula> μm, respectively.]]></description><identifier>ISSN: 0733-8724</identifier><identifier>EISSN: 1558-2213</identifier><identifier>DOI: 10.1109/JLT.2015.2415795</identifier><identifier>CODEN: JLTEDG</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>birefringence ; Fiber optics ; Indium ; Optical fiber couplers ; Optical fiber devices ; Optical fiber polarization ; Sagnac fiber interferometers ; Temperature measurement ; thermo-optical devices</subject><ispartof>Journal of lightwave technology, 2015-07, Vol.33 (14), p.2930-2937</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Jul 15, 2015</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c291t-63f060f181c7df69a003a4dd9aee0b25751626c7704a63017fe26cf9e1a58f8e3</citedby><cites>FETCH-LOGICAL-c291t-63f060f181c7df69a003a4dd9aee0b25751626c7704a63017fe26cf9e1a58f8e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/7065204$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,54775</link.rule.ids></links><search><creatorcontrib>Lee, Seung Ho</creatorcontrib><creatorcontrib>Kim, Bok Hyeon</creatorcontrib><creatorcontrib>Son, Dong Hoon</creatorcontrib><creatorcontrib>Jeong, Seongmook</creatorcontrib><creatorcontrib>Kim, Youngwoong</creatorcontrib><creatorcontrib>Han, Won-Taek</creatorcontrib><title>Effect of Cross-Sectional Structure on Optical Properties of Metal-Filled Side-Hole Fiber</title><title>Journal of lightwave technology</title><addtitle>JLT</addtitle><description><![CDATA[The effect of the cross-sectional structure of metal-filled side-hole fiber on the birefringence and thermooptic properties was investigated by the fiber-optic Sagnac loop interferometry. The optical fibers having different cross-sectional structures filled with indium metal were fabricated by drawing a fiber preform with two side holes at different temperatures followed by metal infiltration. The original circular core and two identical holes in the fiber preform were deformed into the fiber core with various core ellipticities and different hole diameters after the drawing. It was found that the fiber birefringence (<inline-formula><tex-math>{\boldsymbol B}</tex-math> </inline-formula>) and the temperature dependence were strongly influenced by the deformation of the fiber cross section, the birefringence increased from <inline-formula><tex-math>5.68 \,{\times}\, 10 ^{-5}</tex-math> </inline-formula> to <inline-formula><tex-math>1.16 \,{\times}\, 10^{-4}</tex-math></inline-formula> with the increase of the core ellipticity from <inline-formula><tex-math>0.273</tex-math></inline-formula> to <inline-formula> <tex-math>0.412</tex-math></inline-formula>. Additional birefringence was found to be induced after the infiltration of indium into holes due to the large thermal expansion mismatch between indium and silica glass of the fiber. The temperature sensitivities of the unfilled side-hole fibers ( d( δλ<inline-formula> <tex-math>_{n}</tex-math></inline-formula> )/dT ) were almost the same and found to be constant of ∼−<inline-formula><tex-math>0.60</tex-math></inline-formula> nm/K regardless of the fiber cross sections. On the other hand, the sensitivities of the indium-filled side-hole fibers ( d( δλ<inline-formula><tex-math>_{m}</tex-math></inline-formula> )/dT ) were enhanced 10-15 times larger than those of the unfilled side-hole fibers, increased from −<inline-formula><tex-math> 5.98</tex-math></inline-formula> to −<inline-formula><tex-math>11.03</tex-math></inline-formula>  nm/K with the increase of the filler indium diameter from ∼ <inline-formula><tex-math>18.5 </tex-math></inline-formula> to <inline-formula><tex-math>24.1</tex-math></inline-formula> μm, respectively.]]></description><subject>birefringence</subject><subject>Fiber optics</subject><subject>Indium</subject><subject>Optical fiber couplers</subject><subject>Optical fiber devices</subject><subject>Optical fiber polarization</subject><subject>Sagnac fiber interferometers</subject><subject>Temperature measurement</subject><subject>thermo-optical devices</subject><issn>0733-8724</issn><issn>1558-2213</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNo9kEFLw0AQhRdRsFbvgpeA560zm-xu9iiltUqlQuvB07JNZiElNnE3OfjvTWhxLsMb3ht4H2P3CDNEME9v691MAMqZyFBqIy_YBKXMuRCYXrIJ6DTluRbZNbuJ8QCAWZbrCftaeE9FlzQ-mYcmRr4dVNUcXZ1su9AXXR8oaY7Jpu2qYjh-hKal0FUUx8g7da7my6quqUy2VUl81dSULKs9hVt25V0d6e68p-xzudjNV3y9eXmdP695IQx2XKUeFHjMsdClV8YBpC4rS-OIYC-klqiEKrSGzKkUUHsapDeETuY-p3TKHk9_29D89BQ7e2j6MBSIFpVRZhiEwQUnVzG2DORtG6pvF34tgh0B2gGgHQHaM8Ah8nCKVET0b9egpIAs_QPO3msx</recordid><startdate>20150715</startdate><enddate>20150715</enddate><creator>Lee, Seung Ho</creator><creator>Kim, Bok Hyeon</creator><creator>Son, Dong Hoon</creator><creator>Jeong, Seongmook</creator><creator>Kim, Youngwoong</creator><creator>Han, Won-Taek</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The optical fibers having different cross-sectional structures filled with indium metal were fabricated by drawing a fiber preform with two side holes at different temperatures followed by metal infiltration. The original circular core and two identical holes in the fiber preform were deformed into the fiber core with various core ellipticities and different hole diameters after the drawing. It was found that the fiber birefringence (<inline-formula><tex-math>{\boldsymbol B}</tex-math> </inline-formula>) and the temperature dependence were strongly influenced by the deformation of the fiber cross section, the birefringence increased from <inline-formula><tex-math>5.68 \,{\times}\, 10 ^{-5}</tex-math> </inline-formula> to <inline-formula><tex-math>1.16 \,{\times}\, 10^{-4}</tex-math></inline-formula> with the increase of the core ellipticity from <inline-formula><tex-math>0.273</tex-math></inline-formula> to <inline-formula> <tex-math>0.412</tex-math></inline-formula>. Additional birefringence was found to be induced after the infiltration of indium into holes due to the large thermal expansion mismatch between indium and silica glass of the fiber. The temperature sensitivities of the unfilled side-hole fibers ( d( δλ<inline-formula> <tex-math>_{n}</tex-math></inline-formula> )/dT ) were almost the same and found to be constant of ∼−<inline-formula><tex-math>0.60</tex-math></inline-formula> nm/K regardless of the fiber cross sections. On the other hand, the sensitivities of the indium-filled side-hole fibers ( d( δλ<inline-formula><tex-math>_{m}</tex-math></inline-formula> )/dT ) were enhanced 10-15 times larger than those of the unfilled side-hole fibers, increased from −<inline-formula><tex-math> 5.98</tex-math></inline-formula> to −<inline-formula><tex-math>11.03</tex-math></inline-formula>  nm/K with the increase of the filler indium diameter from ∼ <inline-formula><tex-math>18.5 </tex-math></inline-formula> to <inline-formula><tex-math>24.1</tex-math></inline-formula> μm, respectively.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JLT.2015.2415795</doi><tpages>8</tpages></addata></record>
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subjects birefringence
Fiber optics
Indium
Optical fiber couplers
Optical fiber devices
Optical fiber polarization
Sagnac fiber interferometers
Temperature measurement
thermo-optical devices
title Effect of Cross-Sectional Structure on Optical Properties of Metal-Filled Side-Hole Fiber
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