Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber

A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Fu, Xinghu [verfasserIn] Wen, Jing [verfasserIn] Zhang, Yuepeng [verfasserIn] Wang, Dong [verfasserIn] Liu, Fan [verfasserIn] Xie, Haiyang [verfasserIn] Fu, Guangwei [verfasserIn] Bi, Weihong [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2018

Schlagwörter:	Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber

Übergeordnetes Werk:	Enthalten in: Optics communications - Amsterdam, 1969, 429, Seite 5-11
Übergeordnetes Werk:	volume:429 ; pages:5-11

DOI / URN:	10.1016/j.optcom.2018.07.077

Katalog-ID:	ELV000415715

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245	1	0	\|a Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
264		1	\|c 2018
336			\|a nicht spezifiziert \|b zzz \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
520			\|a A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1.
650		4	\|a Cladding mode resonance
650		4	\|a Fiber-optic sensors
650		4	\|a Curvature
650		4	\|a Triple cladding quartz specialty fiber
700	1		\|a Wen, Jing \|e verfasserin \|4 aut
700	1		\|a Zhang, Yuepeng \|e verfasserin \|4 aut
700	1		\|a Wang, Dong \|e verfasserin \|4 aut
700	1		\|a Liu, Fan \|e verfasserin \|4 aut
700	1		\|a Xie, Haiyang \|e verfasserin \|4 aut
700	1		\|a Fu, Guangwei \|e verfasserin \|4 aut
700	1		\|a Bi, Weihong \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t Optics communications \|d Amsterdam, 1969 \|g 429, Seite 5-11 \|h Online-Ressource \|w (DE-627)266889247 \|w (DE-600)1468811-6 \|w (DE-576)07596239X \|x 1873-0310 \|7 nnns
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author_variant	x f xf j w jw y z yz d w dw f l fl h x hx g f gf w b wb
matchkey_str	article:18730310:2018----::xeietlntertclnlssfuvtrsnobsdnldigoeeoacwtti
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publishDate	2018
allfields	10.1016/j.optcom.2018.07.077 doi (DE-627)ELV000415715 (ELSEVIER)S0030-4018(18)30669-2 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Fu, Xinghu verfasserin aut Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1. Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber Wen, Jing verfasserin aut Zhang, Yuepeng verfasserin aut Wang, Dong verfasserin aut Liu, Fan verfasserin aut Xie, Haiyang verfasserin aut Fu, Guangwei verfasserin aut Bi, Weihong verfasserin aut Enthalten in Optics communications Amsterdam, 1969 429, Seite 5-11 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:429 pages:5-11 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 429 5-11
spelling	10.1016/j.optcom.2018.07.077 doi (DE-627)ELV000415715 (ELSEVIER)S0030-4018(18)30669-2 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Fu, Xinghu verfasserin aut Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1. Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber Wen, Jing verfasserin aut Zhang, Yuepeng verfasserin aut Wang, Dong verfasserin aut Liu, Fan verfasserin aut Xie, Haiyang verfasserin aut Fu, Guangwei verfasserin aut Bi, Weihong verfasserin aut Enthalten in Optics communications Amsterdam, 1969 429, Seite 5-11 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:429 pages:5-11 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 429 5-11
allfields_unstemmed	10.1016/j.optcom.2018.07.077 doi (DE-627)ELV000415715 (ELSEVIER)S0030-4018(18)30669-2 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Fu, Xinghu verfasserin aut Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1. Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber Wen, Jing verfasserin aut Zhang, Yuepeng verfasserin aut Wang, Dong verfasserin aut Liu, Fan verfasserin aut Xie, Haiyang verfasserin aut Fu, Guangwei verfasserin aut Bi, Weihong verfasserin aut Enthalten in Optics communications Amsterdam, 1969 429, Seite 5-11 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:429 pages:5-11 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 429 5-11
allfieldsGer	10.1016/j.optcom.2018.07.077 doi (DE-627)ELV000415715 (ELSEVIER)S0030-4018(18)30669-2 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Fu, Xinghu verfasserin aut Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1. Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber Wen, Jing verfasserin aut Zhang, Yuepeng verfasserin aut Wang, Dong verfasserin aut Liu, Fan verfasserin aut Xie, Haiyang verfasserin aut Fu, Guangwei verfasserin aut Bi, Weihong verfasserin aut Enthalten in Optics communications Amsterdam, 1969 429, Seite 5-11 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:429 pages:5-11 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 429 5-11
allfieldsSound	10.1016/j.optcom.2018.07.077 doi (DE-627)ELV000415715 (ELSEVIER)S0030-4018(18)30669-2 DE-627 ger DE-627 rda eng 530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Fu, Xinghu verfasserin aut Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1. Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber Wen, Jing verfasserin aut Zhang, Yuepeng verfasserin aut Wang, Dong verfasserin aut Liu, Fan verfasserin aut Xie, Haiyang verfasserin aut Fu, Guangwei verfasserin aut Bi, Weihong verfasserin aut Enthalten in Optics communications Amsterdam, 1969 429, Seite 5-11 Online-Ressource (DE-627)266889247 (DE-600)1468811-6 (DE-576)07596239X 1873-0310 nnns volume:429 pages:5-11 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik AR 429 5-11
language	English
source	Enthalten in Optics communications 429, Seite 5-11 volume:429 pages:5-11
sourceStr	Enthalten in Optics communications 429, Seite 5-11 volume:429 pages:5-11
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bklname	Optik Quantenoptik nichtlineare Optik Technische Optik
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topic_facet	Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber
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container_title	Optics communications
authorswithroles_txt_mv	Fu, Xinghu @@aut@@ Wen, Jing @@aut@@ Zhang, Yuepeng @@aut@@ Wang, Dong @@aut@@ Liu, Fan @@aut@@ Xie, Haiyang @@aut@@ Fu, Guangwei @@aut@@ Bi, Weihong @@aut@@
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author	Fu, Xinghu
spellingShingle	Fu, Xinghu ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Cladding mode resonance misc Fiber-optic sensors misc Curvature misc Triple cladding quartz specialty fiber Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
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topic_title	530 DE-600 33.18 bkl 33.38 bkl 50.37 bkl Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber Cladding mode resonance Fiber-optic sensors Curvature Triple cladding quartz specialty fiber
topic	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Cladding mode resonance misc Fiber-optic sensors misc Curvature misc Triple cladding quartz specialty fiber
topic_unstemmed	ddc 530 bkl 33.18 bkl 33.38 bkl 50.37 misc Cladding mode resonance misc Fiber-optic sensors misc Curvature misc Triple cladding quartz specialty fiber
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title	Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
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title_full	Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
author_sort	Fu, Xinghu
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author_browse	Fu, Xinghu Wen, Jing Zhang, Yuepeng Wang, Dong Liu, Fan Xie, Haiyang Fu, Guangwei Bi, Weihong
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title_sort	experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
title_auth	Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
abstract	A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1.
abstractGer	A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1.
abstract_unstemmed	A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1.
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title_short	Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber
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author2	Wen, Jing Zhang, Yuepeng Wang, Dong Liu, Fan Xie, Haiyang Fu, Guangwei Bi, Weihong
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up_date	2024-07-06T17:53:33.238Z
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fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV000415715</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230524141741.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">230427s2018 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.optcom.2018.07.077</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV000415715</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0030-4018(18)30669-2</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rda</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.18</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.38</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">50.37</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Fu, Xinghu</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2018</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">A curvature sensor based on the triple cladding quartz specialty fiber (TCQSF) is proposed. The TCQSF is spliced between two single mode fibers. The curvature sensor is performed by cladding mode resonance. The TCQSF with the length of 10 mm, 35 mm, and 50 mm is prepared and applied to the curvature measurement experiment. The bending model is created and analyzed by the finite element method theoretically. The experiment results show that the curvature sensitivity of sensor with different length are −1.83001 nm/m−1, −1.56231 nm/m−1 and −1.0114 nm/m−1 in the curvature range of 0 ∼ 0.94m−1.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Cladding mode resonance</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fiber-optic sensors</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Curvature</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Triple cladding quartz specialty fiber</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Wen, Jing</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zhang, Yuepeng</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" 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Experimental and theoretical analysis of curvature sensor based on cladding mode resonance with triple cladding quartz specialty fiber

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