Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks
The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyze...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Yin, Rui [verfasserIn] Cao, Lingxin [verfasserIn] Huang, Qingjie [verfasserIn] Lu, Lin [verfasserIn] Yang, Xu [verfasserIn] Ying, Jun [verfasserIn] Yang, Hongliang [verfasserIn] Ji, Wei [verfasserIn] Liu, Pengcheng [verfasserIn] Jiang, Shouzhen [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2023 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Measurement - Amsterdam [u.a.] : Elsevier Science, 1983, 215 |
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| Übergeordnetes Werk: |
volume:215 |
| DOI / URN: |
10.1016/j.measurement.2023.112852 |
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| Katalog-ID: |
ELV009840400 |
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| 245 | 1 | 0 | |a Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks |
| 264 | 1 | |c 2023 | |
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| 520 | |a The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. | ||
| 650 | 4 | |a Larger measurement range | |
| 650 | 4 | |a Optical sensor | |
| 650 | 4 | |a Free spectral range | |
| 650 | 4 | |a Photonics | |
| 700 | 1 | |a Cao, Lingxin |e verfasserin |4 aut | |
| 700 | 1 | |a Huang, Qingjie |e verfasserin |0 (orcid)0000-0003-1504-1158 |4 aut | |
| 700 | 1 | |a Lu, Lin |e verfasserin |0 (orcid)0000-0001-5881-892X |4 aut | |
| 700 | 1 | |a Yang, Xu |e verfasserin |4 aut | |
| 700 | 1 | |a Ying, Jun |e verfasserin |4 aut | |
| 700 | 1 | |a Yang, Hongliang |e verfasserin |4 aut | |
| 700 | 1 | |a Ji, Wei |e verfasserin |4 aut | |
| 700 | 1 | |a Liu, Pengcheng |e verfasserin |4 aut | |
| 700 | 1 | |a Jiang, Shouzhen |e verfasserin |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Measurement |d Amsterdam [u.a.] : Elsevier Science, 1983 |g 215 |h Online-Ressource |w (DE-627)320404927 |w (DE-600)2000550-7 |w (DE-576)259484342 |7 nnns |
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| 912 | |a GBV_ILN_370 | ||
| 912 | |a GBV_ILN_602 | ||
| 912 | |a GBV_ILN_702 | ||
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| 912 | |a GBV_ILN_2088 | ||
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| 912 | |a GBV_ILN_4249 | ||
| 912 | |a GBV_ILN_4251 | ||
| 912 | |a GBV_ILN_4305 | ||
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| 912 | |a GBV_ILN_4313 | ||
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| 912 | |a GBV_ILN_4338 | ||
| 912 | |a GBV_ILN_4393 | ||
| 912 | |a GBV_ILN_4700 | ||
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10.1016/j.measurement.2023.112852 doi (DE-627)ELV009840400 (ELSEVIER)S0263-2241(23)00416-5 DE-627 ger DE-627 rda eng 660 VZ 50.21 bkl Yin, Rui verfasserin aut Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. Larger measurement range Optical sensor Free spectral range Photonics Cao, Lingxin verfasserin aut Huang, Qingjie verfasserin (orcid)0000-0003-1504-1158 aut Lu, Lin verfasserin (orcid)0000-0001-5881-892X aut Yang, Xu verfasserin aut Ying, Jun verfasserin aut Yang, Hongliang verfasserin aut Ji, Wei verfasserin aut Liu, Pengcheng verfasserin aut Jiang, Shouzhen verfasserin aut Enthalten in Measurement Amsterdam [u.a.] : Elsevier Science, 1983 215 Online-Ressource (DE-627)320404927 (DE-600)2000550-7 (DE-576)259484342 nnns volume:215 GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 Messtechnik VZ AR 215 |
| spelling |
10.1016/j.measurement.2023.112852 doi (DE-627)ELV009840400 (ELSEVIER)S0263-2241(23)00416-5 DE-627 ger DE-627 rda eng 660 VZ 50.21 bkl Yin, Rui verfasserin aut Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. Larger measurement range Optical sensor Free spectral range Photonics Cao, Lingxin verfasserin aut Huang, Qingjie verfasserin (orcid)0000-0003-1504-1158 aut Lu, Lin verfasserin (orcid)0000-0001-5881-892X aut Yang, Xu verfasserin aut Ying, Jun verfasserin aut Yang, Hongliang verfasserin aut Ji, Wei verfasserin aut Liu, Pengcheng verfasserin aut Jiang, Shouzhen verfasserin aut Enthalten in Measurement Amsterdam [u.a.] : Elsevier Science, 1983 215 Online-Ressource (DE-627)320404927 (DE-600)2000550-7 (DE-576)259484342 nnns volume:215 GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 Messtechnik VZ AR 215 |
| allfields_unstemmed |
10.1016/j.measurement.2023.112852 doi (DE-627)ELV009840400 (ELSEVIER)S0263-2241(23)00416-5 DE-627 ger DE-627 rda eng 660 VZ 50.21 bkl Yin, Rui verfasserin aut Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. Larger measurement range Optical sensor Free spectral range Photonics Cao, Lingxin verfasserin aut Huang, Qingjie verfasserin (orcid)0000-0003-1504-1158 aut Lu, Lin verfasserin (orcid)0000-0001-5881-892X aut Yang, Xu verfasserin aut Ying, Jun verfasserin aut Yang, Hongliang verfasserin aut Ji, Wei verfasserin aut Liu, Pengcheng verfasserin aut Jiang, Shouzhen verfasserin aut Enthalten in Measurement Amsterdam [u.a.] : Elsevier Science, 1983 215 Online-Ressource (DE-627)320404927 (DE-600)2000550-7 (DE-576)259484342 nnns volume:215 GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 Messtechnik VZ AR 215 |
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10.1016/j.measurement.2023.112852 doi (DE-627)ELV009840400 (ELSEVIER)S0263-2241(23)00416-5 DE-627 ger DE-627 rda eng 660 VZ 50.21 bkl Yin, Rui verfasserin aut Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. Larger measurement range Optical sensor Free spectral range Photonics Cao, Lingxin verfasserin aut Huang, Qingjie verfasserin (orcid)0000-0003-1504-1158 aut Lu, Lin verfasserin (orcid)0000-0001-5881-892X aut Yang, Xu verfasserin aut Ying, Jun verfasserin aut Yang, Hongliang verfasserin aut Ji, Wei verfasserin aut Liu, Pengcheng verfasserin aut Jiang, Shouzhen verfasserin aut Enthalten in Measurement Amsterdam [u.a.] : Elsevier Science, 1983 215 Online-Ressource (DE-627)320404927 (DE-600)2000550-7 (DE-576)259484342 nnns volume:215 GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 Messtechnik VZ AR 215 |
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10.1016/j.measurement.2023.112852 doi (DE-627)ELV009840400 (ELSEVIER)S0263-2241(23)00416-5 DE-627 ger DE-627 rda eng 660 VZ 50.21 bkl Yin, Rui verfasserin aut Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks 2023 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. Larger measurement range Optical sensor Free spectral range Photonics Cao, Lingxin verfasserin aut Huang, Qingjie verfasserin (orcid)0000-0003-1504-1158 aut Lu, Lin verfasserin (orcid)0000-0001-5881-892X aut Yang, Xu verfasserin aut Ying, Jun verfasserin aut Yang, Hongliang verfasserin aut Ji, Wei verfasserin aut Liu, Pengcheng verfasserin aut Jiang, Shouzhen verfasserin aut Enthalten in Measurement Amsterdam [u.a.] : Elsevier Science, 1983 215 Online-Ressource (DE-627)320404927 (DE-600)2000550-7 (DE-576)259484342 nnns volume:215 GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 50.21 Messtechnik VZ AR 215 |
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Yin, Rui @@aut@@ Cao, Lingxin @@aut@@ Huang, Qingjie @@aut@@ Lu, Lin @@aut@@ Yang, Xu @@aut@@ Ying, Jun @@aut@@ Yang, Hongliang @@aut@@ Ji, Wei @@aut@@ Liu, Pengcheng @@aut@@ Jiang, Shouzhen @@aut@@ |
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expansion of measurement range: tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks |
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Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks |
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The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. |
| abstractGer |
The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. |
| abstract_unstemmed |
The two-peak method has been widely used to expand the measurement range of F-P cavities in the past decades. Previous studies have found that a dozen peak pairs should be involved to calculate the average value to reduce the possibility of misjudgment of the interference order m. This paper analyzes the impact of data error on the two-peak method and proposes the condition for correctly judging m using only one peak pair or peak-valley pair at the current technical level: m <1000. For experimental verification, a force sensor based on an integrated LiNbO3 asymmetric Mach-Zehnder interferometer (AMZI) with m around 30 is fabricated and tested. The measurement range is originally 63 N due to the limitation of FSR (free spectral range). With the help of the two-peak method with only one peak-valley pair, the measurement range is successfully increased to 150 N. Experimental data show that the two-peak method exhibits a large tolerance when m is far less than 1000. This result extends the application of the two-peak method to the field of integrated optical sensors. |
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Expansion of measurement range: Tolerance analysis and application of the two-peak method for optical sensors with a few spectral peaks |
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Cao, Lingxin Huang, Qingjie Lu, Lin Yang, Xu Ying, Jun Yang, Hongliang Ji, Wei Liu, Pengcheng Jiang, Shouzhen |
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| score |
7.397456 |