Permittivity measurement of the substrate by using the corrected differential phase method and quick-press test fixture
Permittivity is critical for analyzing electromagnetic propagation in the substrate. The differential phase method is desirable to measure the permittivity of the substrate. The actual measurement is usually required to be started at a low frequency to avoid the S21-phase ambiguity problem. To get r...
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Veröffentlicht in: | Review of scientific instruments 2022-09, Vol.93 (9) |
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description | Permittivity is critical for analyzing electromagnetic propagation in the substrate. The differential phase method is desirable to measure the permittivity of the substrate. The actual measurement is usually required to be started at a low frequency to avoid the S21-phase ambiguity problem. To get rid of this problem, the unwrapped S21-phase is calculated accurately at any measurement frequency range. In the classical method of calculating the real permittivity from the effective permittivity, the calculation error increases gradually with increasing frequency, especially in an ultra-wide frequency range. To effectively reduce the error, the ratio of the calculated and real permittivity is used in the permittivity correction, which is a function with respect to frequency, dimension, and permittivity of the microstrip line. A two-step fitting process is proposed to reduce the dimension of the ratio function from three-dimension to two-dimension. Furthermore, a quick-press test fixture is designed for a more convenient measurement, which is characterized by no soldering requirement and ultra-wide frequency range. Compared with the stripline resonant method, in the proposed method, the maximum deviations of the four substrates are 0.035, −0.04, 0.07, and 0.13, in the frequency range of 1–40 GHz. |
doi_str_mv | 10.1063/5.0087780 |
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The differential phase method is desirable to measure the permittivity of the substrate. The actual measurement is usually required to be started at a low frequency to avoid the S21-phase ambiguity problem. To get rid of this problem, the unwrapped S21-phase is calculated accurately at any measurement frequency range. In the classical method of calculating the real permittivity from the effective permittivity, the calculation error increases gradually with increasing frequency, especially in an ultra-wide frequency range. To effectively reduce the error, the ratio of the calculated and real permittivity is used in the permittivity correction, which is a function with respect to frequency, dimension, and permittivity of the microstrip line. A two-step fitting process is proposed to reduce the dimension of the ratio function from three-dimension to two-dimension. Furthermore, a quick-press test fixture is designed for a more convenient measurement, which is characterized by no soldering requirement and ultra-wide frequency range. Compared with the stripline resonant method, in the proposed method, the maximum deviations of the four substrates are 0.035, −0.04, 0.07, and 0.13, in the frequency range of 1–40 GHz.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/5.0087780</identifier><identifier>CODEN: RSINAK</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Error reduction ; Frequency ranges ; Mathematical analysis ; Microstrip transmission lines ; Permittivity ; Scientific apparatus & instruments ; Substrates</subject><ispartof>Review of scientific instruments, 2022-09, Vol.93 (9)</ispartof><rights>Author(s)</rights><rights>2022 Author(s). Published under an exclusive license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c217t-c198a5d9a7f93bf322e509a67e786b700dc5d2e50cb504163c0318b2c068b023</cites><orcidid>0000-0003-0463-9293 ; 0000-0003-2313-7934 ; 0000-0002-7303-5058</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/rsi/article-lookup/doi/10.1063/5.0087780$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,4510,27922,27923,76154</link.rule.ids></links><search><creatorcontrib>Zhu, Hui</creatorcontrib><creatorcontrib>Gao, Chong</creatorcontrib><creatorcontrib>Li, En</creatorcontrib><creatorcontrib>Yu, Chengyong</creatorcontrib><creatorcontrib>Xu, Xinjie</creatorcontrib><creatorcontrib>Pan, Junwen</creatorcontrib><title>Permittivity measurement of the substrate by using the corrected differential phase method and quick-press test fixture</title><title>Review of scientific instruments</title><description>Permittivity is critical for analyzing electromagnetic propagation in the substrate. The differential phase method is desirable to measure the permittivity of the substrate. The actual measurement is usually required to be started at a low frequency to avoid the S21-phase ambiguity problem. To get rid of this problem, the unwrapped S21-phase is calculated accurately at any measurement frequency range. In the classical method of calculating the real permittivity from the effective permittivity, the calculation error increases gradually with increasing frequency, especially in an ultra-wide frequency range. To effectively reduce the error, the ratio of the calculated and real permittivity is used in the permittivity correction, which is a function with respect to frequency, dimension, and permittivity of the microstrip line. A two-step fitting process is proposed to reduce the dimension of the ratio function from three-dimension to two-dimension. Furthermore, a quick-press test fixture is designed for a more convenient measurement, which is characterized by no soldering requirement and ultra-wide frequency range. Compared with the stripline resonant method, in the proposed method, the maximum deviations of the four substrates are 0.035, −0.04, 0.07, and 0.13, in the frequency range of 1–40 GHz.</description><subject>Error reduction</subject><subject>Frequency ranges</subject><subject>Mathematical analysis</subject><subject>Microstrip transmission lines</subject><subject>Permittivity</subject><subject>Scientific apparatus & instruments</subject><subject>Substrates</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLAzEUhYMoWKsL_0HAlcLUm8lMMrOU4gsKuug-ZDKJTe08mmSq_femtuhC8G4uHL5zDhyELglMCDB6m08ACs4LOEIjAkWZcJbSYzQCoFnCeFacojPvlxAvJ2SEPl61a2wIdmPDFjda-sHpRrcBdwaHhcZ-qHxwMmhcbfHgbfv2LavOOa2CrnFtjdEuOqxc4X4hvY4xYdHVWLY1Xg9WvSe9097joH3Axn6GWHGOToxceX1x-GM0f7ifT5-S2cvj8_RulqiU8JAoUhYyr0vJTUkrQ9NU51BKxjUvWMUBapXXO01VOWSEUQWUFFWqgBUVpHSMrvaxvevWQ-wXy25wbWwUKSdZybI4TKSu95RynfdOG9E720i3FQTEblaRi8Oskb3Zs17ZIIPt2h9407lfUPS1-Q_-m_wFKCuHyg</recordid><startdate>20220901</startdate><enddate>20220901</enddate><creator>Zhu, Hui</creator><creator>Gao, Chong</creator><creator>Li, En</creator><creator>Yu, Chengyong</creator><creator>Xu, Xinjie</creator><creator>Pan, Junwen</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-0463-9293</orcidid><orcidid>https://orcid.org/0000-0003-2313-7934</orcidid><orcidid>https://orcid.org/0000-0002-7303-5058</orcidid></search><sort><creationdate>20220901</creationdate><title>Permittivity measurement of the substrate by using the corrected differential phase method and quick-press test fixture</title><author>Zhu, Hui ; Gao, Chong ; Li, En ; Yu, Chengyong ; Xu, Xinjie ; Pan, Junwen</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c217t-c198a5d9a7f93bf322e509a67e786b700dc5d2e50cb504163c0318b2c068b023</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Error reduction</topic><topic>Frequency ranges</topic><topic>Mathematical analysis</topic><topic>Microstrip transmission lines</topic><topic>Permittivity</topic><topic>Scientific apparatus & instruments</topic><topic>Substrates</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhu, Hui</creatorcontrib><creatorcontrib>Gao, Chong</creatorcontrib><creatorcontrib>Li, En</creatorcontrib><creatorcontrib>Yu, Chengyong</creatorcontrib><creatorcontrib>Xu, Xinjie</creatorcontrib><creatorcontrib>Pan, Junwen</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhu, Hui</au><au>Gao, Chong</au><au>Li, En</au><au>Yu, Chengyong</au><au>Xu, Xinjie</au><au>Pan, Junwen</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Permittivity measurement of the substrate by using the corrected differential phase method and quick-press test fixture</atitle><jtitle>Review of scientific instruments</jtitle><date>2022-09-01</date><risdate>2022</risdate><volume>93</volume><issue>9</issue><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>Permittivity is critical for analyzing electromagnetic propagation in the substrate. The differential phase method is desirable to measure the permittivity of the substrate. The actual measurement is usually required to be started at a low frequency to avoid the S21-phase ambiguity problem. To get rid of this problem, the unwrapped S21-phase is calculated accurately at any measurement frequency range. In the classical method of calculating the real permittivity from the effective permittivity, the calculation error increases gradually with increasing frequency, especially in an ultra-wide frequency range. To effectively reduce the error, the ratio of the calculated and real permittivity is used in the permittivity correction, which is a function with respect to frequency, dimension, and permittivity of the microstrip line. A two-step fitting process is proposed to reduce the dimension of the ratio function from three-dimension to two-dimension. Furthermore, a quick-press test fixture is designed for a more convenient measurement, which is characterized by no soldering requirement and ultra-wide frequency range. Compared with the stripline resonant method, in the proposed method, the maximum deviations of the four substrates are 0.035, −0.04, 0.07, and 0.13, in the frequency range of 1–40 GHz.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0087780</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0003-0463-9293</orcidid><orcidid>https://orcid.org/0000-0003-2313-7934</orcidid><orcidid>https://orcid.org/0000-0002-7303-5058</orcidid></addata></record> |
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source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Error reduction Frequency ranges Mathematical analysis Microstrip transmission lines Permittivity Scientific apparatus & instruments Substrates |
title | Permittivity measurement of the substrate by using the corrected differential phase method and quick-press test fixture |
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