Noninvasive prediction of SAR distributions with an electro-optical E field sensor
An integrated electro-optical (eo) E field sensor is developed on the basis of a Ti:LiNbO3 Mach-Zehnder interferometer. A measuring device based on the lock-in principle is introduced to register the E field in phase and amplitude using this E field probe. Segmented electrodes are used to minimize i...
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Veröffentlicht in: | International journal of hyperthermia 1995, Vol.11 (2), p.295-310 |
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creator | Wust, P. Meier, T. Seebass, M. Fähling, H. Petermann, K. Felix, R. |
description | An integrated electro-optical (eo) E field sensor is developed on the basis of a Ti:LiNbO3 Mach-Zehnder interferometer. A measuring device based on the lock-in principle is introduced to register the E field in phase and amplitude using this E field probe. Segmented electrodes are used to minimize influences from the dielectric surroundings on the base point capacitance of the receiving dipole. The operating point is stabilized against drift phenomena resulting from optical damage and pyroelectric effect. Sensitivity, dynamic range, harmonic distortions and mechanical properties of a prototype of this electro-optical E field sensor are evaluated. A phantom setup in the SIGMA-60 applicator was developed to test this electro-optical sensor for hyperthermia applications. Power deposition patterns of various standard adjustments of the SIGMA ring are visualized in an elliptical lamp phantom. Simultaneously, E field in phase and amplitude is determined on a closed curve in 10° steps around the phantom in a substitute bolus. The numbers are stored and utilized as boundary conditions in a two-dimensional finite elements code which calculates the SAR distribution on an appropriate triangular grid inside the closed curve. An excellent qualitative agreement is obtained between visualized and calculated SAR patterns. This novel measurement method is therefore suitable for noninvasive monitoring of SAR patterns during clinical application of regional radiofrequency hyperthermia. |
doi_str_mv | 10.3109/02656739509022464 |
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A measuring device based on the lock-in principle is introduced to register the E field in phase and amplitude using this E field probe. Segmented electrodes are used to minimize influences from the dielectric surroundings on the base point capacitance of the receiving dipole. The operating point is stabilized against drift phenomena resulting from optical damage and pyroelectric effect. Sensitivity, dynamic range, harmonic distortions and mechanical properties of a prototype of this electro-optical E field sensor are evaluated. A phantom setup in the SIGMA-60 applicator was developed to test this electro-optical sensor for hyperthermia applications. Power deposition patterns of various standard adjustments of the SIGMA ring are visualized in an elliptical lamp phantom. Simultaneously, E field in phase and amplitude is determined on a closed curve in 10° steps around the phantom in a substitute bolus. The numbers are stored and utilized as boundary conditions in a two-dimensional finite elements code which calculates the SAR distribution on an appropriate triangular grid inside the closed curve. An excellent qualitative agreement is obtained between visualized and calculated SAR patterns. This novel measurement method is therefore suitable for noninvasive monitoring of SAR patterns during clinical application of regional radiofrequency hyperthermia.</description><identifier>ISSN: 0265-6736</identifier><identifier>EISSN: 1464-5157</identifier><identifier>DOI: 10.3109/02656739509022464</identifier><identifier>PMID: 7790742</identifier><language>eng</language><publisher>England: Informa UK Ltd</publisher><subject>E field sensor ; Electrodes ; hyperthermia ; Hyperthermia, Induced - instrumentation ; Hyperthermia, Induced - methods ; Radio Waves ; Radiofrequency</subject><ispartof>International journal of hyperthermia, 1995, Vol.11 (2), p.295-310</ispartof><rights>1995 Informa UK Ltd All rights reserved: reproduction in whole or part not permitted 1995</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c316t-443f0733eeaa1fe824336660f235386118161ca9da85fa690db295e62f31e1123</citedby><cites>FETCH-LOGICAL-c316t-443f0733eeaa1fe824336660f235386118161ca9da85fa690db295e62f31e1123</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.tandfonline.com/doi/pdf/10.3109/02656739509022464$$EPDF$$P50$$Ginformaworld$$H</linktopdf><linktohtml>$$Uhttps://www.tandfonline.com/doi/full/10.3109/02656739509022464$$EHTML$$P50$$Ginformaworld$$H</linktohtml><link.rule.ids>314,776,780,4010,27900,27901,27902,59620,60409,61194,61375</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/7790742$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Wust, P.</creatorcontrib><creatorcontrib>Meier, T.</creatorcontrib><creatorcontrib>Seebass, M.</creatorcontrib><creatorcontrib>Fähling, H.</creatorcontrib><creatorcontrib>Petermann, K.</creatorcontrib><creatorcontrib>Felix, R.</creatorcontrib><title>Noninvasive prediction of SAR distributions with an electro-optical E field sensor</title><title>International journal of hyperthermia</title><addtitle>Int J Hyperthermia</addtitle><description>An integrated electro-optical (eo) E field sensor is developed on the basis of a Ti:LiNbO3 Mach-Zehnder interferometer. A measuring device based on the lock-in principle is introduced to register the E field in phase and amplitude using this E field probe. Segmented electrodes are used to minimize influences from the dielectric surroundings on the base point capacitance of the receiving dipole. The operating point is stabilized against drift phenomena resulting from optical damage and pyroelectric effect. Sensitivity, dynamic range, harmonic distortions and mechanical properties of a prototype of this electro-optical E field sensor are evaluated. A phantom setup in the SIGMA-60 applicator was developed to test this electro-optical sensor for hyperthermia applications. Power deposition patterns of various standard adjustments of the SIGMA ring are visualized in an elliptical lamp phantom. Simultaneously, E field in phase and amplitude is determined on a closed curve in 10° steps around the phantom in a substitute bolus. The numbers are stored and utilized as boundary conditions in a two-dimensional finite elements code which calculates the SAR distribution on an appropriate triangular grid inside the closed curve. An excellent qualitative agreement is obtained between visualized and calculated SAR patterns. This novel measurement method is therefore suitable for noninvasive monitoring of SAR patterns during clinical application of regional radiofrequency hyperthermia.</description><subject>E field sensor</subject><subject>Electrodes</subject><subject>hyperthermia</subject><subject>Hyperthermia, Induced - instrumentation</subject><subject>Hyperthermia, Induced - methods</subject><subject>Radio Waves</subject><subject>Radiofrequency</subject><issn>0265-6736</issn><issn>1464-5157</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp9kF1LIzEUhsOiaLfuD9gLIVfezZqvSWbQmyLuKhQXXPd6SDMnNCVNapJR_PdOaRFE9OqF835weBD6SckvTkl7TpispeJtTVrCmJDiG5rQUaqa1uoATbZ-NQbkMfqe84oQImqmjtCRUi1Rgk3Q_V0MLjzp7J4AbxL0zhQXA44W_5vd497lktxi2N4yfnZliXXA4MGUFKu4Kc5oj6-xdeB7nCHkmE7QodU-w4-9TtH_39cPVzfV_O-f26vZvDKcylIJwS1RnANoTS00THAupSSW8Zo3ktKGSmp02-umtlq2pF-wtgbJLKdAKeNTdLbb3aT4OEAu3dplA97rAHHInVJcCNKQMUh3QZNizglst0lurdNLR0m35dh94Dh2Tvfjw2IN_VtjD270L3e-CzamtX6Oyfdd0S8-Jpt0MC5vpz-fv3hXX4L2ZWl0gm4VhxRGbl889wqFF5IE</recordid><startdate>1995</startdate><enddate>1995</enddate><creator>Wust, P.</creator><creator>Meier, T.</creator><creator>Seebass, M.</creator><creator>Fähling, H.</creator><creator>Petermann, K.</creator><creator>Felix, R.</creator><general>Informa UK Ltd</general><general>Taylor & Francis</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>1995</creationdate><title>Noninvasive prediction of SAR distributions with an electro-optical E field sensor</title><author>Wust, P. ; Meier, T. ; Seebass, M. ; Fähling, H. ; Petermann, K. ; Felix, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c316t-443f0733eeaa1fe824336660f235386118161ca9da85fa690db295e62f31e1123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1995</creationdate><topic>E field sensor</topic><topic>Electrodes</topic><topic>hyperthermia</topic><topic>Hyperthermia, Induced - instrumentation</topic><topic>Hyperthermia, Induced - methods</topic><topic>Radio Waves</topic><topic>Radiofrequency</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wust, P.</creatorcontrib><creatorcontrib>Meier, T.</creatorcontrib><creatorcontrib>Seebass, M.</creatorcontrib><creatorcontrib>Fähling, H.</creatorcontrib><creatorcontrib>Petermann, K.</creatorcontrib><creatorcontrib>Felix, R.</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>International journal of hyperthermia</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wust, P.</au><au>Meier, T.</au><au>Seebass, M.</au><au>Fähling, H.</au><au>Petermann, K.</au><au>Felix, R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Noninvasive prediction of SAR distributions with an electro-optical E field sensor</atitle><jtitle>International journal of hyperthermia</jtitle><addtitle>Int J Hyperthermia</addtitle><date>1995</date><risdate>1995</risdate><volume>11</volume><issue>2</issue><spage>295</spage><epage>310</epage><pages>295-310</pages><issn>0265-6736</issn><eissn>1464-5157</eissn><abstract>An integrated electro-optical (eo) E field sensor is developed on the basis of a Ti:LiNbO3 Mach-Zehnder interferometer. A measuring device based on the lock-in principle is introduced to register the E field in phase and amplitude using this E field probe. Segmented electrodes are used to minimize influences from the dielectric surroundings on the base point capacitance of the receiving dipole. The operating point is stabilized against drift phenomena resulting from optical damage and pyroelectric effect. Sensitivity, dynamic range, harmonic distortions and mechanical properties of a prototype of this electro-optical E field sensor are evaluated. A phantom setup in the SIGMA-60 applicator was developed to test this electro-optical sensor for hyperthermia applications. Power deposition patterns of various standard adjustments of the SIGMA ring are visualized in an elliptical lamp phantom. Simultaneously, E field in phase and amplitude is determined on a closed curve in 10° steps around the phantom in a substitute bolus. The numbers are stored and utilized as boundary conditions in a two-dimensional finite elements code which calculates the SAR distribution on an appropriate triangular grid inside the closed curve. An excellent qualitative agreement is obtained between visualized and calculated SAR patterns. This novel measurement method is therefore suitable for noninvasive monitoring of SAR patterns during clinical application of regional radiofrequency hyperthermia.</abstract><cop>England</cop><pub>Informa UK Ltd</pub><pmid>7790742</pmid><doi>10.3109/02656739509022464</doi><tpages>16</tpages></addata></record> |
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subjects | E field sensor Electrodes hyperthermia Hyperthermia, Induced - instrumentation Hyperthermia, Induced - methods Radio Waves Radiofrequency |
title | Noninvasive prediction of SAR distributions with an electro-optical E field sensor |
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