Ozkan Doganay, Kundan Thind, Trevor Wade, Alexei Ouriadov, Giles E. Santyr
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{"title":"大鼠肺超极化129Xe MRI的单发射/单接收射频线圈配置","authors":"Ozkan Doganay, Kundan Thind, Trevor Wade, Alexei Ouriadov, Giles E. Santyr","doi":"10.1002/cmr.b.21288","DOIUrl":null,"url":null,"abstract":"<p>We report a novel radiofrequency (RF) transmit-only/receive-only (TO/RO) coil configuration providing excellent transmit <b>B<sub>1+</sub></b> field uniformity as well as high sensitivity for hyperpolarized <sup>129</sup>Xe MR lung imaging of rats at 3T (35.34 MHz). The TO/RO coil configuration consisted of two separate components: (i) a high-pass birdcage transmit coil which produces a homogeneous <b>B<sub>1+</sub></b> magnetic field, (ii) a saddle-shaped single-turn receive-only surface coil that couples closely to the rat lung. On transmit, the receive-only coil is decoupled from the transmit coil using a detuning circuit. On receive, the bird-cage coil is deactivated through the use of PIN diodes. The sensitivity and uniformity of the saddle-shaped receive coil were optimized solving the Biot-Savart equation using 3D finite element modeling. The electrical performance of the new TO/RO configuration in transmit/receive (T/R) mode was compared with a commercial T/R birdcage coil of similar diameter, which was considering to be the gold standard for conventional T/R mode imaging. Experimental results in phantoms confirm that our novel TO/RO coil configuration provides a factor of three increase in SNR without compromising <b>B<sub>1</sub></b> transmit uniformity compared with the commercial T/R birdcage coil configuration. The novel TO/RO coil was successfully tested for in vivo rat lung imaging. © 2015 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 45B: 115–124, 2015</p>","PeriodicalId":50623,"journal":{"name":"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering","volume":"45 3","pages":"115-124"},"PeriodicalIF":0.9000,"publicationDate":"2015-06-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1002/cmr.b.21288","citationCount":"8","resultStr":"{\"title\":\"Transmit-only/receive-only radiofrequency coil configuration for hyperpolarized 129Xe MRI of rat lungs\",\"authors\":\"Ozkan Doganay, Kundan Thind, Trevor Wade, Alexei Ouriadov, Giles E. Santyr\",\"doi\":\"10.1002/cmr.b.21288\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We report a novel radiofrequency (RF) transmit-only/receive-only (TO/RO) coil configuration providing excellent transmit <b>B<sub>1+</sub></b> field uniformity as well as high sensitivity for hyperpolarized <sup>129</sup>Xe MR lung imaging of rats at 3T (35.34 MHz). The TO/RO coil configuration consisted of two separate components: (i) a high-pass birdcage transmit coil which produces a homogeneous <b>B<sub>1+</sub></b> magnetic field, (ii) a saddle-shaped single-turn receive-only surface coil that couples closely to the rat lung. On transmit, the receive-only coil is decoupled from the transmit coil using a detuning circuit. On receive, the bird-cage coil is deactivated through the use of PIN diodes. The sensitivity and uniformity of the saddle-shaped receive coil were optimized solving the Biot-Savart equation using 3D finite element modeling. The electrical performance of the new TO/RO configuration in transmit/receive (T/R) mode was compared with a commercial T/R birdcage coil of similar diameter, which was considering to be the gold standard for conventional T/R mode imaging. Experimental results in phantoms confirm that our novel TO/RO coil configuration provides a factor of three increase in SNR without compromising <b>B<sub>1</sub></b> transmit uniformity compared with the commercial T/R birdcage coil configuration. The novel TO/RO coil was successfully tested for in vivo rat lung imaging. © 2015 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 45B: 115–124, 2015</p>\",\"PeriodicalId\":50623,\"journal\":{\"name\":\"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering\",\"volume\":\"45 3\",\"pages\":\"115-124\"},\"PeriodicalIF\":0.9000,\"publicationDate\":\"2015-06-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1002/cmr.b.21288\",\"citationCount\":\"8\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering\",\"FirstCategoryId\":\"3\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/cmr.b.21288\",\"RegionNum\":4,\"RegionCategory\":\"医学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Concepts in Magnetic Resonance Part B-Magnetic Resonance Engineering","FirstCategoryId":"3","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/cmr.b.21288","RegionNum":4,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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