Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds
Imaging exams involving hyperpolarized, 13 C‐labeled compounds require novel RF coils for efficient signal utilization. While 13 C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps pri...
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Veröffentlicht in: | Magnetic resonance in medicine 2008-10, Vol.60 (4), p.928-933 |
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container_title | Magnetic resonance in medicine |
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creator | Hancu, Ileana Wood, S. James Piel, Joseph Whitt, David B. Fish, Kenneth M. Rutt, Brian K. Tropp, James Dixon, W. Thomas |
description | Imaging exams involving hyperpolarized,
13
C‐labeled compounds require novel RF coils for efficient signal utilization. While
13
C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps prior to the image acquisition. Imaging/pulsing at the
1
H frequency is typically used for anatomical localization and shimming. Flip angle (FA) calibration, which is difficult or impossible to achieve at the
13
C frequency, can be accurately performed at the
23
Na frequency using the natural abundance signal that exists in any living tissue. We demonstrate here a single RF resonant structure that is capable of operating linearly at the
1
H and
23
Na frequencies for scan setup steps, and in quadrature at the
13
C frequency for imaging. Images at the three resonant frequencies of this coil are presented from an exam involving hyperpolarized
13
C compounds in vivo. Magn Reson Med 60:928–933, 2008. © 2008 Wiley‐Liss, Inc. |
doi_str_mv | 10.1002/mrm.21698 |
format | Article |
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13
C‐labeled compounds require novel RF coils for efficient signal utilization. While
13
C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps prior to the image acquisition. Imaging/pulsing at the
1
H frequency is typically used for anatomical localization and shimming. Flip angle (FA) calibration, which is difficult or impossible to achieve at the
13
C frequency, can be accurately performed at the
23
Na frequency using the natural abundance signal that exists in any living tissue. We demonstrate here a single RF resonant structure that is capable of operating linearly at the
1
H and
23
Na frequencies for scan setup steps, and in quadrature at the
13
C frequency for imaging. Images at the three resonant frequencies of this coil are presented from an exam involving hyperpolarized
13
C compounds in vivo. Magn Reson Med 60:928–933, 2008. © 2008 Wiley‐Liss, Inc.</description><identifier>ISSN: 0740-3194</identifier><identifier>EISSN: 1522-2594</identifier><identifier>DOI: 10.1002/mrm.21698</identifier><language>eng</language><ispartof>Magnetic resonance in medicine, 2008-10, Vol.60 (4), p.928-933</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c748-f29aac828bce5fc5c2f1dc06f3db930380bc96c1b1171a49b50bcb22213321933</citedby><cites>FETCH-LOGICAL-c748-f29aac828bce5fc5c2f1dc06f3db930380bc96c1b1171a49b50bcb22213321933</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Hancu, Ileana</creatorcontrib><creatorcontrib>Wood, S. James</creatorcontrib><creatorcontrib>Piel, Joseph</creatorcontrib><creatorcontrib>Whitt, David B.</creatorcontrib><creatorcontrib>Fish, Kenneth M.</creatorcontrib><creatorcontrib>Rutt, Brian K.</creatorcontrib><creatorcontrib>Tropp, James</creatorcontrib><creatorcontrib>Dixon, W. Thomas</creatorcontrib><title>Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds</title><title>Magnetic resonance in medicine</title><description>Imaging exams involving hyperpolarized,
13
C‐labeled compounds require novel RF coils for efficient signal utilization. While
13
C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps prior to the image acquisition. Imaging/pulsing at the
1
H frequency is typically used for anatomical localization and shimming. Flip angle (FA) calibration, which is difficult or impossible to achieve at the
13
C frequency, can be accurately performed at the
23
Na frequency using the natural abundance signal that exists in any living tissue. We demonstrate here a single RF resonant structure that is capable of operating linearly at the
1
H and
23
Na frequencies for scan setup steps, and in quadrature at the
13
C frequency for imaging. Images at the three resonant frequencies of this coil are presented from an exam involving hyperpolarized
13
C compounds in vivo. Magn Reson Med 60:928–933, 2008. © 2008 Wiley‐Liss, Inc.</description><issn>0740-3194</issn><issn>1522-2594</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNotkM1KxDAURoMoWEcXvkG2gh1zk_5lKcUZhQFBui9JmnQibVMTZ1FXPoLP6JOYUVeXe7-Pw-UgdA1kDYTQu9GPawoFr05QAjmlKc15dooSUmYkZcCzc3QRwishhPMyS1DX7L3W359fxuu3g57Ugl82WDk74E4H20-6w8Z57OZ3O9qPuNlR9HbqsTN4v8zaz24Q_pjcYmC4jqhBSD3EpnLj7A5TFy7RmRFD0Ff_c4WazUNTP6a75-1Tfb9LVZlVqaFcCFXRSiqdG5UraqBTpDCsk5wRVhGpeKFAApQgMi7zeJCUUmCMAmdshW7-sMq7ELw27ezjt35pgbRHO2200_7aYT9WCFrN</recordid><startdate>200810</startdate><enddate>200810</enddate><creator>Hancu, Ileana</creator><creator>Wood, S. James</creator><creator>Piel, Joseph</creator><creator>Whitt, David B.</creator><creator>Fish, Kenneth M.</creator><creator>Rutt, Brian K.</creator><creator>Tropp, James</creator><creator>Dixon, W. Thomas</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>200810</creationdate><title>Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds</title><author>Hancu, Ileana ; Wood, S. James ; Piel, Joseph ; Whitt, David B. ; Fish, Kenneth M. ; Rutt, Brian K. ; Tropp, James ; Dixon, W. Thomas</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c748-f29aac828bce5fc5c2f1dc06f3db930380bc96c1b1171a49b50bcb22213321933</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hancu, Ileana</creatorcontrib><creatorcontrib>Wood, S. James</creatorcontrib><creatorcontrib>Piel, Joseph</creatorcontrib><creatorcontrib>Whitt, David B.</creatorcontrib><creatorcontrib>Fish, Kenneth M.</creatorcontrib><creatorcontrib>Rutt, Brian K.</creatorcontrib><creatorcontrib>Tropp, James</creatorcontrib><creatorcontrib>Dixon, W. Thomas</creatorcontrib><collection>CrossRef</collection><jtitle>Magnetic resonance in medicine</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hancu, Ileana</au><au>Wood, S. James</au><au>Piel, Joseph</au><au>Whitt, David B.</au><au>Fish, Kenneth M.</au><au>Rutt, Brian K.</au><au>Tropp, James</au><au>Dixon, W. Thomas</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds</atitle><jtitle>Magnetic resonance in medicine</jtitle><date>2008-10</date><risdate>2008</risdate><volume>60</volume><issue>4</issue><spage>928</spage><epage>933</epage><pages>928-933</pages><issn>0740-3194</issn><eissn>1522-2594</eissn><abstract>Imaging exams involving hyperpolarized,
13
C‐labeled compounds require novel RF coils for efficient signal utilization. While
13
C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps prior to the image acquisition. Imaging/pulsing at the
1
H frequency is typically used for anatomical localization and shimming. Flip angle (FA) calibration, which is difficult or impossible to achieve at the
13
C frequency, can be accurately performed at the
23
Na frequency using the natural abundance signal that exists in any living tissue. We demonstrate here a single RF resonant structure that is capable of operating linearly at the
1
H and
23
Na frequencies for scan setup steps, and in quadrature at the
13
C frequency for imaging. Images at the three resonant frequencies of this coil are presented from an exam involving hyperpolarized
13
C compounds in vivo. Magn Reson Med 60:928–933, 2008. © 2008 Wiley‐Liss, Inc.</abstract><doi>10.1002/mrm.21698</doi><tpages>6</tpages></addata></record> |
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language | eng |
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source | Wiley Free Content; Wiley Online Library Journals Frontfile Complete |
title | Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds |
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