SQUID‐detected MRI at 132 μT with T 1 ‐weighted contrast established at 10 μT–300 mT
T 1 ‐weighted contrast MRI with prepolarization was detected with a superconducting quantum interference device (SQUID). A spin evolution period in a variable field between prepolarization and detection enabled the measurement of T 1 in fields between 1.7 μT and 300 mT; T 1 dispersion curves of agar...
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Veröffentlicht in: | Magnetic resonance in medicine 2005-01, Vol.53 (1), p.9-14 |
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creator | Lee, Seung Kyun Möβle, Michael Myers, Whittier Kelso, Nathan Trabesinger, Andreas H. Pines, Alexander Clarke, John |
description | T
1
‐weighted contrast MRI with prepolarization was detected with a superconducting quantum interference device (SQUID). A spin evolution period in a variable field between prepolarization and detection enabled the measurement of
T
1
in fields between 1.7 μT and 300 mT;
T
1
dispersion curves of agarose gel samples over five decades in frequency were obtained. SQUID detection at 5.6 kHz drastically reduces the field homogeneity requirements compared to conventional field‐cycling methods using Faraday coil detection. This allows
T
1
dispersion measurements to be easily combined with MRI, so that
T
1
in a wide range of fields can be used for tissue contrast. Images of gel phantoms with
T
1
‐weighted contrast at four different fields between 10 μT and 300 mT demonstrated dramatic contrast enhancement in low fields. A modified inversion recovery technique further enhanced the contrast by selectively suppressing the signal contribution for a specific value of the low‐field
T
1
. Magn Reson Med 53:9–14, 2005. Published 2004 Wiley‐Liss, Inc. |
doi_str_mv | 10.1002/mrm.20316 |
format | Article |
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1
‐weighted contrast MRI with prepolarization was detected with a superconducting quantum interference device (SQUID). A spin evolution period in a variable field between prepolarization and detection enabled the measurement of
T
1
in fields between 1.7 μT and 300 mT;
T
1
dispersion curves of agarose gel samples over five decades in frequency were obtained. SQUID detection at 5.6 kHz drastically reduces the field homogeneity requirements compared to conventional field‐cycling methods using Faraday coil detection. This allows
T
1
dispersion measurements to be easily combined with MRI, so that
T
1
in a wide range of fields can be used for tissue contrast. Images of gel phantoms with
T
1
‐weighted contrast at four different fields between 10 μT and 300 mT demonstrated dramatic contrast enhancement in low fields. A modified inversion recovery technique further enhanced the contrast by selectively suppressing the signal contribution for a specific value of the low‐field
T
1
. Magn Reson Med 53:9–14, 2005. Published 2004 Wiley‐Liss, Inc.</description><identifier>ISSN: 0740-3194</identifier><identifier>EISSN: 1522-2594</identifier><identifier>DOI: 10.1002/mrm.20316</identifier><language>eng</language><ispartof>Magnetic resonance in medicine, 2005-01, Vol.53 (1), p.9-14</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c159t-b0cbaf09ec730b1d562b93705b41f6ba444e3ebfcbdf2224a579340764b0d6263</citedby><cites>FETCH-LOGICAL-c159t-b0cbaf09ec730b1d562b93705b41f6ba444e3ebfcbdf2224a579340764b0d6263</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>Lee, Seung Kyun</creatorcontrib><creatorcontrib>Möβle, Michael</creatorcontrib><creatorcontrib>Myers, Whittier</creatorcontrib><creatorcontrib>Kelso, Nathan</creatorcontrib><creatorcontrib>Trabesinger, Andreas H.</creatorcontrib><creatorcontrib>Pines, Alexander</creatorcontrib><creatorcontrib>Clarke, John</creatorcontrib><title>SQUID‐detected MRI at 132 μT with T 1 ‐weighted contrast established at 10 μT–300 mT</title><title>Magnetic resonance in medicine</title><description>T
1
‐weighted contrast MRI with prepolarization was detected with a superconducting quantum interference device (SQUID). A spin evolution period in a variable field between prepolarization and detection enabled the measurement of
T
1
in fields between 1.7 μT and 300 mT;
T
1
dispersion curves of agarose gel samples over five decades in frequency were obtained. SQUID detection at 5.6 kHz drastically reduces the field homogeneity requirements compared to conventional field‐cycling methods using Faraday coil detection. This allows
T
1
dispersion measurements to be easily combined with MRI, so that
T
1
in a wide range of fields can be used for tissue contrast. Images of gel phantoms with
T
1
‐weighted contrast at four different fields between 10 μT and 300 mT demonstrated dramatic contrast enhancement in low fields. A modified inversion recovery technique further enhanced the contrast by selectively suppressing the signal contribution for a specific value of the low‐field
T
1
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1
‐weighted contrast MRI with prepolarization was detected with a superconducting quantum interference device (SQUID). A spin evolution period in a variable field between prepolarization and detection enabled the measurement of
T
1
in fields between 1.7 μT and 300 mT;
T
1
dispersion curves of agarose gel samples over five decades in frequency were obtained. SQUID detection at 5.6 kHz drastically reduces the field homogeneity requirements compared to conventional field‐cycling methods using Faraday coil detection. This allows
T
1
dispersion measurements to be easily combined with MRI, so that
T
1
in a wide range of fields can be used for tissue contrast. Images of gel phantoms with
T
1
‐weighted contrast at four different fields between 10 μT and 300 mT demonstrated dramatic contrast enhancement in low fields. A modified inversion recovery technique further enhanced the contrast by selectively suppressing the signal contribution for a specific value of the low‐field
T
1
. Magn Reson Med 53:9–14, 2005. Published 2004 Wiley‐Liss, Inc.</abstract><doi>10.1002/mrm.20316</doi><tpages>6</tpages></addata></record> |
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title | SQUID‐detected MRI at 132 μT with T 1 ‐weighted contrast established at 10 μT–300 mT |
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