Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T
Purpose To develop 2D turbo spin‐echo (TSE) imaging using annular spiral rings (abbreviated “SPRING‐RIO TSE”) with compensation of concomitant gradient fields and B0 inhomogeneity at both 0.55T and 1.5T for fast T2‐weighted imaging. Methods Strategies of gradient waveform modifications were implemen...
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Veröffentlicht in: | Magnetic resonance in medicine 2023-08, Vol.90 (2), p.552-568 |
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creator | Wang, Zhixing Ramasawmy, Rajiv Feng, Xue Campbell‐Washburn, Adrienne E. Mugler, John P. Meyer, Craig H. |
description | Purpose
To develop 2D turbo spin‐echo (TSE) imaging using annular spiral rings (abbreviated “SPRING‐RIO TSE”) with compensation of concomitant gradient fields and B0 inhomogeneity at both 0.55T and 1.5T for fast T2‐weighted imaging.
Methods
Strategies of gradient waveform modifications were implemented in SPRING‐RIO TSE for compensation of self‐squared concomitant gradient terms at the TE and across echo spacings, along with reconstruction‐based corrections to simultaneously compensate for the residual concomitant gradient and B0 field induced phase accruals along the readout. The signal pathway disturbance caused by time‐varying and spatially dependent concomitant fields was simulated, and echo‐to‐echo phase variations before and after sequence‐based compensation were compared. Images from SPRING‐RIO TSE with no compensation, with compensation, and Cartesian TSE were also compared via phantom and in vivo acquisitions.
Results
Simulation showed how concomitant fields affected the signal evolution with no compensation, and both simulation and phantom studies demonstrated the performance of the proposed sequence modifications, as well as the readout off‐resonance corrections. Volunteer data showed that after full correction, the SPRING‐RIO TSE sequence achieved high image quality with improved SNR efficiency (15%–20% increase), and reduced RF SAR (˜50% reduction), compared to the standard Cartesian TSE, presenting potential benefits, especially in regaining SNR at low‐field (0.55T).
Conclusion
Implementation of SPRING‐RIO TSE with concomitant field compensation was tested at 0.55T and 1.5T. The compensation principles can be extended to correct for other trajectory types that are time‐varying along the echo train and temporally asymmetric in TSE‐based imaging. |
doi_str_mv | 10.1002/mrm.29663 |
format | Article |
fullrecord | <record><control><sourceid>proquest_pubme</sourceid><recordid>TN_cdi_pubmedcentral_primary_oai_pubmedcentral_nih_gov_10578525</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2799172992</sourcerecordid><originalsourceid>FETCH-LOGICAL-c4443-9f2195dde9fe2fb7f4cab86fc7fe85178a2d09370e32cbd43048fb4f39b319f33</originalsourceid><addsrcrecordid>eNp1kd9KHDEYxUOp1NX2oi8ggd7Ui1nzdzO5KmW1VVAKZXsdMplkzTKTrMlMy975CD5jn6RZV0WFXn3wnR-HczgAfMRoihEiJ33qp0TOZvQNmGBOSEW4ZG_BBAmGKool2wcHOa8QQlIK9g7sU4HoDFE6Aat5DCb2ftBhgL1eBjt48_f2znnbtbAoaxuyHnwM0MUEySnMa590V5DkwxIOY2ri9hfKx5rrCH1x2Sp6gGjK-QLq0EI85Yv3YM_pLtsPD_cQ_Pp2tpifV5c_vl_Mv15WhjFGK-kIlrxtrXSWuEY4ZnRTz5wRztYci1qTFsnSwFJimpZRxGrXMEdlU6o6Sg_Bl53vemx62xobhhJYrVNJljYqaq9eKsFfq2X8rTDiouaEF4fPDw4p3ow2D6r32diu08HGMSsipMSCSEkK-ukVuopjCqWfIjUum2DOWaGOd5RJMedk3VMajNR2QlUmVPcTFvboefwn8nGzApzsgD--s5v_O6mrn1c7y38Y46jE</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2819661554</pqid></control><display><type>article</type><title>Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T</title><source>MEDLINE</source><source>Wiley Online Library Journals Frontfile Complete</source><creator>Wang, Zhixing ; Ramasawmy, Rajiv ; Feng, Xue ; Campbell‐Washburn, Adrienne E. ; Mugler, John P. ; Meyer, Craig H.</creator><creatorcontrib>Wang, Zhixing ; Ramasawmy, Rajiv ; Feng, Xue ; Campbell‐Washburn, Adrienne E. ; Mugler, John P. ; Meyer, Craig H.</creatorcontrib><description>Purpose
To develop 2D turbo spin‐echo (TSE) imaging using annular spiral rings (abbreviated “SPRING‐RIO TSE”) with compensation of concomitant gradient fields and B0 inhomogeneity at both 0.55T and 1.5T for fast T2‐weighted imaging.
Methods
Strategies of gradient waveform modifications were implemented in SPRING‐RIO TSE for compensation of self‐squared concomitant gradient terms at the TE and across echo spacings, along with reconstruction‐based corrections to simultaneously compensate for the residual concomitant gradient and B0 field induced phase accruals along the readout. The signal pathway disturbance caused by time‐varying and spatially dependent concomitant fields was simulated, and echo‐to‐echo phase variations before and after sequence‐based compensation were compared. Images from SPRING‐RIO TSE with no compensation, with compensation, and Cartesian TSE were also compared via phantom and in vivo acquisitions.
Results
Simulation showed how concomitant fields affected the signal evolution with no compensation, and both simulation and phantom studies demonstrated the performance of the proposed sequence modifications, as well as the readout off‐resonance corrections. Volunteer data showed that after full correction, the SPRING‐RIO TSE sequence achieved high image quality with improved SNR efficiency (15%–20% increase), and reduced RF SAR (˜50% reduction), compared to the standard Cartesian TSE, presenting potential benefits, especially in regaining SNR at low‐field (0.55T).
Conclusion
Implementation of SPRING‐RIO TSE with concomitant field compensation was tested at 0.55T and 1.5T. The compensation principles can be extended to correct for other trajectory types that are time‐varying along the echo train and temporally asymmetric in TSE‐based imaging.</description><identifier>ISSN: 0740-3194</identifier><identifier>ISSN: 1522-2594</identifier><identifier>EISSN: 1522-2594</identifier><identifier>DOI: 10.1002/mrm.29663</identifier><identifier>PMID: 37036033</identifier><language>eng</language><publisher>United States: Wiley Subscription Services, Inc</publisher><subject>Brain - diagnostic imaging ; Cartesian coordinates ; Compensation ; concomitant gradient field ; fast imaging ; Humans ; Image Enhancement - methods ; Image quality ; Image reconstruction ; Inhomogeneity ; Magnetic Phenomena ; Magnetic Resonance Imaging - methods ; Phantoms, Imaging ; Phase variations ; Simulation ; spiral imaging ; turbo spin‐echo imaging ; Waveforms</subject><ispartof>Magnetic resonance in medicine, 2023-08, Vol.90 (2), p.552-568</ispartof><rights>2023 The Authors. published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine.</rights><rights>2023 The Authors. Magnetic Resonance in Medicine published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine.</rights><rights>2023. This article is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4443-9f2195dde9fe2fb7f4cab86fc7fe85178a2d09370e32cbd43048fb4f39b319f33</citedby><cites>FETCH-LOGICAL-c4443-9f2195dde9fe2fb7f4cab86fc7fe85178a2d09370e32cbd43048fb4f39b319f33</cites><orcidid>0000-0002-8189-0601 ; 0000-0002-2181-9889 ; 0000-0002-7169-5693</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fmrm.29663$$EPDF$$P50$$Gwiley$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fmrm.29663$$EHTML$$P50$$Gwiley$$Hfree_for_read</linktohtml><link.rule.ids>230,314,776,780,881,1411,27901,27902,45550,45551</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/37036033$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Wang, Zhixing</creatorcontrib><creatorcontrib>Ramasawmy, Rajiv</creatorcontrib><creatorcontrib>Feng, Xue</creatorcontrib><creatorcontrib>Campbell‐Washburn, Adrienne E.</creatorcontrib><creatorcontrib>Mugler, John P.</creatorcontrib><creatorcontrib>Meyer, Craig H.</creatorcontrib><title>Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T</title><title>Magnetic resonance in medicine</title><addtitle>Magn Reson Med</addtitle><description>Purpose
To develop 2D turbo spin‐echo (TSE) imaging using annular spiral rings (abbreviated “SPRING‐RIO TSE”) with compensation of concomitant gradient fields and B0 inhomogeneity at both 0.55T and 1.5T for fast T2‐weighted imaging.
Methods
Strategies of gradient waveform modifications were implemented in SPRING‐RIO TSE for compensation of self‐squared concomitant gradient terms at the TE and across echo spacings, along with reconstruction‐based corrections to simultaneously compensate for the residual concomitant gradient and B0 field induced phase accruals along the readout. The signal pathway disturbance caused by time‐varying and spatially dependent concomitant fields was simulated, and echo‐to‐echo phase variations before and after sequence‐based compensation were compared. Images from SPRING‐RIO TSE with no compensation, with compensation, and Cartesian TSE were also compared via phantom and in vivo acquisitions.
Results
Simulation showed how concomitant fields affected the signal evolution with no compensation, and both simulation and phantom studies demonstrated the performance of the proposed sequence modifications, as well as the readout off‐resonance corrections. Volunteer data showed that after full correction, the SPRING‐RIO TSE sequence achieved high image quality with improved SNR efficiency (15%–20% increase), and reduced RF SAR (˜50% reduction), compared to the standard Cartesian TSE, presenting potential benefits, especially in regaining SNR at low‐field (0.55T).
Conclusion
Implementation of SPRING‐RIO TSE with concomitant field compensation was tested at 0.55T and 1.5T. The compensation principles can be extended to correct for other trajectory types that are time‐varying along the echo train and temporally asymmetric in TSE‐based imaging.</description><subject>Brain - diagnostic imaging</subject><subject>Cartesian coordinates</subject><subject>Compensation</subject><subject>concomitant gradient field</subject><subject>fast imaging</subject><subject>Humans</subject><subject>Image Enhancement - methods</subject><subject>Image quality</subject><subject>Image reconstruction</subject><subject>Inhomogeneity</subject><subject>Magnetic Phenomena</subject><subject>Magnetic Resonance Imaging - methods</subject><subject>Phantoms, Imaging</subject><subject>Phase variations</subject><subject>Simulation</subject><subject>spiral imaging</subject><subject>turbo spin‐echo imaging</subject><subject>Waveforms</subject><issn>0740-3194</issn><issn>1522-2594</issn><issn>1522-2594</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>24P</sourceid><sourceid>EIF</sourceid><recordid>eNp1kd9KHDEYxUOp1NX2oi8ggd7Ui1nzdzO5KmW1VVAKZXsdMplkzTKTrMlMy975CD5jn6RZV0WFXn3wnR-HczgAfMRoihEiJ33qp0TOZvQNmGBOSEW4ZG_BBAmGKool2wcHOa8QQlIK9g7sU4HoDFE6Aat5DCb2ftBhgL1eBjt48_f2znnbtbAoaxuyHnwM0MUEySnMa590V5DkwxIOY2ri9hfKx5rrCH1x2Sp6gGjK-QLq0EI85Yv3YM_pLtsPD_cQ_Pp2tpifV5c_vl_Mv15WhjFGK-kIlrxtrXSWuEY4ZnRTz5wRztYci1qTFsnSwFJimpZRxGrXMEdlU6o6Sg_Bl53vemx62xobhhJYrVNJljYqaq9eKsFfq2X8rTDiouaEF4fPDw4p3ow2D6r32diu08HGMSsipMSCSEkK-ukVuopjCqWfIjUum2DOWaGOd5RJMedk3VMajNR2QlUmVPcTFvboefwn8nGzApzsgD--s5v_O6mrn1c7y38Y46jE</recordid><startdate>202308</startdate><enddate>202308</enddate><creator>Wang, Zhixing</creator><creator>Ramasawmy, Rajiv</creator><creator>Feng, Xue</creator><creator>Campbell‐Washburn, Adrienne E.</creator><creator>Mugler, John P.</creator><creator>Meyer, Craig H.</creator><general>Wiley Subscription Services, Inc</general><scope>24P</scope><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>8FD</scope><scope>FR3</scope><scope>K9.</scope><scope>M7Z</scope><scope>P64</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0002-8189-0601</orcidid><orcidid>https://orcid.org/0000-0002-2181-9889</orcidid><orcidid>https://orcid.org/0000-0002-7169-5693</orcidid></search><sort><creationdate>202308</creationdate><title>Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T</title><author>Wang, Zhixing ; Ramasawmy, Rajiv ; Feng, Xue ; Campbell‐Washburn, Adrienne E. ; Mugler, John P. ; Meyer, Craig H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4443-9f2195dde9fe2fb7f4cab86fc7fe85178a2d09370e32cbd43048fb4f39b319f33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Brain - diagnostic imaging</topic><topic>Cartesian coordinates</topic><topic>Compensation</topic><topic>concomitant gradient field</topic><topic>fast imaging</topic><topic>Humans</topic><topic>Image Enhancement - methods</topic><topic>Image quality</topic><topic>Image reconstruction</topic><topic>Inhomogeneity</topic><topic>Magnetic Phenomena</topic><topic>Magnetic Resonance Imaging - methods</topic><topic>Phantoms, Imaging</topic><topic>Phase variations</topic><topic>Simulation</topic><topic>spiral imaging</topic><topic>turbo spin‐echo imaging</topic><topic>Waveforms</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wang, Zhixing</creatorcontrib><creatorcontrib>Ramasawmy, Rajiv</creatorcontrib><creatorcontrib>Feng, Xue</creatorcontrib><creatorcontrib>Campbell‐Washburn, Adrienne E.</creatorcontrib><creatorcontrib>Mugler, John P.</creatorcontrib><creatorcontrib>Meyer, Craig H.</creatorcontrib><collection>Wiley Online Library Open Access</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>ProQuest Health & Medical Complete (Alumni)</collection><collection>Biochemistry Abstracts 1</collection><collection>Biotechnology and BioEngineering Abstracts</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Magnetic resonance in medicine</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, Zhixing</au><au>Ramasawmy, Rajiv</au><au>Feng, Xue</au><au>Campbell‐Washburn, Adrienne E.</au><au>Mugler, John P.</au><au>Meyer, Craig H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T</atitle><jtitle>Magnetic resonance in medicine</jtitle><addtitle>Magn Reson Med</addtitle><date>2023-08</date><risdate>2023</risdate><volume>90</volume><issue>2</issue><spage>552</spage><epage>568</epage><pages>552-568</pages><issn>0740-3194</issn><issn>1522-2594</issn><eissn>1522-2594</eissn><abstract>Purpose
To develop 2D turbo spin‐echo (TSE) imaging using annular spiral rings (abbreviated “SPRING‐RIO TSE”) with compensation of concomitant gradient fields and B0 inhomogeneity at both 0.55T and 1.5T for fast T2‐weighted imaging.
Methods
Strategies of gradient waveform modifications were implemented in SPRING‐RIO TSE for compensation of self‐squared concomitant gradient terms at the TE and across echo spacings, along with reconstruction‐based corrections to simultaneously compensate for the residual concomitant gradient and B0 field induced phase accruals along the readout. The signal pathway disturbance caused by time‐varying and spatially dependent concomitant fields was simulated, and echo‐to‐echo phase variations before and after sequence‐based compensation were compared. Images from SPRING‐RIO TSE with no compensation, with compensation, and Cartesian TSE were also compared via phantom and in vivo acquisitions.
Results
Simulation showed how concomitant fields affected the signal evolution with no compensation, and both simulation and phantom studies demonstrated the performance of the proposed sequence modifications, as well as the readout off‐resonance corrections. Volunteer data showed that after full correction, the SPRING‐RIO TSE sequence achieved high image quality with improved SNR efficiency (15%–20% increase), and reduced RF SAR (˜50% reduction), compared to the standard Cartesian TSE, presenting potential benefits, especially in regaining SNR at low‐field (0.55T).
Conclusion
Implementation of SPRING‐RIO TSE with concomitant field compensation was tested at 0.55T and 1.5T. The compensation principles can be extended to correct for other trajectory types that are time‐varying along the echo train and temporally asymmetric in TSE‐based imaging.</abstract><cop>United States</cop><pub>Wiley Subscription Services, Inc</pub><pmid>37036033</pmid><doi>10.1002/mrm.29663</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0002-8189-0601</orcidid><orcidid>https://orcid.org/0000-0002-2181-9889</orcidid><orcidid>https://orcid.org/0000-0002-7169-5693</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Brain - diagnostic imaging Cartesian coordinates Compensation concomitant gradient field fast imaging Humans Image Enhancement - methods Image quality Image reconstruction Inhomogeneity Magnetic Phenomena Magnetic Resonance Imaging - methods Phantoms, Imaging Phase variations Simulation spiral imaging turbo spin‐echo imaging Waveforms |
title | Concomitant magnetic‐field compensation for 2D spiral‐ring turbo spin‐echo imaging at 0.55T and 1.5T |
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