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An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver
Purpose To find an optimized b‐value distribution for reproducible triexponential intravoxel incoherent motion (IVIM) exams in the liver. Methods A numeric optimization of b‐value distributions was performed using the triexponential IVIM equation and 27 different IVIM parameter sets. Starting with a...
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Published in: | Magnetic resonance in medicine 2021-04, Vol.85 (4), p.2095-2108 |
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creator | Riexinger, Andreas Martin, Jan Wetscherek, Andreas Kuder, Tristan Anselm Uder, Michael Hensel, Bernhard Laun, Frederik Bernd |
description | Purpose
To find an optimized b‐value distribution for reproducible triexponential intravoxel incoherent motion (IVIM) exams in the liver.
Methods
A numeric optimization of b‐value distributions was performed using the triexponential IVIM equation and 27 different IVIM parameter sets. Starting with an initially optimized distribution of 6 b‐values, the number of b‐values was increased stepwise. Each new b‐value was chosen from a set of 64 predefined b‐values based on the computed summed relative mean error of the fitted triexponential IVIM parameters. This process was repeated for up to 100 b‐values. In simulations and in vivo measurements, optimized b‐value distributions were compared to 4 representative distributions found in literature.
Results
The first 16 optimized b‐values were 0, 0.3, 0.3, 70, 200, 800, 70, 1, 3.5, 5, 70, 1.2, 6, 45, 1.5, and 60 in units of s/mm2. Low b‐values were much more frequent than high b‐values. The optimized b‐value distribution resulted in a higher fit stability compared to distributions used in literature in both, simulation and in vivo measurements. Using more than 6 b‐values, ideally 16 or more, increased the fit stability considerably.
Conclusion
Using optimized b‐values, the fit uncertainty in triexponential IVIM can be largely reduced. Ideally, 16 or more b‐values should be acquired. |
doi_str_mv | 10.1002/mrm.28582 |
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fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_2461393117</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2473611109</sourcerecordid><originalsourceid>FETCH-LOGICAL-c3882-58c2be5f18f382d9547ca3fe401bc8692d12a17d99f950662fdaebf468bb31ac3</originalsourceid><addsrcrecordid>eNp10MFO3DAQBmCrApUt9NAXQJa4wCHgsZ3EPiLUlpVYISHgGjnJuBgl8dZOFuipj8Az8iQYlnKoxMljzadfo5-Qb8AOgTF-1If-kKtc8U9kBjnnGc-13CAzVkqWCdByi3yJ8ZYxpnUpP5MtITiDXOoZ-XU8UL8cXe_-YEvrp7-PK9NNSFsXx-DqaXR-oNYHmn54v_QDDqMzHXXDGMzK3-PL2PgbDGlBe__q9-fX88VBWtDxBmnnVhh2yKY1XcSvb-82ufrx_fLkNDs7_zk_OT7LGqEUz3LV8BpzC8oKxVudy7IxwqJkUDeq0LwFbqBstbY6Z0XBbWuwtrJQdS3ANGKb7K9zl8H_njCOVe9ig11nBvRTrLgsQGgBUCa69x-99VMY0nVJlaIAAKaTOlirJvgYA9pqGVxvwkMFrHppv0rtV6_tJ7v7ljjVPbbv8l_dCRytwZ3r8OHjpGpxsVhHPgOawo_y</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2473611109</pqid></control><display><type>article</type><title>An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver</title><source>Wiley-Blackwell Read & Publish Collection</source><creator>Riexinger, Andreas ; Martin, Jan ; Wetscherek, Andreas ; Kuder, Tristan Anselm ; Uder, Michael ; Hensel, Bernhard ; Laun, Frederik Bernd</creator><creatorcontrib>Riexinger, Andreas ; Martin, Jan ; Wetscherek, Andreas ; Kuder, Tristan Anselm ; Uder, Michael ; Hensel, Bernhard ; Laun, Frederik Bernd</creatorcontrib><description>Purpose
To find an optimized b‐value distribution for reproducible triexponential intravoxel incoherent motion (IVIM) exams in the liver.
Methods
A numeric optimization of b‐value distributions was performed using the triexponential IVIM equation and 27 different IVIM parameter sets. Starting with an initially optimized distribution of 6 b‐values, the number of b‐values was increased stepwise. Each new b‐value was chosen from a set of 64 predefined b‐values based on the computed summed relative mean error of the fitted triexponential IVIM parameters. This process was repeated for up to 100 b‐values. In simulations and in vivo measurements, optimized b‐value distributions were compared to 4 representative distributions found in literature.
Results
The first 16 optimized b‐values were 0, 0.3, 0.3, 70, 200, 800, 70, 1, 3.5, 5, 70, 1.2, 6, 45, 1.5, and 60 in units of s/mm2. Low b‐values were much more frequent than high b‐values. The optimized b‐value distribution resulted in a higher fit stability compared to distributions used in literature in both, simulation and in vivo measurements. Using more than 6 b‐values, ideally 16 or more, increased the fit stability considerably.
Conclusion
Using optimized b‐values, the fit uncertainty in triexponential IVIM can be largely reduced. Ideally, 16 or more b‐values should be acquired.</description><identifier>ISSN: 0740-3194</identifier><identifier>EISSN: 1522-2594</identifier><identifier>DOI: 10.1002/mrm.28582</identifier><identifier>PMID: 33201549</identifier><language>eng</language><publisher>United States: Wiley Subscription Services, Inc</publisher><subject>Algorithms ; Computer Simulation ; diffusion ; Diffusion Magnetic Resonance Imaging ; intravoxel incoherent motion ; Liver ; Liver - diagnostic imaging ; Motion ; MRI ; Numerical methods ; Optimization ; Process parameters ; Stability ; triexponential</subject><ispartof>Magnetic resonance in medicine, 2021-04, Vol.85 (4), p.2095-2108</ispartof><rights>2020 The Authors. published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine</rights><rights>2020 The Authors. Magnetic Resonance in Medicine published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine.</rights><rights>2020. 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-c3882-58c2be5f18f382d9547ca3fe401bc8692d12a17d99f950662fdaebf468bb31ac3</citedby><cites>FETCH-LOGICAL-c3882-58c2be5f18f382d9547ca3fe401bc8692d12a17d99f950662fdaebf468bb31ac3</cites><orcidid>0000-0002-9269-5609 ; 0000-0002-6346-3526</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27922,27923</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/33201549$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Riexinger, Andreas</creatorcontrib><creatorcontrib>Martin, Jan</creatorcontrib><creatorcontrib>Wetscherek, Andreas</creatorcontrib><creatorcontrib>Kuder, Tristan Anselm</creatorcontrib><creatorcontrib>Uder, Michael</creatorcontrib><creatorcontrib>Hensel, Bernhard</creatorcontrib><creatorcontrib>Laun, Frederik Bernd</creatorcontrib><title>An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver</title><title>Magnetic resonance in medicine</title><addtitle>Magn Reson Med</addtitle><description>Purpose
To find an optimized b‐value distribution for reproducible triexponential intravoxel incoherent motion (IVIM) exams in the liver.
Methods
A numeric optimization of b‐value distributions was performed using the triexponential IVIM equation and 27 different IVIM parameter sets. Starting with an initially optimized distribution of 6 b‐values, the number of b‐values was increased stepwise. Each new b‐value was chosen from a set of 64 predefined b‐values based on the computed summed relative mean error of the fitted triexponential IVIM parameters. This process was repeated for up to 100 b‐values. In simulations and in vivo measurements, optimized b‐value distributions were compared to 4 representative distributions found in literature.
Results
The first 16 optimized b‐values were 0, 0.3, 0.3, 70, 200, 800, 70, 1, 3.5, 5, 70, 1.2, 6, 45, 1.5, and 60 in units of s/mm2. Low b‐values were much more frequent than high b‐values. The optimized b‐value distribution resulted in a higher fit stability compared to distributions used in literature in both, simulation and in vivo measurements. Using more than 6 b‐values, ideally 16 or more, increased the fit stability considerably.
Conclusion
Using optimized b‐values, the fit uncertainty in triexponential IVIM can be largely reduced. Ideally, 16 or more b‐values should be acquired.</description><subject>Algorithms</subject><subject>Computer Simulation</subject><subject>diffusion</subject><subject>Diffusion Magnetic Resonance Imaging</subject><subject>intravoxel incoherent motion</subject><subject>Liver</subject><subject>Liver - diagnostic imaging</subject><subject>Motion</subject><subject>MRI</subject><subject>Numerical methods</subject><subject>Optimization</subject><subject>Process parameters</subject><subject>Stability</subject><subject>triexponential</subject><issn>0740-3194</issn><issn>1522-2594</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>24P</sourceid><recordid>eNp10MFO3DAQBmCrApUt9NAXQJa4wCHgsZ3EPiLUlpVYISHgGjnJuBgl8dZOFuipj8Az8iQYlnKoxMljzadfo5-Qb8AOgTF-1If-kKtc8U9kBjnnGc-13CAzVkqWCdByi3yJ8ZYxpnUpP5MtITiDXOoZ-XU8UL8cXe_-YEvrp7-PK9NNSFsXx-DqaXR-oNYHmn54v_QDDqMzHXXDGMzK3-PL2PgbDGlBe__q9-fX88VBWtDxBmnnVhh2yKY1XcSvb-82ufrx_fLkNDs7_zk_OT7LGqEUz3LV8BpzC8oKxVudy7IxwqJkUDeq0LwFbqBstbY6Z0XBbWuwtrJQdS3ANGKb7K9zl8H_njCOVe9ig11nBvRTrLgsQGgBUCa69x-99VMY0nVJlaIAAKaTOlirJvgYA9pqGVxvwkMFrHppv0rtV6_tJ7v7ljjVPbbv8l_dCRytwZ3r8OHjpGpxsVhHPgOawo_y</recordid><startdate>202104</startdate><enddate>202104</enddate><creator>Riexinger, Andreas</creator><creator>Martin, Jan</creator><creator>Wetscherek, Andreas</creator><creator>Kuder, Tristan Anselm</creator><creator>Uder, Michael</creator><creator>Hensel, Bernhard</creator><creator>Laun, Frederik Bernd</creator><general>Wiley Subscription Services, Inc</general><scope>24P</scope><scope>WIN</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><orcidid>https://orcid.org/0000-0002-9269-5609</orcidid><orcidid>https://orcid.org/0000-0002-6346-3526</orcidid></search><sort><creationdate>202104</creationdate><title>An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver</title><author>Riexinger, Andreas ; Martin, Jan ; Wetscherek, Andreas ; Kuder, Tristan Anselm ; Uder, Michael ; Hensel, Bernhard ; Laun, Frederik Bernd</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3882-58c2be5f18f382d9547ca3fe401bc8692d12a17d99f950662fdaebf468bb31ac3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Algorithms</topic><topic>Computer Simulation</topic><topic>diffusion</topic><topic>Diffusion Magnetic Resonance Imaging</topic><topic>intravoxel incoherent motion</topic><topic>Liver</topic><topic>Liver - diagnostic imaging</topic><topic>Motion</topic><topic>MRI</topic><topic>Numerical methods</topic><topic>Optimization</topic><topic>Process parameters</topic><topic>Stability</topic><topic>triexponential</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Riexinger, Andreas</creatorcontrib><creatorcontrib>Martin, Jan</creatorcontrib><creatorcontrib>Wetscherek, Andreas</creatorcontrib><creatorcontrib>Kuder, Tristan Anselm</creatorcontrib><creatorcontrib>Uder, Michael</creatorcontrib><creatorcontrib>Hensel, Bernhard</creatorcontrib><creatorcontrib>Laun, Frederik Bernd</creatorcontrib><collection>Open Access: Wiley-Blackwell Open Access Journals</collection><collection>Wiley Free Archive</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><jtitle>Magnetic resonance in medicine</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Riexinger, Andreas</au><au>Martin, Jan</au><au>Wetscherek, Andreas</au><au>Kuder, Tristan Anselm</au><au>Uder, Michael</au><au>Hensel, Bernhard</au><au>Laun, Frederik Bernd</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver</atitle><jtitle>Magnetic resonance in medicine</jtitle><addtitle>Magn Reson Med</addtitle><date>2021-04</date><risdate>2021</risdate><volume>85</volume><issue>4</issue><spage>2095</spage><epage>2108</epage><pages>2095-2108</pages><issn>0740-3194</issn><eissn>1522-2594</eissn><abstract>Purpose
To find an optimized b‐value distribution for reproducible triexponential intravoxel incoherent motion (IVIM) exams in the liver.
Methods
A numeric optimization of b‐value distributions was performed using the triexponential IVIM equation and 27 different IVIM parameter sets. Starting with an initially optimized distribution of 6 b‐values, the number of b‐values was increased stepwise. Each new b‐value was chosen from a set of 64 predefined b‐values based on the computed summed relative mean error of the fitted triexponential IVIM parameters. This process was repeated for up to 100 b‐values. In simulations and in vivo measurements, optimized b‐value distributions were compared to 4 representative distributions found in literature.
Results
The first 16 optimized b‐values were 0, 0.3, 0.3, 70, 200, 800, 70, 1, 3.5, 5, 70, 1.2, 6, 45, 1.5, and 60 in units of s/mm2. Low b‐values were much more frequent than high b‐values. The optimized b‐value distribution resulted in a higher fit stability compared to distributions used in literature in both, simulation and in vivo measurements. Using more than 6 b‐values, ideally 16 or more, increased the fit stability considerably.
Conclusion
Using optimized b‐values, the fit uncertainty in triexponential IVIM can be largely reduced. Ideally, 16 or more b‐values should be acquired.</abstract><cop>United States</cop><pub>Wiley Subscription Services, Inc</pub><pmid>33201549</pmid><doi>10.1002/mrm.28582</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0002-9269-5609</orcidid><orcidid>https://orcid.org/0000-0002-6346-3526</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Algorithms Computer Simulation diffusion Diffusion Magnetic Resonance Imaging intravoxel incoherent motion Liver Liver - diagnostic imaging Motion MRI Numerical methods Optimization Process parameters Stability triexponential |
title | An optimized b‐value distribution for triexponential intravoxel incoherent motion (IVIM) in the liver |
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