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dc.contributor.authorFühres, T
dc.contributor.authorRiexinger, AJ
dc.contributor.authorLoh, M
dc.contributor.authorMartin, J
dc.contributor.authorWetscherek, A
dc.contributor.authorKuder, TA
dc.contributor.authorUder, M
dc.contributor.authorHensel, B
dc.contributor.authorLaun, FB
dc.date.accessioned2021-11-25T13:20:15Z
dc.date.available2021-11-25T13:20:15Z
dc.date.issued2021-08-28
dc.identifier.citationMagnetic resonance in medicine, 2021
dc.identifier.issn0740-3194
dc.identifier.urihttps://repository.icr.ac.uk/handle/internal/4898
dc.identifier.eissn1522-2594
dc.identifier.doi10.1002/mrm.28996
dc.description.abstractPURPOSE: Intravoxel incoherent motion (IVIM) studies are performed with different acquisition protocols. Comparing them requires knowledge of echo time (TE) dependencies. The TE-dependence of the biexponential perfusion fraction f is well-documented, unlike that of its triexponential counterparts f1 and f2 and the biexponential and triexponential pseudodiffusion coefficients D* , D1∗ , and D2∗ . The purpose was to investigate the TE-dependence of these parameters and to check whether the triexponential pseudodiffusion compartments are associated with arterial and venous blood. METHODS: Fifteen healthy volunteers (19-58 y; mean: 24.7 y) underwent diffusion-weighted imaging of the abdomen with 24 b-values (0.2-800 s/mm2 ) at TEs of 45, 60, 75, and 90 ms. Regions of interest (ROIs) were manually drawn in the liver. One set of bi- and triexponential IVIM parameters per volunteer and TE was determined. The TE-dependence was assessed with the Kruskal-Wallis test. RESULTS: TE-dependence was observed for f (P < .001), f1 (P = .001), and f2 (P < .001). Their median values at the four measured TEs were: f: 0.198/0.240/0.274/0.359, f1 : 0.113/0.139/0.146/0.205, f2 : 0.115/0.155/0.182/0.194. D, D* , D1∗ , and D2∗ showed no significant TE-dependence. Their values were: diffusion coefficient D (10-4 mm2 /s): 9.45/9.63/9.75/9.41, biexponential D* (10-2 mm2 /s): 5.26/5.52/6.13/5.82, triexponential D1∗ (10-2 mm2 /s): 1.73/2.91/2.25/2.51, triexponential D2∗ (mm2 /s): 0.478/1.385/0.616/0.846. CONCLUSION: f1 and f2 show similar TE-dependence as f, ie, increase with rising TE; an effect that must be accounted for when comparing different studies. The diffusion and pseudodiffusion coefficients might be compared without TE correction. Because of the similar TE-dependence of f1 and f2 , the triexponential pseudodiffusion compartments are most probably not associated to venous and arterial blood.
dc.formatPrint-Electronic
dc.languageeng
dc.language.isoeng
dc.publisherWILEY
dc.rights.urihttps://creativecommons.org/licenses/by/4.0
dc.titleEcho time dependence of biexponential and triexponential intravoxel incoherent motion parameters in the liver.
dc.typeJournal Article
dcterms.dateAccepted2021-08-12
rioxxterms.versionVoR
rioxxterms.versionofrecord10.1002/mrm.28996
rioxxterms.licenseref.urihttps://creativecommons.org/licenses/by/4.0
rioxxterms.licenseref.startdate2021-08-28
rioxxterms.typeJournal Article/Review
dc.relation.isPartOfMagnetic resonance in medicine
pubs.notesNot known
pubs.organisational-group/ICR
pubs.organisational-group/ICR/Primary Group
pubs.organisational-group/ICR/Primary Group/ICR Divisions
pubs.organisational-group/ICR/Primary Group/ICR Divisions/Radiotherapy and Imaging
pubs.organisational-group/ICR/Primary Group/ICR Divisions/Radiotherapy and Imaging/Radiotherapy Physics Modelling
pubs.publication-statusPublished
pubs.embargo.termsNot known
icr.researchteamRadiotherapy Physics Modelling
dc.contributor.icrauthorWetscherek, Andreas


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