Multiple interleaved mode saturation (MIMOSA) for B


Journal

Magnetic resonance in medicine
ISSN: 1522-2594
Titre abrégé: Magn Reson Med
Pays: United States
ID NLM: 8505245

Informations de publication

Date de publication:
08 2019
Historique:
received: 23 12 2018
revised: 25 02 2019
accepted: 13 03 2019
pubmed: 20 4 2019
medline: 12 5 2020
entrez: 20 4 2019
Statut: ppublish

Résumé

To mitigate Multiple interleaved mode saturation employs interleaving of 2 complementary phase sets during the saturation pulse train. Phase differences of 45° (first mode) and 90° (second mode) between 2 adjacent transmitter coil channels are used. The influence of the new saturation scheme on the CEST contrast was analyzed using Bloch-McConnell simulations. The presented method was verified in phantom and in vivo measurements of the healthy human brain. The relayed nuclear Overhauser effect was evaluated, and the inverse magnetic transfer ratio metric was calculated. Results were compared to a published Simulations showed that the inverse magnetic transfer ratio metric contrast of relayed nuclear Overhauser effect shows a smaller dependency on the relative amplitudes of the 2 different modes than the contrasts of Cr and amide proton transfer. Measurements of an egg white phantom showed markedly improved homogeneity compared to the uncorrected inverse magnetic transfer ratio metric (relayed nuclear Overhauser effect) images and slightly improved results compared to Multiple interleaved mode saturation can be used as a simple method to mitigate

Identifiants

pubmed: 31002432
doi: 10.1002/mrm.27762
doi:

Substances chimiques

Amides 0
Protons 0

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

693-705

Informations de copyright

© 2019 International Society for Magnetic Resonance in Medicine.

Auteurs

Andrzej Liebert (A)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Moritz Zaiss (M)

High-Field Magnetic Resonance Center, Max Planck Institute for Biological Cybernetics, Tuebingen, Germany.

Rene Gumbrecht (R)

Siemens Healthcare GmbH, Erlangen, Germany.

Katharina Tkotz (K)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Peter Linz (P)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Benjamin Schmitt (B)

Siemens Healthcare GmbH, Erlangen, Germany.

Frederik B Laun (FB)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Arnd Doerfler (A)

Department of Neuroradiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Michael Uder (M)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.

Armin M Nagel (AM)

Institute of Radiology, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.
Institute of Medical Physics, University Hospital Erlangen, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany.
Division of Medical Physics in Radiology, German Cancer Research Centre (DKFZ), Heidelberg, Germany.

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