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Unbalanced SSFP for super-resolution in MRI

PURPOSE: To achieve rapid, low specific absorption rate (SAR) super-resolution imaging by exploiting the characteristic magnetization off-resonance profile in SSFP. THEORY AND METHODS: In the presented technique, low flip angle unbalanced SSFP imaging is used to acquire a series of images at a low n...

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Autores principales: Lally, Peter J., Matthews, Paul M., Bangerter, Neal K.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8972796/
https://www.ncbi.nlm.nih.gov/pubmed/33201538
http://dx.doi.org/10.1002/mrm.28593
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author Lally, Peter J.
Matthews, Paul M.
Bangerter, Neal K.
author_facet Lally, Peter J.
Matthews, Paul M.
Bangerter, Neal K.
author_sort Lally, Peter J.
collection PubMed
description PURPOSE: To achieve rapid, low specific absorption rate (SAR) super-resolution imaging by exploiting the characteristic magnetization off-resonance profile in SSFP. THEORY AND METHODS: In the presented technique, low flip angle unbalanced SSFP imaging is used to acquire a series of images at a low nominal resolution that are then combined in a super-resolution strategy analogous to non-linear structured illumination microscopy. This is demonstrated in principle via Bloch simulations and synthetic phantoms, and the performance is quantified in terms of point-spread function (PSF) and SNR for gray and white matter from field strengths of 0.35T to 9.4T. A k-space reconstruction approach is proposed to account for B(0) effects. This was applied to reconstruct super-resolution images from a test object at 9.4T. RESULTS: Artifact-free super-resolution images were produced after incorporating sufficient preparation time for the magnetization to approach the steady state. High-resolution images of a test object were obtained at 9.4T, in the presence of considerable B(0) inhomogeneity. For gray matter, the highest achievable resolution ranges from 3% of the acquired voxel dimension at 0.35T, to 9% at 9.4T. For white matter, this corresponds to 3% and 10%, respectively. Compared to an equivalent segmented gradient echo acquisition at the optimal flip angle, with a fixed TR of 8 ms, gray matter has up to 34% of the SNR at 9.4T while using a ×10 smaller flip angle. For white matter, this corresponds to 29% with a ×11 smaller flip angle. CONCLUSION: This approach achieves high degrees of super-resolution enhancement with minimal RF power requirements.
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spelling pubmed-89727962022-04-01 Unbalanced SSFP for super-resolution in MRI Lally, Peter J. Matthews, Paul M. Bangerter, Neal K. Magn Reson Med Article PURPOSE: To achieve rapid, low specific absorption rate (SAR) super-resolution imaging by exploiting the characteristic magnetization off-resonance profile in SSFP. THEORY AND METHODS: In the presented technique, low flip angle unbalanced SSFP imaging is used to acquire a series of images at a low nominal resolution that are then combined in a super-resolution strategy analogous to non-linear structured illumination microscopy. This is demonstrated in principle via Bloch simulations and synthetic phantoms, and the performance is quantified in terms of point-spread function (PSF) and SNR for gray and white matter from field strengths of 0.35T to 9.4T. A k-space reconstruction approach is proposed to account for B(0) effects. This was applied to reconstruct super-resolution images from a test object at 9.4T. RESULTS: Artifact-free super-resolution images were produced after incorporating sufficient preparation time for the magnetization to approach the steady state. High-resolution images of a test object were obtained at 9.4T, in the presence of considerable B(0) inhomogeneity. For gray matter, the highest achievable resolution ranges from 3% of the acquired voxel dimension at 0.35T, to 9% at 9.4T. For white matter, this corresponds to 3% and 10%, respectively. Compared to an equivalent segmented gradient echo acquisition at the optimal flip angle, with a fixed TR of 8 ms, gray matter has up to 34% of the SNR at 9.4T while using a ×10 smaller flip angle. For white matter, this corresponds to 29% with a ×11 smaller flip angle. CONCLUSION: This approach achieves high degrees of super-resolution enhancement with minimal RF power requirements. 2021-05 2020-11-17 /pmc/articles/PMC8972796/ /pubmed/33201538 http://dx.doi.org/10.1002/mrm.28593 Text en https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the Creative Commons Attribution (https://creativecommons.org/licenses/by/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Article
Lally, Peter J.
Matthews, Paul M.
Bangerter, Neal K.
Unbalanced SSFP for super-resolution in MRI
title Unbalanced SSFP for super-resolution in MRI
title_full Unbalanced SSFP for super-resolution in MRI
title_fullStr Unbalanced SSFP for super-resolution in MRI
title_full_unstemmed Unbalanced SSFP for super-resolution in MRI
title_short Unbalanced SSFP for super-resolution in MRI
title_sort unbalanced ssfp for super-resolution in mri
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8972796/
https://www.ncbi.nlm.nih.gov/pubmed/33201538
http://dx.doi.org/10.1002/mrm.28593
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