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Principles and limitations of NMR diffusion measurements

Diffusion spectroscopy, imaging and particularly diffusion tensor imaging have become popular thanks to their numerous clinical and research applications which span from brain stroke evaluation to fiber tracking. With a few exceptions, these methods are rooted in the classic Stejskal-Tanner formula...

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Detalles Bibliográficos
Autores principales: Hrabe, Jan, Kaur, Gurjinder, Guilfoyle, David N.
Formato: Texto
Lenguaje:English
Publicado: Medknow Publications 2007
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3003887/
https://www.ncbi.nlm.nih.gov/pubmed/21217917
http://dx.doi.org/10.4103/0971-6203.31148
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author Hrabe, Jan
Kaur, Gurjinder
Guilfoyle, David N.
author_facet Hrabe, Jan
Kaur, Gurjinder
Guilfoyle, David N.
author_sort Hrabe, Jan
collection PubMed
description Diffusion spectroscopy, imaging and particularly diffusion tensor imaging have become popular thanks to their numerous clinical and research applications which span from brain stroke evaluation to fiber tracking. With a few exceptions, these methods are rooted in the classic Stejskal-Tanner formula for the diffusion-attenuated signal, usually obtained by solving the Bloch-Torrey partial differential equations. Here we derive the Stejskal-Tanner formula in the simplest possible manner, avoiding integrals and differential equations. This approach makes it easy to understand the origin of the diffusion signal attenuation, the effects of various diffusion sequence parameters, and also the numerous important pitfalls, which are discussed in the last section.
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spelling pubmed-30038872011-01-07 Principles and limitations of NMR diffusion measurements Hrabe, Jan Kaur, Gurjinder Guilfoyle, David N. J Med Phys Original Article Diffusion spectroscopy, imaging and particularly diffusion tensor imaging have become popular thanks to their numerous clinical and research applications which span from brain stroke evaluation to fiber tracking. With a few exceptions, these methods are rooted in the classic Stejskal-Tanner formula for the diffusion-attenuated signal, usually obtained by solving the Bloch-Torrey partial differential equations. Here we derive the Stejskal-Tanner formula in the simplest possible manner, avoiding integrals and differential equations. This approach makes it easy to understand the origin of the diffusion signal attenuation, the effects of various diffusion sequence parameters, and also the numerous important pitfalls, which are discussed in the last section. Medknow Publications 2007 /pmc/articles/PMC3003887/ /pubmed/21217917 http://dx.doi.org/10.4103/0971-6203.31148 Text en © Journal of Medical Physics http://creativecommons.org/licenses/by/2.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Original Article
Hrabe, Jan
Kaur, Gurjinder
Guilfoyle, David N.
Principles and limitations of NMR diffusion measurements
title Principles and limitations of NMR diffusion measurements
title_full Principles and limitations of NMR diffusion measurements
title_fullStr Principles and limitations of NMR diffusion measurements
title_full_unstemmed Principles and limitations of NMR diffusion measurements
title_short Principles and limitations of NMR diffusion measurements
title_sort principles and limitations of nmr diffusion measurements
topic Original Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3003887/
https://www.ncbi.nlm.nih.gov/pubmed/21217917
http://dx.doi.org/10.4103/0971-6203.31148
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