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Imaging Sequences for Hyperpolarized Solids

Hyperpolarization is one of the approaches to enhance Nuclear Magnetic Resonance (NMR) and Magnetic Resonance Imaging (MRI) signal by increasing the population difference between the nuclear spin states. Imaging hyperpolarized solids opens up extensive possibilities, yet is challenging to perform. T...

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Autores principales: Lv, Xudong, Walton, Jeffrey, Druga, Emanuel, Nazaryan, Raffi, Mao, Haiyan, Pines, Alexander, Ajoy, Ashok, Reimer, Jeffrey
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7795150/
https://www.ncbi.nlm.nih.gov/pubmed/33396762
http://dx.doi.org/10.3390/molecules26010133
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author Lv, Xudong
Walton, Jeffrey
Druga, Emanuel
Nazaryan, Raffi
Mao, Haiyan
Pines, Alexander
Ajoy, Ashok
Reimer, Jeffrey
author_facet Lv, Xudong
Walton, Jeffrey
Druga, Emanuel
Nazaryan, Raffi
Mao, Haiyan
Pines, Alexander
Ajoy, Ashok
Reimer, Jeffrey
author_sort Lv, Xudong
collection PubMed
description Hyperpolarization is one of the approaches to enhance Nuclear Magnetic Resonance (NMR) and Magnetic Resonance Imaging (MRI) signal by increasing the population difference between the nuclear spin states. Imaging hyperpolarized solids opens up extensive possibilities, yet is challenging to perform. The highly populated state is normally not replenishable to the initial polarization level by spin-lattice relaxation, which regular MRI sequences rely on. This makes it necessary to carefully “budget” the polarization to optimize the image quality. In this paper, we present a theoretical framework to address such challenge under the assumption of either variable flip angles or a constant flip angle. In addition, we analyze the gradient arrangement to perform fast imaging to overcome intrinsic short decoherence in solids. Hyperpolarized diamonds imaging is demonstrated as a prototypical platform to test the theory.
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spelling pubmed-77951502021-01-10 Imaging Sequences for Hyperpolarized Solids Lv, Xudong Walton, Jeffrey Druga, Emanuel Nazaryan, Raffi Mao, Haiyan Pines, Alexander Ajoy, Ashok Reimer, Jeffrey Molecules Article Hyperpolarization is one of the approaches to enhance Nuclear Magnetic Resonance (NMR) and Magnetic Resonance Imaging (MRI) signal by increasing the population difference between the nuclear spin states. Imaging hyperpolarized solids opens up extensive possibilities, yet is challenging to perform. The highly populated state is normally not replenishable to the initial polarization level by spin-lattice relaxation, which regular MRI sequences rely on. This makes it necessary to carefully “budget” the polarization to optimize the image quality. In this paper, we present a theoretical framework to address such challenge under the assumption of either variable flip angles or a constant flip angle. In addition, we analyze the gradient arrangement to perform fast imaging to overcome intrinsic short decoherence in solids. Hyperpolarized diamonds imaging is demonstrated as a prototypical platform to test the theory. MDPI 2020-12-30 /pmc/articles/PMC7795150/ /pubmed/33396762 http://dx.doi.org/10.3390/molecules26010133 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Lv, Xudong
Walton, Jeffrey
Druga, Emanuel
Nazaryan, Raffi
Mao, Haiyan
Pines, Alexander
Ajoy, Ashok
Reimer, Jeffrey
Imaging Sequences for Hyperpolarized Solids
title Imaging Sequences for Hyperpolarized Solids
title_full Imaging Sequences for Hyperpolarized Solids
title_fullStr Imaging Sequences for Hyperpolarized Solids
title_full_unstemmed Imaging Sequences for Hyperpolarized Solids
title_short Imaging Sequences for Hyperpolarized Solids
title_sort imaging sequences for hyperpolarized solids
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7795150/
https://www.ncbi.nlm.nih.gov/pubmed/33396762
http://dx.doi.org/10.3390/molecules26010133
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