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3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
(31)P MR spectroscopic imaging (MRSI) is a versatile technique to study phospholipid precursors and energy metabolism in the healthy and diseased human brain. However, mainly due to its low sensitivity, (31)P MRSI is currently limited to research purposes. To obtain 3D (31)P MRSI spectra with improv...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8244063/ https://www.ncbi.nlm.nih.gov/pubmed/31518036 http://dx.doi.org/10.1002/nbm.4169 |
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author | Peeters, Tom H. van Uden, Mark J. Rijpma, Anne Scheenen, Tom W.J. Heerschap, Arend |
author_facet | Peeters, Tom H. van Uden, Mark J. Rijpma, Anne Scheenen, Tom W.J. Heerschap, Arend |
author_sort | Peeters, Tom H. |
collection | PubMed |
description | (31)P MR spectroscopic imaging (MRSI) is a versatile technique to study phospholipid precursors and energy metabolism in the healthy and diseased human brain. However, mainly due to its low sensitivity, (31)P MRSI is currently limited to research purposes. To obtain 3D (31)P MRSI spectra with improved signal‐to‐noise ratio on clinical 3 T MR systems, we used a coil combination consisting of a dual‐tuned birdcage transmit coil and a (31)P eight‐channel phased‐array receive insert. To further increase resolution and sensitivity we applied WALTZ4 (1)H decoupling and continuous wave nuclear Overhauser effect (NOE) enhancement and acquired high‐quality MRSI spectra with nominal voxel volumes of ~ 17.6 cm(3) (effective voxel volume ~ 51 cm(3)) in a clinically relevant measurement time of ~ 13 minutes, without exceeding SAR limits. Steady‐state NOE enhancements ranged from 15 ± 9% (γ‐ATP) and 33 ± 3% (phosphocreatine) to 48 ± 11% (phosphoethanolamine). Because of these improvements, we resolved and detected all (31)P signals of metabolites that have also been reported for ultrahigh field strengths, including resonances for NAD(+), NADH and extracellular inorganic phosphate. T(1) times of extracellular inorganic phosphate were longer than for intracellular inorganic phosphate (3.8 ± 1.4s vs 1.8 ± 0.65 seconds). A comparison of measured T(1) relaxation times and NOE enhancements at 3 T with published values between 1.5 and 9.4 T indicates that T(1) relaxation of (31)P metabolite spins in the human brain is dominated by dipolar relaxation for this field strength range. Even although intrinsic sensitivity is higher at ultrahigh fields, we demonstrate that at a clinical field strength of 3 T, similar (31)P MRSI information content can be obtained using a sophisticated coil design combined with (1)H decoupling and NOE enhancement. |
format | Online Article Text |
id | pubmed-8244063 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-82440632021-07-02 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+) Peeters, Tom H. van Uden, Mark J. Rijpma, Anne Scheenen, Tom W.J. Heerschap, Arend NMR Biomed Special Issue Research Articles (31)P MR spectroscopic imaging (MRSI) is a versatile technique to study phospholipid precursors and energy metabolism in the healthy and diseased human brain. However, mainly due to its low sensitivity, (31)P MRSI is currently limited to research purposes. To obtain 3D (31)P MRSI spectra with improved signal‐to‐noise ratio on clinical 3 T MR systems, we used a coil combination consisting of a dual‐tuned birdcage transmit coil and a (31)P eight‐channel phased‐array receive insert. To further increase resolution and sensitivity we applied WALTZ4 (1)H decoupling and continuous wave nuclear Overhauser effect (NOE) enhancement and acquired high‐quality MRSI spectra with nominal voxel volumes of ~ 17.6 cm(3) (effective voxel volume ~ 51 cm(3)) in a clinically relevant measurement time of ~ 13 minutes, without exceeding SAR limits. Steady‐state NOE enhancements ranged from 15 ± 9% (γ‐ATP) and 33 ± 3% (phosphocreatine) to 48 ± 11% (phosphoethanolamine). Because of these improvements, we resolved and detected all (31)P signals of metabolites that have also been reported for ultrahigh field strengths, including resonances for NAD(+), NADH and extracellular inorganic phosphate. T(1) times of extracellular inorganic phosphate were longer than for intracellular inorganic phosphate (3.8 ± 1.4s vs 1.8 ± 0.65 seconds). A comparison of measured T(1) relaxation times and NOE enhancements at 3 T with published values between 1.5 and 9.4 T indicates that T(1) relaxation of (31)P metabolite spins in the human brain is dominated by dipolar relaxation for this field strength range. Even although intrinsic sensitivity is higher at ultrahigh fields, we demonstrate that at a clinical field strength of 3 T, similar (31)P MRSI information content can be obtained using a sophisticated coil design combined with (1)H decoupling and NOE enhancement. John Wiley and Sons Inc. 2019-09-13 2021-05 /pmc/articles/PMC8244063/ /pubmed/31518036 http://dx.doi.org/10.1002/nbm.4169 Text en © 2019 The Authors. NMR in Biomedicine published by John Wiley & Sons Ltd https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ (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 | Special Issue Research Articles Peeters, Tom H. van Uden, Mark J. Rijpma, Anne Scheenen, Tom W.J. Heerschap, Arend 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+) |
title | 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
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title_full | 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
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title_fullStr | 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
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title_full_unstemmed | 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
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title_short | 3D (31)P MR spectroscopic imaging of the human brain at 3 T with a (31)P receive array: An assessment of (1)H decoupling, T(1) relaxation times, (1)H‐(31)P nuclear Overhauser effects and NAD(+)
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title_sort | 3d (31)p mr spectroscopic imaging of the human brain at 3 t with a (31)p receive array: an assessment of (1)h decoupling, t(1) relaxation times, (1)h‐(31)p nuclear overhauser effects and nad(+) |
topic | Special Issue Research Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8244063/ https://www.ncbi.nlm.nih.gov/pubmed/31518036 http://dx.doi.org/10.1002/nbm.4169 |
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