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Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping

[Image: see text] We describe temperature-ramped spin-exchange optical pumping (TR-SEOP) in an automated high-throughput batch-mode (129)Xe hyperpolarizer utilizing three key temperature regimes: (i) “hot”—where the (129)Xe hyperpolarization rate is maximal, (ii) “warm”—where the (129)Xe hyperpolari...

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Autores principales: Nikolaou, Panayiotis, Coffey, Aaron M., Barlow, Michael J., Rosen, Matthew S., Goodson, Boyd M., Chekmenev, Eduard Y.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2014
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4139178/
https://www.ncbi.nlm.nih.gov/pubmed/25008290
http://dx.doi.org/10.1021/ac501537w
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author Nikolaou, Panayiotis
Coffey, Aaron M.
Barlow, Michael J.
Rosen, Matthew S.
Goodson, Boyd M.
Chekmenev, Eduard Y.
author_facet Nikolaou, Panayiotis
Coffey, Aaron M.
Barlow, Michael J.
Rosen, Matthew S.
Goodson, Boyd M.
Chekmenev, Eduard Y.
author_sort Nikolaou, Panayiotis
collection PubMed
description [Image: see text] We describe temperature-ramped spin-exchange optical pumping (TR-SEOP) in an automated high-throughput batch-mode (129)Xe hyperpolarizer utilizing three key temperature regimes: (i) “hot”—where the (129)Xe hyperpolarization rate is maximal, (ii) “warm”—where the (129)Xe hyperpolarization approaches unity, and (iii) “cool”—where hyperpolarized (129)Xe gas is transferred into a Tedlar bag with low Rb content (<5 ng per ∼1 L dose) suitable for human imaging applications. Unlike with the conventional approach of batch-mode SEOP, here all three temperature regimes may be operated under continuous high-power (170 W) laser irradiation, and hyperpolarized (129)Xe gas is delivered without the need for a cryocollection step. The variable-temperature approach increased the SEOP rate by more than 2-fold compared to the constant-temperature polarization rate (e.g., giving effective values for the exponential buildup constant γ(SEOP) of 62.5 ± 3.7 × 10(–3) min(–1) vs 29.9 ± 1.2 × 10(–3) min(–1)) while achieving nearly the same maximum %P(Xe) value (88.0 ± 0.8% vs 90.1% ± 0.8%, for a 500 Torr (67 kPa) Xe cell loading—corresponding to nuclear magnetic resonance/magnetic resonance imaging (NMR/MRI) enhancements of ∼3.1 × 10(5) and ∼2.32 × 10(8) at the relevant fields for clinical imaging and HP (129)Xe production of 3 T and 4 mT, respectively); moreover, the intercycle “dead” time was also significantly decreased. The higher-throughput TR-SEOP approach can be implemented without sacrificing the level of (129)Xe hyperpolarization or the experimental stability for automation—making this approach beneficial for improving the overall (129)Xe production rate in clinical settings.
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spelling pubmed-41391782015-07-10 Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping Nikolaou, Panayiotis Coffey, Aaron M. Barlow, Michael J. Rosen, Matthew S. Goodson, Boyd M. Chekmenev, Eduard Y. Anal Chem [Image: see text] We describe temperature-ramped spin-exchange optical pumping (TR-SEOP) in an automated high-throughput batch-mode (129)Xe hyperpolarizer utilizing three key temperature regimes: (i) “hot”—where the (129)Xe hyperpolarization rate is maximal, (ii) “warm”—where the (129)Xe hyperpolarization approaches unity, and (iii) “cool”—where hyperpolarized (129)Xe gas is transferred into a Tedlar bag with low Rb content (<5 ng per ∼1 L dose) suitable for human imaging applications. Unlike with the conventional approach of batch-mode SEOP, here all three temperature regimes may be operated under continuous high-power (170 W) laser irradiation, and hyperpolarized (129)Xe gas is delivered without the need for a cryocollection step. The variable-temperature approach increased the SEOP rate by more than 2-fold compared to the constant-temperature polarization rate (e.g., giving effective values for the exponential buildup constant γ(SEOP) of 62.5 ± 3.7 × 10(–3) min(–1) vs 29.9 ± 1.2 × 10(–3) min(–1)) while achieving nearly the same maximum %P(Xe) value (88.0 ± 0.8% vs 90.1% ± 0.8%, for a 500 Torr (67 kPa) Xe cell loading—corresponding to nuclear magnetic resonance/magnetic resonance imaging (NMR/MRI) enhancements of ∼3.1 × 10(5) and ∼2.32 × 10(8) at the relevant fields for clinical imaging and HP (129)Xe production of 3 T and 4 mT, respectively); moreover, the intercycle “dead” time was also significantly decreased. The higher-throughput TR-SEOP approach can be implemented without sacrificing the level of (129)Xe hyperpolarization or the experimental stability for automation—making this approach beneficial for improving the overall (129)Xe production rate in clinical settings. American Chemical Society 2014-07-10 2014-08-19 /pmc/articles/PMC4139178/ /pubmed/25008290 http://dx.doi.org/10.1021/ac501537w Text en Copyright © 2014 American Chemical Society Terms of Use (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html)
spellingShingle Nikolaou, Panayiotis
Coffey, Aaron M.
Barlow, Michael J.
Rosen, Matthew S.
Goodson, Boyd M.
Chekmenev, Eduard Y.
Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title_full Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title_fullStr Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title_full_unstemmed Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title_short Temperature-Ramped (129)Xe Spin-Exchange Optical Pumping
title_sort temperature-ramped (129)xe spin-exchange optical pumping
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4139178/
https://www.ncbi.nlm.nih.gov/pubmed/25008290
http://dx.doi.org/10.1021/ac501537w
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