Literature DB >> 33070086

A semi-empirical model to optimize continuous-flow hyperpolarized 129Xe production under practical cryogenic-accumulation conditions.

Joseph W Plummer1, Kiarash Emami2, Andrew Dummer2, Jason C Woods3, Laura L Walkup4, Zackary I Cleveland5.   

Abstract

Continuous-flow spin exchange optical pumping (SEOP) with cryogenic accumulation is a powerful technique to generate multiple, large volumes of hyperpolarized (HP) 129Xe in rapid succession. It enables a range of studies, from dark matter tracking to preclinical and clinical MRI. Multiple analytical models based on first principles atomic physics and device-specific design features have been proposed for individual processes within HP 129Xe production. However, the modeling efforts have not yet integrated all the steps involved in practical, large volume HP 129Xe production process (e.g., alkali vapor generation, continuous-flow SEOP, and cryogenic accumulation). Here, we use a simplified analytical model that couples both SEOP and cryogenic accumulation, incorporating only two system-specific empirical parameters: the longitudinal relaxation time of the polycrystalline 129Xe "snow', T1snow, generated during cryogenic accumulation, and 2) the average Rb density during active, continuous-flow polarization. By fitting the model to polarization data collected from >140 L of 129Xe polarized across a range of flow and volume conditions, the estimates for Rb density and T1snow were 1.6 ± 0.1 × 1013 cm-3 and 84 ± 5 min, respectively - each notably less than expected based on previous literature. Together, these findings indicate that 1) earlier polarization predictions were hindered by miscalculated Rb densities, and 2) polarization is not optimized by maximizing SEOP efficiency with a low concentration 129Xe, but rather by using richer 129Xe-buffer gas blends that enable faster accumulation. Accordingly, modeling and experimentation revealed the optimal fraction of 129Xe, f, in the 129Xe-buffer gas blend was ~2%. Further, if coupled with modest increases in laser power, the model predicts liter volumes of HP 129Xe with polarizations exceeding 60% could be generated routinely in only tens of minutes.
Copyright © 2020 Elsevier Inc. All rights reserved.

Entities:  

Keywords:  (129)Xe-buffer gas blend; Continuous-flow spin-exchange optical pumping; Hyperpolarized(129)Xe; Laser power; Parameter optimization; Polarization model; Rb density; Solid T(1) relaxation

Year:  2020        PMID: 33070086      PMCID: PMC7655637          DOI: 10.1016/j.jmr.2020.106845

Source DB:  PubMed          Journal:  J Magn Reson        ISSN: 1090-7807            Impact factor:   2.229


  31 in total

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Authors:  B Chann; I A Nelson; L W Anderson; B Driehuys; T G Walker
Journal:  Phys Rev Lett       Date:  2002-02-28       Impact factor: 9.161

2.  Hybrid spin-exchange optical pumping of 3He.

Authors:  Earl Babcock; Ian Nelson; Steve Kadlecek; Bastiaan Driehuys; L W Anderson; F W Hersman; Thad G Walker
Journal:  Phys Rev Lett       Date:  2003-09-16       Impact factor: 9.161

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Journal:  Phys Rev Lett       Date:  1993-02-01       Impact factor: 9.161

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Journal:  Phys Rev Lett       Date:  2004-10-11       Impact factor: 9.161

5.  Optical pumping of Rb in the presence of high-pressure 3He buffer gas.

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Journal:  Phys Rev A       Date:  1991-09-01       Impact factor: 3.140

6.  Feasibility, tolerability and safety of pediatric hyperpolarized 129Xe magnetic resonance imaging in healthy volunteers and children with cystic fibrosis.

Authors:  Laura L Walkup; Robert P Thomen; Teckla G Akinyi; Erin Watters; Kai Ruppert; John P Clancy; Jason C Woods; Zackary I Cleveland
Journal:  Pediatr Radiol       Date:  2016-08-05

7.  Preparation of biogenic gas vesicle nanostructures for use as contrast agents for ultrasound and MRI.

Authors:  Anupama Lakshmanan; George J Lu; Arash Farhadi; Suchita P Nety; Martin Kunth; Audrey Lee-Gosselin; David Maresca; Raymond W Bourdeau; Melissa Yin; Judy Yan; Christopher Witte; Dina Malounda; F Stuart Foster; Leif Schröder; Mikhail G Shapiro
Journal:  Nat Protoc       Date:  2017-09-07       Impact factor: 13.491

8.  An Expanded Palette of Xenon-129 NMR Biosensors.

Authors:  Yanfei Wang; Ivan J Dmochowski
Journal:  Acc Chem Res       Date:  2016-09-19       Impact factor: 22.384

9.  ^{129}Xe-Rb Spin-Exchange Optical Pumping with High Photon Efficiency.

Authors:  G Norquay; G J Collier; M Rao; N J Stewart; J M Wild
Journal:  Phys Rev Lett       Date:  2018-10-12       Impact factor: 9.161

Review 10.  Probing Reversible Guest Binding with Hyperpolarized 129Xe-NMR: Characteristics and Applications for Cucurbit[n]urils.

Authors:  Jabadurai Jayapaul; Leif Schröder
Journal:  Molecules       Date:  2020-02-20       Impact factor: 4.411

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  3 in total

1.  Improving hyperpolarized 129 Xe ADC mapping in pediatric and adult lungs with uncertainty propagation.

Authors:  Abdullah S Bdaiwi; Peter J Niedbalski; Md M Hossain; Matthew M Willmering; Laura L Walkup; Hui Wang; Robert P Thomen; Kai Ruppert; Jason C Woods; Zackary I Cleveland
Journal:  NMR Biomed       Date:  2021-11-02       Impact factor: 4.044

Review 2.  Enabling Clinical Technologies for Hyperpolarized 129 Xenon Magnetic Resonance Imaging and Spectroscopy.

Authors:  Alixander S Khan; Rebecca L Harvey; Jonathan R Birchall; Robert K Irwin; Panayiotis Nikolaou; Geoffry Schrank; Kiarash Emami; Andrew Dummer; Michael J Barlow; Boyd M Goodson; Eduard Y Chekmenev
Journal:  Angew Chem Int Ed Engl       Date:  2021-06-09       Impact factor: 16.823

Review 3.  [Noninvasive functional lung imaging with hyperpolarized xenon : Breakthrough for diagnostics?]

Authors:  Mariia Anikeeva; Maitreyi Sangal; Oliver Speck; Graham Norquay; Maaz Zuhayra; Ulf Lützen; Josh Peters; Olav Jansen; Jan-Bernd Hövener
Journal:  Radiologie (Heidelb)       Date:  2022-04-11
  3 in total

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