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Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()

As an alternative to cryogenic gas handling, hyperpolarized (hp) gas mixtures were extracted directly from the spin exchange optical pumping (SEOP) process through expansion followed by compression to ambient pressure for biomedical MRI applications. The omission of cryogenic gas separation generall...

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Detalles Bibliográficos
Autores principales: Hughes-Riley, Theodore, Six, Joseph S., Lilburn, David M.L., Stupic, Karl F., Dorkes, Alan C., Shaw, Dominick E., Pavlovskaya, Galina E., Meersmann, Thomas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2013
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3863958/
https://www.ncbi.nlm.nih.gov/pubmed/24135800
http://dx.doi.org/10.1016/j.jmr.2013.09.008
Descripción
Sumario:As an alternative to cryogenic gas handling, hyperpolarized (hp) gas mixtures were extracted directly from the spin exchange optical pumping (SEOP) process through expansion followed by compression to ambient pressure for biomedical MRI applications. The omission of cryogenic gas separation generally requires the usage of high xenon or krypton concentrations at low SEOP gas pressures to generate hp (129)Xe or hp (83)Kr with sufficient MR signal intensity for imaging applications. Two different extraction schemes for the hp gasses were explored with focus on the preservation of the nuclear spin polarization. It was found that an extraction scheme based on an inflatable, pressure controlled balloon is sufficient for hp (129)Xe handling, while (83)Kr can efficiently be extracted through a single cycle piston pump. The extraction methods were tested for ex vivo MRI applications with excised rat lungs. Precise mixing of the hp gases with oxygen, which may be of interest for potential in vivo applications, was accomplished during the extraction process using a piston pump. The (83)Kr bulk gas phase T(1) relaxation in the mixtures containing more than approximately 1% O(2) was found to be slower than that of (129)Xe in corresponding mixtures. The experimental setup also facilitated (129)Xe T(1) relaxation measurements as a function of O(2) concentration within excised lungs.