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DC Field | Value | Language |
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dc.contributor.advisor | Albert, Mitchell | - |
dc.contributor.author | Fitterman, Avner | - |
dc.date.accessioned | 2015-12-03T16:44:25Z | - |
dc.date.available | 2015-12-03T16:44:25Z | - |
dc.date.created | 2015 | |
dc.date.issued | 2015-12-03 | - |
dc.identifier.uri | http://knowledgecommons.lakeheadu.ca/handle/2453/686 | - |
dc.description.abstract | Conventional magnetic resonance imaging (MRI) modality is based on the magnetization that is formed by the influence of a strong polarizing magnetic field on the spin of protons, typically those of water molecules within the body. In Hyperpolarized (HP) gas MRI, a dramatic increase in spin polarization is achieved using spin-exchange optical pumping (SEOP), which allows images to be obtained with a high signal-to-noise ratio (SNR). Batch-mode custom-built polarizers can serve to produce the HP gas, however, such custom-built systems require optimization in terms of pressure and temperature parameters. This study is comprised of three objectives: i) Gaining understanding regarding the physics of the nuclear polarization process of 129Xe; ii) Examining experimentally the pressure and temperature dependences of the polarization, similarly to the way it was done in previous studies; iii) Exploiting this knowledge for the benefit of the optimization of the custom-built polarizer in our lab. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Magnetic resonance imaging (MRI) | en_US |
dc.subject | Hyperpolarized gas | en_US |
dc.subject | Xenon gas | en_US |
dc.title | Theory and Production of Hyperpolarized Xenon Gas | en_US |
dc.type | Thesis | |
etd.degree.name | Masters of Science | en_US |
etd.degree.level | Master | en_US |
etd.degree.discipline | Physics | en_US |
etd.degree.grantor | Lakehead University | en_US |
Appears in Collections: | Electronic Theses and Dissertations from 2009 |
Files in This Item:
File | Description | Size | Format | |
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FittermanA2015m-1b.pdf | 1.97 MB | Adobe PDF | View/Open |
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