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dc.contributor.advisorChen, Wei
dc.creatorSahi, Sunil Kumar
dc.date.accessioned2016-07-08T20:01:28Z
dc.date.available2016-07-08T20:01:28Z
dc.date.created2016-05
dc.date.issued2016-05-11
dc.date.submittedMay 2016
dc.identifier.urihttp://hdl.handle.net/10106/25766
dc.description.abstractInorganic single crystal and organic (plastic and liquid) scintillators are commonly used for radiation detection. Inorganic single crystals are efficient and have better energy resolution compared to organic scintillators. However, inorganic single crystals are difficult to grow in large size and hence expensive. On the other hand, fast decay time and ease of fabrication makes organic scintillators attractive for many applications. However, poor energy resolution of organic scintillators limits its applications in gamma ray spectroscopy. The poor energy resolution is due to the low Z-Value and low density of organic scintillator. The Z-value of organic plastic scintillator can be increase by loading nanoparticles in plastic matrix. It is expected that the increase in Z-value would result in improve energy resolution of nanocomposite scintillator. However, the loss of optical transparency due to nanoparticles loading is one of the major concerns of nanocomposite scintillators. In this dissertation, we used different methods to synthesize LaxCe1-xF3 nanoparticles with high dispersion in polymer matrix. High nanoparticle dispersion is important to load high concentration of nanoparticles into polymer matrix without losing the transparency of the polymer matrix. The as synthesized nanoparticles are dispersed into monomers and polymerized using heat initiated bulk polymerization method. Nanoparticles are characterized using TEM, XRD, FTIR and TGA. The optical and scintillation properties of nanoparticles and nanocomposites are studied using spectroscopic techniques. The pulse height spectra obtained using nanocomposite fabricated by loading up to 30 wt% nanoparticles clearly show a photopeak for the 122 keV line of the Co-57 isotope. The generation of the photopeak is due to the enhanced photoelectric effect as a result of increased effective atomic number (Zeff) and density of nanocomposite scintillator. The pulse height spectra of Cs-137 gamma source show a full energy peak at around 622 keV, due to the escape of La and Ce Kα X-rays. The fabrication process of transparent nanocomposite scintillator is discussed in details.
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.subjectNanocomposite scintillators
dc.subjectScintillation
dc.subjectPolymerizable surfactant
dc.subjectHVDAC
dc.subjectTransparent ceramic
dc.subjectLaF3-Ce
dc.subjectLaxY2-xO3
dc.subjectPolymer nancomposite
dc.titleSynthesis and Characterization of Nanocomposite Scintillators for Radiation Detection
dc.typeThesis
dc.degree.departmentPhysics
dc.degree.nameDoctor of Philosophy in Physics and Applied Physics
dc.date.updated2016-07-08T20:02:31Z
thesis.degree.departmentPhysics
thesis.degree.grantorThe University of Texas at Arlington
thesis.degree.levelDoctoral
thesis.degree.nameDoctor of Philosophy in Physics and Applied Physics
dc.type.materialtext
dc.creator.orcid0000-0001-5379-9942


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