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Delelopment of an x-ray prism for a combined diffraction enhanced imaging and fluorescence imaging system

dc.contributor.advisorChapman, Deanen_US
dc.contributor.committeeMemberPywell, Roben_US
dc.contributor.committeeMemberThomlinson, Williamen_US
dc.contributor.committeeMemberGeorge, Grahamen_US
dc.contributor.committeeMemberHall, Chrisen_US
dc.contributor.committeeMemberSmolyakov, Andreien_US
dc.creatorBewer, Brian Edwarden_US
dc.date.accessioned2010-10-21T10:51:54Zen_US
dc.date.accessioned2013-01-04T05:06:28Z
dc.date.available2012-02-25T08:00:00Zen_US
dc.date.available2013-01-04T05:06:28Z
dc.date.created2010-12en_US
dc.date.issued2010-12en_US
dc.date.submittedDecember 2010en_US
dc.description.abstractAnalyzer crystal based imaging techniques such as diffraction enhanced imaging (DEI) and multiple imaging radiography (MIR) utilize the Bragg peak of perfect crystal diffraction to convert angular changes into intensity changes. These X-ray techniques extend the capability of conventional radiography, which derives image contrast from absorption, by providing a large change in intensity for a small angle change introduced by the X-ray beam traversing the sample. Objects that have very little absorption contrast may have considerable refraction and ultra small angle X-ray scattering (USAXS) contrast thus improving visualization and extending the utility of X-ray imaging. To improve on the current DEI technique this body of work describes the design of an X-ray prism (XRP) included in the imaging system which allows the analyzer crystal to be aligned anywhere on the rocking curve without moving the analyzer from the Bragg angle. By using the XRP to set the rocking curve alignment rather than moving the analyzer crystal physically the needed angle sensitivity is changed from ìradians for direct mechanical movement of the analyzer crystal to milliradian control for movement the XRP angle. In addition to using an XRP for the traditional DEI acquisition method of two scans on opposite sides of the rocking curve preliminary tests will be presented showing the potential of using an XRP to scan quickly through the entire rocking curve. This has the benefit of collecting all the required data for image reconstruction in a single fast measurement thus removing the occurrence of motion artifacts for each point or line used during a scan. The XRP design is also intended to be compatible with combined imaging systems where more than one technique is used to investigate a sample. Candidates for complimentary techniques are investigated and measurements from a combined X-ray imaging system are presented.en_US
dc.identifier.urihttp://hdl.handle.net/10388/etd-10212010-105154en_US
dc.language.isoen_USen_US
dc.subjectprismen_US
dc.subjectAnalyzer based imagingen_US
dc.subjectMIRen_US
dc.subjectDEIen_US
dc.subjectXRPen_US
dc.titleDelelopment of an x-ray prism for a combined diffraction enhanced imaging and fluorescence imaging systemen_US
dc.type.genreThesisen_US
dc.type.materialtexten_US
thesis.degree.departmentPhysics and Engineering Physicsen_US
thesis.degree.disciplinePhysics and Engineering Physicsen_US
thesis.degree.grantorUniversity of Saskatchewanen_US
thesis.degree.levelDoctoralen_US
thesis.degree.nameDoctor of Philosophy (Ph.D.)en_US

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