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dc.contributor.authorLIEPMANN, TILL WOLFGANG.
dc.creatorLIEPMANN, TILL WOLFGANG.en_US
dc.date.accessioned2011-10-31T18:11:07Z
dc.date.available2011-10-31T18:11:07Z
dc.date.issued1983en_US
dc.identifier.urihttp://hdl.handle.net/10150/186493
dc.description.abstractA common path interferometer utilizing noncritically phase matched frequency doubling crystals is presented. The interference pattern is directly sensitive to the wavefront shape (like that of a Mach Zender) and is in the second harmonic of the laser source. This interferometer has twice the sensitivity of a two beam interferometer. All the optics are 100% transmitting (i.e. no beam splitters), the contrast is adjustable, and the laser intensity pattern is not affected by the interferometer. This interferometer is similar in some ways to the Point Diffraction interferometer, and the two are compared in this paper. A theory of operation is presented, though the reference wave of the interferometer is flatter than predicted. Several possible reasons for this were examined, but no discovery made.
dc.language.isoenen_US
dc.publisherThe University of Arizona.en_US
dc.rightsCopyright © is held by the author. Digital access to this material is made possible by the University Libraries, University of Arizona. Further transmission, reproduction or presentation (such as public display or performance) of protected items is prohibited except with permission of the author.en_US
dc.subjectInterferometers.en_US
dc.titleCONVOLUTION PRODUCT INTERFEROMETER.en_US
dc.typetexten_US
dc.typeDissertation-Reproduction (electronic)en_US
dc.identifier.oclc689059032en_US
thesis.degree.grantorUniversity of Arizonaen_US
thesis.degree.leveldoctoralen_US
dc.identifier.proquest8319725en_US
thesis.degree.disciplineOptical Sciencesen_US
thesis.degree.disciplineGraduate Collegeen_US
thesis.degree.namePh.D.en_US
refterms.dateFOA2018-08-15T03:43:34Z
html.description.abstractA common path interferometer utilizing noncritically phase matched frequency doubling crystals is presented. The interference pattern is directly sensitive to the wavefront shape (like that of a Mach Zender) and is in the second harmonic of the laser source. This interferometer has twice the sensitivity of a two beam interferometer. All the optics are 100% transmitting (i.e. no beam splitters), the contrast is adjustable, and the laser intensity pattern is not affected by the interferometer. This interferometer is similar in some ways to the Point Diffraction interferometer, and the two are compared in this paper. A theory of operation is presented, though the reference wave of the interferometer is flatter than predicted. Several possible reasons for this were examined, but no discovery made.


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