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dc.contributor.authorWilson, Nicholas
dc.date.accessioned2014-02-07
dc.date.available2014-02-07
dc.date.issued2013-09-30
dc.identifier.urihttp://hdl.handle.net/2123/10015
dc.description.abstractThe functional integral formulation of finite temperature field theory and its connection to statistical mechanics is reviewed. The one loop contributions to quantum electrodynamics at finite temperature are explicitly calculated. Dyson-Schwinger equations for quantum electrodynamics at finite temperature are constructed and possible methods of solving them are discussed.en_AU
dc.titleDyson-Schwinger equations in quantum electrodynamics at finite temperatureen_AU
dc.typeThesisen_AU
dc.date.valid2014-01-01en_AU
dc.type.thesisMasters by Researchen_AU
usyd.facultyFaculty of Science, School of Mathematics and Statisticsen_AU
usyd.degreeMaster of Science M.Sc.en_AU
usyd.awardinginstThe University of Sydneyen_AU


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