dc.rights.license | CC-BY-NC-ND | |
dc.contributor.advisor | Laenen, Eric | |
dc.contributor.advisor | Gursoy, Umut | |
dc.contributor.author | Rajamov, M. | |
dc.date.accessioned | 2019-08-20T17:00:45Z | |
dc.date.available | 2019-08-20T17:00:45Z | |
dc.date.issued | 2019 | |
dc.identifier.uri | https://studenttheses.uu.nl/handle/20.500.12932/33486 | |
dc.description.abstract | We discuss why the usual perturbation theory in unsuited for the study of bound states in quantum field theory. The Dyson equation for the 4-point Green's function is then presented and the Bethe-Salpeter equation derived from it, by using Green's function factorization around bound state poles. Some historical facts are given for context, after which we discuss a particular approach for solving the Bethe-Salpeter equation known as the quasipotential approach. We discuss several possible choices of gauge and two-body propagator that can be used within this scheme and use one to calculate the leading order hyperfine splitting in positronium. | |
dc.description.sponsorship | Utrecht University | |
dc.format.extent | 535068 | |
dc.format.mimetype | application/pdf | |
dc.language.iso | en | |
dc.title | Quasipotential approach to the Bethe-Salpeter equation for positronium | |
dc.type.content | Master Thesis | |
dc.rights.accessrights | Open Access | |
dc.subject.keywords | Green's function, two-body propagator, positronium, hydrogen, bound state, perturbation theory, quasipotential | |
dc.subject.courseuu | Theoretical Physics | |