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dc.contributor.advisorWatson, Deborah K
dc.creatorLaing, William Blake
dc.date.accessioned2019-04-27T21:27:43Z
dc.date.available2019-04-27T21:27:43Z
dc.date.issued2008
dc.identifier99211551902042
dc.identifier.urihttps://hdl.handle.net/11244/318746
dc.description.abstractWe generalize the harmonic-order N-body DPT method for an isotropically confined quantum system of identical interacting bosons to first-anharmonic order and, in principle, higher orders. We introduce a graphical decomposition of the perturbative expansion of the N-body Hamiltonian. We calculate the Clebsch-Gordon coefficient tensors that couple together 3 irreducible representations of SN analytically, and analytically transformed the graphical basis to collective coordinates. We calculate the N-body wavefunction and density profile in general and have demonstrated agreement with an analytic model. We apply this formalism to the exactly-solvable example of a trapped gas of atoms interacting with a (fully-interacting) harmonic-oscillator "Hooke's law" interaction and compare with the dimensional expansion of the exact ground-state wavefunction and density profile. We report progress on the example of a cold gas BEC (with zero angular momentum).
dc.format.extent212 pages
dc.format.mediumapplication.pdf
dc.languageen_US
dc.relation.requiresAdobe Acrobat Reader
dc.subjectBose-Einstein condensation
dc.subjectPerturbation (Quantum dynamics)
dc.subjectHamiltonian systems
dc.subjectMany-body problem
dc.titleConfined Quantum Systems: Beyond Harmonic Order in Dimensional Perturbation Theory
dc.typetext
dc.typedocument
dc.thesis.degreePh.D.
ou.groupCollege of Arts and Sciences::Homer L. Dodge Department of Physics and Astronomy


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