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Bose-Einstein condensation of lithium

Posted on:1998-04-09Degree:Ph.DType:Dissertation
University:Rice UniversityCandidate:Bradley, Curtis CharlesFull Text:PDF
GTID:1460390014476105Subject:Physics
Abstract/Summary:
Bose-Einstein condensation (BEC) in ultra-cold magnetically-trapped {dollar}sp7{dollar}Li vapor was experimentally observed and quantitative measurements of condensate number were made. Compared to other BEC experiments, lithium is unique due to its negative s-wave scattering length, corresponding to effectively attractive interactions. Due to this attraction, condensates are expected to undergo mechanical collapse if the condensate number exceeds a critical value. In this experiment, an upper limit of about 1000 condensate atoms is found, in agreement with theoretical predictions.; In the experiment, the atoms are confined by a set of six permanent magnets in the Ioffe configuration. Optical forces are used to slow and guide atoms from a thermal atomic beam into the magnetic trap. With about {dollar}10sp8{dollar} atoms loaded into the trap, the vapor is laser-cooled to near 200 {dollar}mu{dollar}K and then evaporatively cooled by application of a resonantly-tuned microwave field. Evaporative cooling produces a million-fold increase in phase-space density, reaching quantum-degenerate conditions with about 10{dollar}sp5{dollar} atoms at temperatures near 300 {dollar}mu{dollar}K. After cooling, the trapped atom distribution is observed by in situ imaging via an optical probe. Calculated atom distributions are fit to the image data.; In initial data, the imaging resolution was insufficient to see the spatially-narrow condensate peak, but as phase-space densities approached the expected phase transition, the images suddenly became distorted. Initial fits to the data suggested as many as 10{dollar}sp5{dollar} condensate atoms, in strong disagreement with theoretical predictions. An imaging model, accounting for imperfections in the imaging optics, shows that the sudden appearance of the distortions is a consequence of BEC, and that these distortions led to the initial over-estimation of cloud phase-space density and condensate number.; Improved imaging was obtained using large probe detunings, a Phase-Contrast Polarization Imaging (PCPI) technique, and near-diffraction-limited imaging optics. The PCPI method exploits the birefringence of the trapped atoms. From the resulting images, quantitative estimates of condensate number are obtained and compared with theory.
Keywords/Search Tags:Condensate number, Atoms, BEC
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