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Bulletin of the American Physical Society

Optimized modulation parameters for a two-dimensional magneto-optical trap for cold fermionic potassium atoms

Jae Hoon Lee, Jongchul Mun

Published May 25, 2016• 0 citations
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We report on an experimental realization of a two-dimensional magneto-optical trap (2D-MOT) that allows the generation of cold atomic beams of $^{39}\mathrm{K}$ and $^{41}\mathrm{K}$ bosonic potassium isotopes. The high measured fluxes up to $1.0\ifmmode\times\else\texttimes\fi{}{10}^{11}\phantom{\rule{0.3em}{0ex}}\mathrm{atoms}∕\mathrm{s}$ and low atomic velocities around $33\phantom{\rule{0.3em}{0ex}}\mathrm{m}∕\mathrm{s}$ are well suited for a fast and reliable three-dimensional magneto-optical trap loading, a basilar feature for new generation experiments on Bose-Einstein condensation of dilute atomic samples. We also present a simple multilevel theoretical model for the calculation of the light-induced force acting on an atom moving in a MOT. The model gives a good agreement between predicted and measured flux and velocity values for our 2D-MOT.

arXiv:cond-mat/0511113•Physical Review A•Mar 14, 2006•53 citations
We present our study on enhancement and optimization of potassium-40 (K40) atomic beam flux from a two-dimensional magneto-optical trap (2D MOT) by modulating the frequency of cooling laser. The laser cooling beam frequencies of the 2D MOT were effectively broadened via electro-optical modulators at 10 MHz, with a modulation index ranging from β=0 to 7, depending on the laser intensity. Laser parameters of the 2D MOT beams and the magnetic field gradient were scanned for optimal settings for maximum atomic beam flux. When compared to a conventional 2D MOT with fixed laser frequencies, we were able to obtain a 3.7 times enhancement of the atomic flux when the total laser power was 640 mW. Numerical calculations predict further improvement for higher laser beam intensities.
We present the design, implementation, and detailed experimental characterization and comparison with numerical simulations of two-dimensional magneto-optical traps (MOTs) of bosonic 23Na and 39K atoms for loading the cold atomic mixture in a dual-species 3DMOT with a large number of atoms. We report our various measurements pertaining to the characterization of two 2D+MOTs via the capture rate in the 3DMOT and also present the optimized parameters for the best performance of the system of the cold atomic mixture. Under the optimized condition, we capture more than 3 × 101039K atoms and 5.8 × 10823Na atoms in the 3DMOT simultaneously from individual 2D+MOTs with a capture rate of 5 × 1010 and 3.5 × 108 atoms/sec for 39K and 23Na, respectively. We also demonstrate improvements of more than a factor of 5 in the capture rate in the 3DMOT from the cold atomic sources when a relatively high-power ultraviolet light is used to cause light-induced atomic desorption in the 2D+MOT glass cells. A detailed study of the light assisted interspecies cold collisions between the co-trapped atoms is presented, and interspecies loss coefficients have been determined to be βNaK ∼ 2 × 10−12 cm3/sec. The cold atomic mixture would be useful for further experiments on quantum simulation with ultra-cold quantum mixtures in optical potentials.
We report on an experimental realization of a two-dimensional magneto-optical trap (2D-MOT) that allows the generation of cold atomic beams of 39K^{39}\mathrm{K}39K and 41K^{41}\mathrm{K}41K bosonic potassium isotopes. The high measured fluxes up to $1.0\ifmmode\times\else\texttimes\fi{}{10}^{11}\phantom{\rule{0.3em}{0ex}}\mathrm{atoms}∕\mathrm{s}$ and low atomic velocities around 33m∕s33\phantom{\rule{0.3em}{0ex}}\mathrm{m}∕\mathrm{s}33m∕s are well suited for a fast and reliable three-dimensional magneto-optical trap loading, a basilar feature for new generation experiments on Bose-Einstein condensation of dilute atomic samples. We also present a simple multilevel theoretical model for the calculation of the light-induced force acting on an atom moving in a MOT. The model gives a good agreement between predicted and measured flux and velocity values for our 2D-MOT.