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Physical Review A

Numerical study of magneto-optical traps through a hierarchical tree method

R. S. de Oliveira, Ernesto P. Raposo, S. S. Vianna

Published Aug 2, 2004• 6 citations
Publisher

Abstract

We approach the problem of $N$ atoms in a magneto-optical trap through a hierarchical tree method, using an algorithm originally developed by Barnes and Hut (BH) in the astrophysical context. Such an algorithm numerically takes care of the particle-particle interaction by controlling the approximation level in a way that offers more physical fidelity than the mean-field treatment and considerably less time consumption ($\ensuremath{\tau}\ensuremath{\sim}N\phantom{\rule{0.3em}{0ex}}{\mathrm{log}}_{10}\phantom{\rule{0.3em}{0ex}}N$ in the hierarchical BH method, in contrast with the $\ensuremath{\tau}\ensuremath{\sim}{N}^{2}$ and $\ensuremath{\tau}\ensuremath{\sim}{N}^{3∕2}$ dependences found in direct and mean-field approaches, respectively). Our results reproduce the experimentally reported single-ring orbital mode for $N\ensuremath{\lesssim}{10}^{6}$ atoms and also find indication of a double-ring structure for $N\ensuremath{\sim}{10}^{7}$, a situation mimicked by a $N={10}^{6}$ system with enhanced radiative force, in agreement with experimental observations. We stress that this high-density regime is not accessed by direct integration of the equations of motion, due to the enormous computing times required, and is not suitably described through mean-field approaches, due to the rather unphysical enhancement of the particle-particle interactions and the presence of a spurious numerical grid dependence.

DOI
10.1103/physreva.70.023402

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Japanese Journal of Applied Physics•Sep 1, 1996•1 citation
We approach the problem of NNN atoms in a magneto-optical trap through a hierarchical tree method, using an algorithm originally developed by Barnes and Hut (BH) in the astrophysical context. Such an algorithm numerically takes care of the particle-particle interaction by controlling the approximation level in a way that offers more physical fidelity than the mean-field treatment and considerably less time consumption (\ensuremathτ\ensuremath∼Nlog10N\ensuremath{\tau}\ensuremath{\sim}N\phantom{\rule{0.3em}{0ex}}{\mathrm{log}}_{10}\phantom{\rule{0.3em}{0ex}}N\ensuremathτ\ensuremath∼Nlog10​N in the hierarchical BH method, in contrast with the \ensuremathτ\ensuremath∼N2\ensuremath{\tau}\ensuremath{\sim}{N}^{2}\ensuremathτ\ensuremath∼N2 and \ensuremathτ\ensuremath∼N3∕2\ensuremath{\tau}\ensuremath{\sim}{N}^{3∕2}\ensuremathτ\ensuremath∼N3∕2 dependences found in direct and mean-field approaches, respectively). Our results reproduce the experimentally reported single-ring orbital mode for N\ensuremath≲106N\ensuremath{\lesssim}{10}^{6}N\ensuremath≲106 atoms and also find indication of a double-ring structure for N\ensuremath∼107N\ensuremath{\sim}{10}^{7}N\ensuremath∼107, a situation mimicked by a N=106N={10}^{6}N=106 system with enhanced radiative force, in agreement with experimental observations. We stress that this high-density regime is not accessed by direct integration of the equations of motion, due to the enormous computing times required, and is not suitably described through mean-field approaches, due to the rather unphysical enhancement of the particle-particle interactions and the presence of a spurious numerical grid dependence.
The different orbital modes that appear from the misalignment of the laser beams in the xy plane of a low-density magneto-optical trap are studied. Using the circular motion approximation, one can obtain a qualitative description of the phenomenon and can calculate the ring radii, the atom’s velocity in the ring, and the trap parameters in which the rings appear. A careful analysis of some theories previously employed in researching this topic shows that they have extrapolation problems that led to unreasonable conclusions. In particular, we compare the results of the circular motion approximation itself with those obtained from a direct numerical integration of the atomic trajectory. Within this approximation the influence of the increase in the number of trapped atoms over the ring is also investigated, and we observe an instability in a ring-shaped structure when the interaction between the atoms is included.
Since the first proposal and the first experiment on magneto-optical trapping of atoms, magneto-optical traps (MOT) became the most popular traps for cold atoms. Despite the numerous successful applications of MOT it is still unclear what ultimate parameters could be expected for atoms trapped in MOT. We develop the theory of MOT for cold atoms under the multilevel dipole interaction schemes. Theory is based on consideration of one-dimensional motion of atoms which have three ground-state sublevels (F/sub g/=1) and five upper-state sublevels (F/sub e/=2) and are in inhomogeneous magnetic field and in the field of two counter-propagating circular polarized laser waves. It is shown that in multilevel interaction schemes two-photon processes are responsible for formation of a narrow velocity and spatial structure in the radiation force. It is found that two-photon coherent process enhances considerably the friction force and the oscillation frequency at negative detuning. Single-photon and two-photon processes are shown to produce the two-component structure of the MOT potential and accordingly the two-component coordinate distribution.
In this work, we present a theoretical study of the origin of the spatial structures in the conventional magneto-optical trap by using a numerical model based on the solutions of the equations of motion of trapped atoms, in the limit where the radiation trapping force is not relevant. Some results relating to the comparison between the experimental and theoretical data are reported. Also, we show that this same analysis can be employed to describe the spatial structures formation in atomic beams.
A single-particle kinetic theory of the magneto-optical trap (MOT) for cold atoms is developed for a multilevel dipole interaction scheme. The theory analyzes the one-dimensional motion of (3+5)(3+5)(3+5)-level atoms in an inhomogeneous magnetic field and in the field of two counterpropagating circularly polarized laser waves. It is shown that in multilevel interaction schemes two-photon and generally even-order multiphoton processes are responsible for the formation of the narrow velocity and spatial structures in the radiation pressure force. The structures are located at zero velocity and near the origin of the trap. It is found that in the case of a (3+5)(3+5)(3+5)-level atom, single- and two-photon processes produce the two-component structure of the MOT potential well. Near the bottom of a conventional spatially broad potential well caused by one-photon processes, there is a much narrower well caused by two-photon processes. The double-structure MOT potential well is shown to be responsible for the two-component spatial distribution of the trapped atomic cloud. It is proposed that tight confinement of atoms near the narrow bottom of the MOT potential well can be used for the creation of a pointlike source of cold atoms for various applications in atom optics.
We present the observation of double stable clouds of cold trapped atoms in a magneto-optical trap and its explanation with a simple model based on radiative forces. This structure occurs for a specific misalignment of the trapping laser beams whose Gaussian profiles introduce an extra term in the equation of motion for the trapped atom. We were able to obtain simple analytical expressions for the trap potential and for the separation of the clouds, and carried out a numerical calculation which agrees well with the experimental observations.