A theoretical investigation is reported of a two-dimensional focusing of an atomic beam by a centrally symmetric optical field formed by two pairs of mutually perpendicular laser beams. Conditions under which this optical field acts as a converging laser lens are identified. The errors of such a laser focusing system are determined.
The principal element in any sort of optics is a lens. It is essential to create laser field configurations capable of focusing neutral atomic beams. There are two possibilities for focusing an atomic beam by laser light: by using the gradient force or by using the light pressure force. The force effecting the focusing of an atom in a beam should be proportional to the atomic displacement. This criterion must be satisfied for the force to produce the true “image”: if this criteria is not met, the image is blurred, i.e. there are aberrations. An approach to treat the focusing of atomic beam by laser light is to use the path integral technique to calculate the evolution of atomic wave function as it propagates in laser field. A particle-optical approach also can be used for treatment of focusing of atoms by laser light. The quadratic radial dependence of the potential is a necessary condition for focusing of atoms.
Summary form only given. Laser focusing of neutral atoms is a unique approach for fabricating periodic small structures. In a standing wave formed by two counter-propagating laser beams, the radiation force acts as a sequence of cylindrical lenses that focus the atoms into a periodic array of parallel lines during deposition onto a substrate. In this way, a pattern is written onto the substrate without the use of any masks. To minimize the feature width on the substrate, the atoms entering the focusing laser must be highly collimated transversely by optical cooling.
We report on the atom optical manipulation of an atom laser beam. Reflection, focusing, and its storage in a resonator are demonstrated. Precise and versatile mechanical control over an atom laser beam propagating in an inhomogeneous magnetic field is achieved by optically inducing spin flips between atomic ground states with different magnetic moment. The magnetic force acting on the atoms can thereby be effectively switched on and off. The surface of the atom optical element is determined by the resonance condition for the spin flip in the inhomogeneous magnetic field. More than 98% of the incident atom laser beam is reflected specularly.
The focusing of a neutral atomic beam using near-resonant laser light is considered. The results of a path integral solution to the Schrodinger in the stationary phase approximation are presented. The details of the derivation of the propagation kernel are presented elsewhere [1]. This approach is general and allows us to deal with "thick" laser lenses. Numerical results for the focusing of a Gaussian atomic beam are presented. These results show that spot diameters on the order of 20 Angstroms are obtainable for many reasonable choices of laser and atomic beam parameters, and that for most of these cases the thin lens approximation is not valid.
Summary form only given. Recently it has been demonstrated that neutral atomic beams can be focused by use of a laser as an atom-optical lens. Standing wave atom-optical (SW) lenses have been of particular interest because of the potential for both high-resolution and high-throughput lithography. In this paper, using sub-Doppler optical cooling schemes in conjunction with mechanical collimation, and a SW with /spl sigma/=56 /spl mu/m, we have been able to achieve <20 nm resolution with contrast of at least 10:1, focusing a thermal atomic sodium beam using 589-nm light corresponding to the D/sub 2/ transition.