We are attempting to produce an atomic vapor that is so cold that the de Broglie wavelength is larger than the interparticle spacing. This is the condition needed to obtain Bose-Einstein condensation of a noninteracting gas. Our approach is to optically trap and cool atomic cesium and then load it into a purely magnetic trap for further cooling. In the course of this work we have investigated a number of magnetic traps and very low temperature collisions that are relevant to the success of this approach. In other work we are developing optical trapping techniques for the efficient collection of radioactive alkali isotopes. This work is aimed at measuring parity violation in these isotopes and thereby stringently testing the standard model of elementary particle physics. We have studied how to optimize the capture efficiency of atoms in an atomic vapor. We are currently developing cells that will allow the atoms to bounce off the walls until they are captured in the optical trap. The efficiency of this capture scheme will be discussed.
We are attempting to produce an atomic vapor that is so cold that the de Broglie wavelength is larger than the interparticle spacing. This is the condition needed to obtain Bose-Einstein condensation of a noninteracting gas. Our approach is to optically trap and cool atomic cesium and then load it into a purely magnetic trap for further cooling. In the course of this work we have investigated a number of magnetic traps and very low temperature collisions that are relevant to the success of this approach. In other work we are developing optical trapping techniques for the efficient collection of radioactive alkali isotopes. This work is aimed at measuring parity violation in these isotopes and thereby stringently testing the standard model of elementary particle physics. We have studied how to optimize the capture efficiency of atoms in an atomic vapor. We are currently developing cells that will allow the atoms to bounce off the walls until they are captured in the optical trap. The efficiency of this capture scheme will be discussed.
Summary form only given. Techniques for cooling and trapping atoms now provide unique capabilities for the manipulation of atoms. In particular, they make possible very low temperatures, extraordinarily high atomic phase space densities, and long perturbation-free observation times. These capabilities enable one to carry out many new measurements on atoms with great precision and/or in entirely new regimes of temperature and density. This tutorial will concentrate primarily on the practical aspects of how to apply current laser cooling and trapping techniques. This will include descriptions of the various techniques and their capabilities, as well as a discussion of tradeoffs between price, complexity, and various performance parameters. Finally, I will briefly discuss how these techniques are applied in a number of specific cases including cold collisions, precision measurements including atomic clocks, atom interferometry, collecting radioactive isotopes, and the creation of Bose-Einstein condensates.
Laser cooling and trapping of rare, radioactive isotopes has the potential for greatly enhancing experiments in high resolution spectroscopy of exotic species, electron electric-dipole moment searches, β-decay asymmetry, and parity nonconservation. The ability to hold atoms for several seconds at high densities (1011 cm-3) and away from the perturbing effects of the cell walls makes laser cooling and trapping attractive for use in the experiments mentioned above. Because many isotopes of interest for these experiments are difficult to produce, the ability to quickly and efficiently collect these atoms from a dilute vapor is crucial. We have demonstrated a 6% collection efficiency in a special wall-coated cell. We have developed a model that predicts the capture efficiency as a function of trap properties and have developed techniques for measuring the pertinent characteristics.
Laser cooling and trapping techniques made possible during the last two decades important achievements in the atomic physics and quantum mechanics fields. These same techniques can be usefully applied to radioactive atoms by opening new fields of investigations. Nuclear processes can be studied with the atomic physics tools. We focused our attention on Francium radioactive atoms. A magneto-optical trap has been set up at the INFN Legnaro laboratories. Preliminary tests with other stable alkali atoms aimed at an improvement of the MOT collection efficiency are reported. Fast and efficient trap loading of rubidium has been obtained through the light-induced atomic desorption from an organic coating. A larger number of sodium atoms, as compared to monochromatic trapping laser, has been trapped by using a broad-band laser.
Abstract The invention and development of laser methods for cooling and trapping atoms have led to the advent of the physics of ultracold matter. Low-temperature quantum physics has so far dealt with condensed media, wherein quantum phenomena (superfluidity and superconductivity) usually manifest themselves at temperatures of a few kelvin. Laser cooling and trapping of atoms have made it possible to successively attain millikelvin, microkelvin, and nanokelvin temperatures, at which the de Broglie wavelength of the atoms becomes commensurable with the interatomic separation, even in dilute gases. The interaction of atoms in ultracold dilute gases becomes essentially quantum mechanical. The physics of such quantum gases is more akin to the well-developed physics of condensed matter at low temperatures. It is in essence a boundary field between atomic, laser, and condensed-matter physics. Following the first, pioneering experiments on the Bose–Einstein condensation of alkali-metal atoms, this field has continued to develop at a very fast pace, which can be explained by the vast variety of particles (atoms, isotopes, and molecules) that can be laser cooled and trapped under degeneracy conditions. This is much more than physicists had at their disposal previously (3,4He). Moreover, laser radiation and magnetic fields additionally make it possible to control not only the intrinsic quantum state of the interacting ultracold particle species, but also the interaction of the particles. All this makes the research in the field of quantum gases a great breakthrough, both in atomic–molecular physics and in many-body-interaction physics, which heretofore was the prerogative of low-temperature condensed-matter physics.
A detailed experimental and theoretical investigation of a magneto-optical trap for caesium atoms is presented. Particular emphasis has been placed on achieving high spatial number densities and low temperatures. Optimizing both of these together enables efficient evaporative cooling from a conservative trap, a procedure which has recently led to the first observations of Bose-Einstein condensation in a dilute atomic vapour. The behaviour of a magneto-optical trap is nominally determined by four independent parameters: the detuning and intensity of the light field, the magnetic field gradient and the number of trapped atoms. A model is presented which incorporates previous treatments into a single description of the trap that encompasses a wide range of its behaviour. This model was tested quantitatively by measuring the temperature of the cloud and its spatial distribution as a function of the four parameters. The maximum density was found to be limited both by the reabsorption of photons scattered within the cloud and by a reduction of the confining force at small light shifts. The nonlinear variation with position of the restoring force was found to be significant in limiting the number of atoms confined to a high density. A maximum density in phase space (defined as the number of atoms in a box with sides of dimension one thermal de Broglie wavelength) of (1.5 ± 0.5) x 10-5 was observed, with a spatial density of 1.5 x 1011 atoms per cm3. Cold collision losses from a caesium magneto-optical trap have been studied with the purpose of assessing their influence on spatial densities. In contrast to previous measurements of similar quantities, these measurements did not require the use of an ultra-low (< 10-10 Torr) background vapour pressure. The dependence of the cold collision loss coefficient β on the trapping intensity was measured to permit identification of the different cold collision processes. The largest loss rates observed were those due to hyperfine structure-changing collisions, with a coefficient β = (2±1) x 10-10cm3s-1. A study is presented of a modified magneto-optical trap in which a fraction of the population is shelved into a hyperfine level that does not interact with the trapping light. In this so-called "dark" magneto-optical trap, improved densities of nearly 1012cm-3 have been previously reported for sodium. The application of the technique to caesium is not straightforward due to the larger excited state hyperfine splittings. A simple theory for caesium is presented and its main predictions verified by measurements of density, number and temperature. A density of nearly 1012cm,-3 was indeed obtained but at a temperature substantially higher than in the conventional magneto-optical trap.
The capability of manipulating neutral atoms with the force of resonant scattered laser light is being exploited in several different areas of research. The author discusses applications in particle and nuclear physics by expediting some measurements of the subtle effects of the fundamental weak interaction in atoms and nuclei. It was shown in two recent experiments that it is possible to efficiently cool accelerator produced short-lived isotopes and load them into magneto-optic traps. These demonstrations open up new possibilities for obtaining the required precision in experiments involving rare radioactive isotopes.