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Diode lasers for use in experiments on cold Rydberg Atoms

Bill Whitledge

Published Jan 1, 2008• 1 citation
OpenAlex

Abstract

This project was to measure the atomic density of (85)Rb atoms in a magneto optical trap using a low-intensity probe laser. Additionally, a dark spontaneous force optical trap was constructed in an attempt to boost the trap density. The dark spot failed to appreciably increase the overall trap density (which remained steady at - N = 10^10 atoms/cm^3) but it did increase the density of dark-state atoms in the trap by an order of magnitude. This is a useful result since many experiments on cold Rydberg atoms involve exciting atoms starting in the ground state rather than the first excited state, which is occupied by a large number of atoms in a traditional magneto optical trap. The dark spot trap shows promise for boosting both the density of dark state atoms in the trap as well as the overall trap density. However, the latter goal will require further adjustment to the trap.

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Chinese Physics Letters•Feb 1, 2009•3 citations
This project was to measure the atomic density of (85)Rb atoms in a magneto optical trap using a low-intensity probe laser. Additionally, a dark spontaneous force optical trap was constructed in an attempt to boost the trap density. The dark spot failed to appreciably increase the overall trap density (which remained steady at - N = 10^10 atoms/cm^3) but it did increase the density of dark-state atoms in the trap by an order of magnitude. This is a useful result since many experiments on cold Rydberg atoms involve exciting atoms starting in the ground state rather than the first excited state, which is occupied by a large number of atoms in a traditional magneto optical trap. The dark spot trap shows promise for boosting both the density of dark state atoms in the trap as well as the overall trap density. However, the latter goal will require further adjustment to the trap.
A free-running, temperature stabilized diode laser has been injection-locked to an external cavity diode laser for use in cold Rydberg atom experiments. Cold rubidium atoms in a magneto-optical trap (MOT) are excited to Rydberg states using a 10 ns laser pulse. The Rydberg atoms spontaneously ionize due to dipole forces, and the collisional ionization dynamics are observed as a function of atom density and principal quantum number of the Rydberg state, n. The injection-locked diode laser will be used as a repumper in conjunction with a dark spontaneous-force optical trap (SPOT) to increase the Rydberg state density. We report on the design of the injection-locked laser system.
Our goal is the preparation and study of ultra- cold plasma and Rydberg matter. We assembled an ex- perimental setup for laser cooling of lithium atoms in a magneto-optical trap (MOT). Trapping of 7 Li atoms in a MOT is demonstrated for a wide range of cooling laser detunings. The number density of 7 Li atoms at different ground-state sublevels is measured by using a probe tun- able laser. The temperature of the trapped atoms is esti- mated. Obtained information is important for the prepara- tion of ultra-cold plasma and highly-excited atoms. duction of recombination in such systems. Our theoreti- cal works show the appearance of short and long-range order (7) and a large reduction of the recombination rate (a few orders of magnitude) in the ultra-cold mixture of Rydberg atoms and plasma in the presence of a strong magnetic field (8-11). The ability to control the decay and crystallization processes in an ensemble of Rydberg atoms could find an application in quantum storage and quan- tum computers. The suggested experiments can model the behavior of the plasma recombination in experiments on creating anti-hydrogen (12-14), and help to increase the number of ground state anti-hydrogen atoms in a strong magnetic field. It is noteworthy that lithium is an element which is very close to hydrogen.
Rydberg atoms are those which have their valence electron excited to high principal quantum number n. Atoms in the Rydberg state are the research focus of the experiment from which this paper derives. Rydberg atoms are fragile, and thermal collisions are enough to ionize and destroy the Rydberg state. A magneto-optical trap (MOT) serves the purpose of "ultra-cooling" atoms to temperatures around 140 micro-Kelvin and dramatically reduces the impact of thermal collisions. This paper details the theory and equipment necessary to realize a MOT of rubidium-85. It will then discuss the characterization of the MOT we implemented by a technique called low intensity absorption imaging. The result of the measurements by the absorption imaging gave an atom count of N=8.87 +/- (0.45)stat + (0.14)sys X 105 atoms and a peak atomic density of n0=1.57 +/- (0.14)stat + (0.02)sys X 1011 cm-3, where "stat" and "sys" denote statistical and systematic uncertainties. The MOT is of sufficient size and density to continue with the long term goals of the experiment [1][2].
A new magneto-optical trap is demonstrated which confines atoms predominantly in a ``dark'' hyperfine level, that does not interact with the trapping light. This leads to much higher atomic densities as repulsive forces between atoms due to rescattered radiation are reduced and trap loss due to excited-state collisions is diminished. In such a trap, more than 1010{10}^{10}1010 sodium atoms have been confined to densities approaching 1012{10}^{12}1012 atoms ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}3}$.