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arXiv:physics/0604026 · Journal of Physics B Atomic Molecular and Optical Physics

Electromagnetically induced transparency in6Li

Jean-Noël Fuchs, G J Duffy, W J Rowlands, A. M. Akulshin

Published Aug 14, 2006• 9 citations
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Abstract

We report electromagnetically induced transparency for the D1 and D2 lines in $^{6}$Li in both a vapour cell and an atomic beam. Electromagnetically induced transparency is created using co-propagating mutually coherent laser beams with a frequency difference equal to the hyperfine ground state splitting of 228.2 MHz. The effects of various optical polarization configurations and applied magnetic fields are investigated. In addition, we apply an optical Ramsey spectroscopy technique which further reduces the observed resonance width.

DOI
10.1088/0953-4075/39/17/006

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Abstract. We report sub-Doppler and sub-natural linewidth spectroscopy of 6Li on the D1 and D2 lines in both a vapour cell and an atomic beam. Electromagnetically induced transparency is created using co-propagating mutually coherent laser beams with a frequency difference equal to the hyperfine ground state splitting of 228.2 MHz. The effects of various optical polarization configurations and applied magnetic fields are investigated. In addition, we present an optical Ramsey spectroscopy technique which further reduces the observed resonance width.
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We report on an investigation of electromagnetically induced transparency (EIT) in sodium vapour. In our experiment, sodium atoms are excited on the D1-line with laser radiation containing two components with a frequency difference close to that of the two hyperfine ground states of sodium (1.772 GHz). Such an excitation leads to coherent trapping of atomic population in “dark” superpositional states, which dramatically reduces the absorption of light. A frequency transparency window is measured to have a subnatural width, which is a clear indication of coherent population trapping. Dependence of EIT on laser frequencies and intensities, on the magnetic field strength as well as on the temperature of the sodium vapour is studied.
We report the first study of electromagnetically induced transparency (EIT) on the D1 and D2 lines of 7 Li in a vapour cell. The effect of different polarizations, background gas pressures and experimental designs on the dark resonance are examined. It is found that EIT is more prominent on the D1 line than on the D2 line and is present at the D2 transition under incident orthogonal linearly polarized fields and parallel circularly polarized fields, but absent for parallel linearly polarized fields and for orthogonal circularly polarized fields. It is shown that the contrast of the dark resonances can be affected by the presence of an inert background gas. An analysis of a further nine resonances observed at the D1 transition and three resonances at the D2 transition is presented.
This thesis investigates the parameters of achieving electromagnetically induced transparency, or EIT. The technique of EIT manipulates the properties of atoms to partially cancel the usual absorption of laser light. In this experiment, the effect was observed using the D1 line of rubidium vapor and a Λ -configuration between the degenerate magnetic sublevels of the 5S1/2(F=1) and 5P1/2(F=1) hyperfine states. Among the parameters investigated were the linear and circular polarization of the light used to drive the transitions, the size of the laser beam used, the effects of the temperature of the rubidium interaction cell on EIT, the density of the rubidium atoms in the interaction cell, and the effects of changing the power of the fields used to drive the transitions. Careful measurements of these parameters were made.
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