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School of Chemistry & Physics
THE UNIVERSITY OF ADELAIDE
SA 5005
AUSTRALIA

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Telephone: +61 8 8303 5996
Facsimile: +61 8 8303 4380

Non-absorption resonances in a J=1 to J=1 atomic system in Samarium with resonant radiation at 686nm.

This project investigates the interaction of a J=1 to J=1 atomic system (see Figure 1) in Samarium with incident resonant radiation at 686nm. Specifically this system is monitored with increasing laser exposure times to evaluate how the atom-laser interaction changes.

When the two ground state Zeeman sub-levels (m=-1,m=+1) of this atomic configuration are simultaneously excited to the single excited state level (m=0), then optical pumping can produce a coherent superposition of states. The resonant radiation creates an atomic coherence so that the atom's evolution is exactly out of phase with the incoming radiation causing non-absorption. The net result is that as the magnetic field approaches zero, the atom is `trapped' in a coherent superposition of states and is unable to absorb less and less resonant radiation until a minimum absorption occurs when the magnetic field is zero. In a three-state Λ system, this phenonmenon is known as `coherent population trapping' or a `dark-line resonance', and was first observed in 1976 by Alzetta et al. See Figure 2.

In the experiment (see Figure 3), a linearly polarized laser at 686nm excites atoms from the level 4f6 6s2 7 F1 to a excited level 4f6 6s6p 9F1 via the process of optical pumping. The resonant radiation is supplied by an external cavity diode laser; manipulation of the external cavity allows the wavelength to be tuned to the transition. When an external magnetic field is applied, a level-crossing fluorescence intensity profile can be recorded. A non-absorption resonance is an obvious feature of these level-crossing profiles.

Level-crossing profiles are recorded with different exposure lengths to resonant radiation. As non-absorption resonances are a second-order effect, these resonances are used as a sensitive indicator of how the J=1 to J=1 atomic system evolves with increasing resonant radiation.


Vacuum system and optical table where interaction takes place between the laser radiation and Samarium atoms.

Figure 3: Vacuum system and optical table where interaction takes place between the laser radiation and Samarium atoms.

References

An experimental method for the observation of rf transitions and laser beat resonances in Na vapour.
G. Alzetta, A. Gozzini, L. Moi, G. Orriols.
Il nuovo cimento, 36B:5, 1976.

Non-absorption resonances by nonlinear coherent effects in a three level system.
G. Orriols.
Il nuovo cimento, 53B:1, 1979.

Personnel

Ms Shu-Yen Lee
A/Prof Murray Hamilton