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Physics Letters A

Forward scattering of monochromatic laser light revisited

Suzanne Giraud-Cotton, V.Paul Kaftandjian, Lewis S. Klein

Published Aug 1, 1982• 4 citations
Publisher
DOI
10.1016/0375-9601(82)90792-7

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The forward scattering of a resonant intense and broad-band (of the order of 1 GHz) laser light on sodium atoms is described. The experimental results for the D 1 and D 2 sodium lines (the 3 2 S 1/2 -3 2 P 1/2 and 3 2 S 1/2 -3 2 P 3/2 transitions) are compared with those of the scattering of the light from a conventional spectral lamp and from a monochromatic laser. The observed differences are explained by taking into account the Zeeman coherences created in the irradiated atoms and the concept of the 'hyperfine uncoupling' is proposed for describing the interaction of atoms with the broad-band laser light.
We present experimental and theoretical investigations of a Gaussian laser beam interacting with Zeeman-tuned J=1\ensuremath{\rightarrow}J=0 atomic systems. In our experiment a single-mode cw dye-laser beam traverses a neon discharge in a longitudinal magnetic field. The excited neon transitions used for these studies are 1s4{\mathit{s}}_{4}s4​(J=1,g=1.464)\ensuremath{\rightarrow}2p3{\mathit{p}}_{3}p3​(J=0) and 1s2{\mathit{s}}_{2}s2​(J=1,g=1.034)\ensuremath{\rightarrow}2p1{\mathit{p}}_{1}p1​(J=0). In the laser-induced forward-scattered light, dark and bright ring-shaped structures are observed. The ring structures are investigated as a function of the magnetic detuning of the m=\ifmmode\pm\else\textpm\fi{}1 sublevels and as a function of the laser-beam power. We find that the line shapes of the spectra, i.e., the forward-scattered light intensities as a function of the magnetic detuning, are sensitive to the transverse intensity distribution of the laser beam. Analytical expressions based on a semiclassical theory are derived and the calculated results on the ring structures and the spectra are compared with the experimental results. Good agreement between the calculated and the experimental results are obtained only when the transverse effects are taken into account.