Optical molasses schematic

Optical molasses is a laser cooling technique that can cool neutral atoms to as low as a few microkelvin, depending on the atomic species. An optical molasses consists of 3 pairs of counter-propagating circularly polarized laser beams intersecting in the region where the atoms are present. The main difference between optical molasses and an MOT is the absence of magnetic field in the former. Therefore, unlike a MOT, an optical molasses provides only cooling and no trapping.

History

When laser cooling was proposed in 1975, a theoretical limit on the lowest possible temperature was predicted.[1] Known as the Doppler limit, , this was given by the lowest possible temperature attainable considering the cooling of two-level atoms by Doppler cooling and the heating of atoms due to momentum diffusion from the scattering of laser photons. Here, , is the natural line-width of the atomic transition, , is the reduced Planck constant and, , is the Boltzmann constant.

Experiments at the National Institute of Standards and Technology, Gaithersburg, found the temperature of cooled atoms to be well below the theoretical limit.[2]In 1988, Lett et al. [2] directed Sodium atoms through an optical molasses and found the temperatures to be as low as ~40μk; 6 times lower than the expected 240μk doppler cooling limit. Other unexpected properties found in other experiments[3]included significant unexpected insensitivity to laser alignment of the counter-propagating beams.


Theory

The best explanation of the phenomenon of optical molasses is based on the principle of polarization gradient cooling.[4] Counterpropagating beams of circularly polarized light cause a standing wave, where the light polarization is linear but the direction rotates along the direction of the beams at a very fast rate. Atoms moving in the spatially varying linear polarisation have a higher probability density of being in a state that is more susceptible to absorption of light from the beam coming head-on, rather than the beam from behind. This results in a velocity dependent damping force that is able to reduce the velocity of a cloud of atoms to near the recoil limit.

See also

References

  1. ↑ Hänsch, T.W.; Schawlow, A.L. (1975). "Cooling of gases by laser radiation". Optics Communications. 13 (1): 68–69. Bibcode:1975OptCo..13...68H. doi:10.1016/0030-4018(75)90159-5. ISSN 0030-4018.
  2. 1 2 Lett, Paul D.; Watts, Richard N.; Westbrook, Christoph I.; Phillips, William D.; Gould, Phillip L.; Metcalf, Harold J. (1988). "Observation of Atoms Laser Cooled below the Doppler Limit". Physical Review Letters. 61 (2): 169–172. Bibcode:1988PhRvL..61..169L. CiteSeerX 10.1.1.208.9100. doi:10.1103/PhysRevLett.61.169. ISSN 0031-9007. PMID 10039050. S2CID 8479501.
  3. ↑ Lett, Paul D.; Westbrook, Christoph I.; Watts, Richard N.; Rolston, S.L; Gould, Phillip L.; Metcalf, Harold J.; Phillips, William D. (1989). "Atoms Laser-Cooled Below the Doppler-Cooling Limit". Frequency Standards and Metrology. Vol. 61. pp. 169–172. doi:10.1007/978-3-642-74501-0_45. ISBN 978-3-642-74503-4. {{cite book}}: |journal= ignored (help)
  4. ↑ Dalibard, J.; Cohen-Tannoudji, C. (November 1989). "Laser cooling below the Doppler limit by polarization gradients: simple theoretical models". JOSA B. 6 (11): 2023–2045. Bibcode:1989JOSAB...6.2023D. doi:10.1364/JOSAB.6.002023. We present two cooling mechanisms that lead to temperatures well below the Doppler limit. These mechanisms are based on laser polarization gradients and work at low laser power when the optical-pumping time between different ground-state sublevels becomes long.
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