Laser Cooling and Trapping Lecture 1 Light Forces Lecture 2 Doppler

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Laser cooling and trapping Lecture 1 Light forces Lecture 2 Doppler cooling Lecture 3 Sub-Doppler cooling Lecture 4 Magneto-optical trap Evaporative cooling How cold? 100 K 1 mK 77 K Liquid N2 10 K 100 µK 4 K Liquid 4He Laser cooling 1 K 10 µK 1 µK 100 mK 30 mK Dilution Bose – Einstein 10 mk refrigerator 100 nK condensate (Record : 500 pK) (Very…) short history Sub-Doppler cooling Beam slowing 1982 1988 Sub-recoil cooling 1980 1985 1990 1997 Optical molasses 1975 Hänsch, Schalow Demhelt, Wineland 1980 S. Chu W. Phillips C. Cohen- Gordon, Ashkin Tannoudji Zeeman slowing Slowed atoms Initial distribution Phillips, PRL 48, p. 596 (1982) Crossed dipole trap – crystal of light Optical lattices 1 - d 2 - d 3 - d (M. Greiner) Optical tweezers: trapping in 3 D High field seekers ω < ω0 Gaussian beam ~ ~ α Diffraction limited optics w ~ λ Trapping volume ~ π λ3 NA = sin α Ex: 1 mW on 1 µm w ~ λ/NA Trap depth = 1 mK Detecting a single atom CCD 5 µm 12 8 4 counts / ms 0 0 5 10 15 20 25 time (sec) Institut d’Optique, France Guiding an atom laser Institut d’Optique, France Bouncing atoms on a surface Institut d’Optique, 1996 3D optical molasses Chu (1985) Laser cooling and Maxwell Boltzman distribution Lett et al., JOSA B 11, p. 2024 (1989) The results of Phillips et al. (1988) Time-of-flight measurement Doppler theory For Na, TD = 240 µK Lett, PRL 61, p. 169 (1988) Laser cooled atoms (2010) Laser cooled atoms (2010) Discovery of sub-Doppler cooling (1988) Time-of-flight measurement Doppler theory For Na, TD = 240 µK Lett, PRL 61, p. 169 (1988) Experimental verifications Salomon et al., Euro. Phys. Lett. 12, p. 683 (1990) Loading a MOT from a slowed beam Solenoid Imaging system Rb oven Slowing beam Oven Slowing Dilute atomic 200 m/s 200 m / s → ~ 1 m / s cloud Rb oven Zeeman slower 6 cooling beams Vacuum chamber 10-11mbar inside A MOT trap of sodium NIST, USA Double MOT system Gakushuin, Japan Loading from a 2D MOT Amsterdam, K. Dieckmann thesis (2001) Absorption imaging y x MIT I0 -n(x,y) σ L I(x,y) = I0 e Phase contrast imaging MIT .

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Direct Frequency Comb Laser Cooling and Trapping
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