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Sisyphus Cooling Justin M. Brown November 8, 2007
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Sisyphus Effect Jean Dalibard and Claude Cohen-Tannoudji (1989) Model to describe sub-Doppler cooling Real atoms have more than two levels Atoms always travel up a hill to decrease KE
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Sub-Doppler Cooling Doppler Limit Consider Atomic Zeeman Structure Approach Recoil Limit
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Polarization Gradient Counter-propagating perpendicular linear polarizations Polarization Gradient from lightshifts
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Lightshifts
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Limitations Must Doppler cool first! –Only works over narrow range of velocities –Traveling over multiple potential hills averages out Doesn’t work if KE > U hill Detune laser further and reduce intensity Cannot break recoil limit – always emit photon
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Experimental Implementation Miller, K. W., Durr, S, and Weinman, C. Rf-induced Sisyphus cooling in an optical trap. Phys. Rev. A, 66(023406), August 2002. 87-Rubidium in an optical dipole trap Circular polarization pumps to end state
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Experimental Implementation Miller, K. W., Durr, S, and Weinman, C. Rf-induced Sisyphus cooling in an optical trap. Phys. Rev. A, 66(023406), August 2002.
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