163 research outputs found

    Photoassociative Production and Trapping of Ultracold KRb Molecules

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    We have produced ultracold heteronuclear KRb molecules by the process of photoassociation in a two-species magneto-optical trap. Following decay of the photoassociated KRb*, the molecules are detected using two-photon ionization and time-of-flight mass spectroscopy of KRb+^+. A portion of the metastable triplet molecules thus formed are magnetically trapped. Photoassociative spectra down to 91 cm−1^{-1} below the K(4ss) + Rb (5p1/2p_{1/2}) asymptote have been obtained. We have made assignments to all eight of the attractive Hund's case (c) KRb* potential curves in this spectral region.Comment: 4 pages, 4 figure

    Macrodimers: ultralong range Rydberg molecules

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    We study long range interactions between two Rydberg atoms and predict the existence of ultralong range Rydberg dimers with equilibrium distances of many thousand Bohr radii. We calculate the dispersion coefficients C5C_{5}, C6C_{6} and C8C_{8} for two rubidium atoms in the same excited level npnp, and find that they scale like n8n^{8}, n11n^{11} and n15n^{15}, respectively. We show that for certain molecular symmetries, these coefficients lead to long range potential wells that can support molecular bound levels. Such macrodimers would be very sensitive to their environment, and could probe weak interactions. We suggest experiments to detect these macrodimers.Comment: 4 pages, submitted to PR

    Enhancement of the formation of ultracold 85^{85}Rb2_2 molecules due to resonant coupling

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    We have studied the effect of resonant electronic state coupling on the formation of ultracold ground-state 85^{85}Rb2_2. Ultracold Rb2_2 molecules are formed by photoassociation (PA) to a coupled pair of 0u+0_u^+ states, 0u+(P1/2)0_u^+(P_{1/2}) and 0u+(P3/2)0_u^+(P_{3/2}), in the region below the 5S+5P1/25S+5P_{1/2} limit. Subsequent radiative decay produces high vibrational levels of the ground state, X1Σg+X ^1\Sigma_g^+. The population distribution of these XX state vibrational levels is monitored by resonance-enhanced two-photon ionization through the 21Σu+2 ^1\Sigma_u^+ state. We find that the populations of vibrational levels v′′v''=112−-116 are far larger than can be accounted for by the Franck-Condon factors for 0u+(P1/2)→X1Σg+0_u^+(P_{1/2}) \to X ^1\Sigma_g^+ transitions with the 0u+(P1/2)0_u^+(P_{1/2}) state treated as a single channel. Further, the ground-state molecule population exhibits oscillatory behavior as the PA laser is tuned through a succession of 0u+0_u^+ state vibrational levels. Both of these effects are explained by a new calculation of transition amplitudes that includes the resonant character of the spin-orbit coupling of the two 0u+0_u^+ states. The resulting enhancement of more deeply bound ground-state molecule formation will be useful for future experiments on ultracold molecules.Comment: 6 pages, 5 figures; corrected author lis

    Scattering length of the ground state Mg+Mg collision

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    We have constructed the X 1SIGMAg+ potential for the collision between two ground state Mg atoms and analyzed the effect of uncertainties in the shape of the potential on scattering properties at ultra-cold temperatures. This potential reproduces the experimental term values to 0.2 inverse cm and has a scattering length of +1.4(5) nm where the error is prodominantly due to the uncertainty in the dissociation energy and the C6 dispersion coefficient. A positive sign of the scattering length suggests that a Bose-Einstein condensate of ground state Mg atoms is stable.Comment: 15 pages, 3 figures, Submitted Phys. Rev.

    Photoassociation spectroscopy of cold He(2(3)S) atoms

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    We observe vibrational states by photoassociation spectroscopy of cold He(2 3S) atoms. Photoassociation resonances are detected as peaks in the Penning ionization rate over a frequency range of 20 GHz below the atomic 2 3S1-2 3P2 transition frequency. We have observed three vibrational series, of which two can be identified. A possible mechanism to explain the observed increase of the Penning ionization rate is discussed
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