Citation for published item:wolonyD eter uF nd qregoryD hilip hF nd tiD honghu nd vuD fo nd u¤ oppingerD wi h el F nd ve ueurD gF uth nd fl kleyD g roline vF nd rutsonD teremy wF nd gornishD imon vF @PHIRA 9gre tion of ultr old VU IQQgs mole ules in the rovi r tion l ground st teF9D hysi l review lettersFD IIQ @PSAF pF PSSQHIF Further information on publisher's website:httpXGGdxFdoiForgGIHFIIHQG hys evvettFIIQFPSSQHI Publisher's copyright statement:Reprinted with permission from the American Physical Society: Physical Review Letters 113, 255301 c 2014 by the American Physical Society. Readers may view, browse, and/or download material for temporary copying purposes only, provided these uses are for noncommercial personal purposes. Except as provided by law, this material may not be further reproduced, distributed, transmitted, modi ed, adapted, performed, displayed, published, or sold in whole or part, without prior written permission from the American Physical Society.Additional information: Use policyThe full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-pro t purposes provided that:• a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders.Please consult the full DRO policy for further details. We report the creation of a sample of over 1000 ultracold 87 Rb 133 Cs molecules in the lowest rovibrational ground state, from an atomic mixture of 87 Rb and 133 Cs, by magnetoassociation on an interspecies Feshbach resonance followed by stimulated Raman adiabatic passage (STIRAP). We measure the binding energy of the RbCs molecule to be hc × 3811.576ð1Þ cm −1 and the jv 00 ¼ 0; J 00 ¼ 0i to jv 00 ¼ 0; J 00 ¼ 2i splitting to be h × 2940.09ð6Þ MHz. Stark spectroscopy of the rovibrational ground state yields an electric dipole moment of 1.225(3)(8) D, where the values in parentheses are the statistical and systematic uncertainties, respectively. We can access a space-fixed dipole moment of 0.355(2)(4) D, which is substantially higher than in previous work.
We report the successful production of an ultracold sample of absolute ground-state ^{23}Na^{87}Rb molecules. Starting from weakly bound Feshbach molecules formed via magnetoassociation, the lowest rovibrational and hyperfine level of the electronic ground state is populated following a high-efficiency and high-resolution two-photon Raman process. The high-purity absolute ground-state samples have up to 8000 molecules and densities of over 10^{11} cm^{-3}. By measuring the Stark shifts induced by external electric fields, we determined the permanent electric dipole moment of the absolute ground-state ^{23}Na^{87}Rb and demonstrated the capability of inducing an effective dipole moment over 1 D. Bimolecular reaction between ground-state ^{23}Na^{87}Rb molecules is endothermic, but we still observed a rather fast decay of the molecular sample. Our results pave the way toward investigation of ultracold molecular collisions in a fully controlled manner and possibly to quantum gases of ultracold bosonic molecules with strong dipolar interactions.
A simple, versatile laser system for the creation of ultracold ground state molecules Here we describe how a relatively simple apparatus consisting of a single fixed-length optical cavity can be used to narrow the linewidth of the two different wavelength lasers required for STIRAP simultaneously. The frequency of each of these lasers is referenced to the cavity and is continuously tunable away from the cavity modes through the use of non-resonant electro-optic modulators. Selfheterodyne measurements suggest the laser linewidths are reduced to several 100 Hz. In the context of 87 Rb 133 Cs molecules produced via magnetoassociation on a Feshbach resonance, we demonstrate the performance of the laser system through one-and two-photon molecular spectroscopy. Finally, we demonstrate transfer of the molecules to the rovibrational ground state using STIRAP.
Spin cat states are promising candidates for quantum-enhanced measurement. Here, we analytically show that the ultimate measurement precision of spin cat states approaches the Heisenberg limit, where the uncertainty is inversely proportional to the total particle number. In order to fully exploit their metrological ability, we propose to use the interaction-based readout for implementing phase estimation. It is demonstrated that the interaction-based readout enables spin cat states to saturate their ultimate precision bounds. The interaction-based readout comprises a one-axis twisting, two π 2 pulses, and a population measurement, which can be realized via current experimental techniques. Compared with the twisting echo scheme on spin squeezed states, our scheme with spin cat states is more robust against detection noise. Our scheme may pave an experimentally feasible way to achieve Heisenberg-limited metrology with non-Gaussian entangled states. and its derivative with respect to φ reads as,Correspondingly, the standard deviation of halfpopulation difference isFinally, we can obtain the phase measurement precision via Eqs. (26) and (27),.(28) When φ = 0, sin(2kφ) = 0 and cos(2kφ) = 1, the phase measurement precision becomesWhen φ = π/2, sin(2kφ) = 0 and (−1) J−k cos(2kφ) = 1, the phase measurement precision can be simplified as ∆φ| φ=π/2 = J k=−J k 2 |a k | 2 J k=−J 2k 2 |a k | 2
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