Abstract
We demonstrate a versatile, state-dependent trapping scheme for the ground and first excited rotational states of ^{23}Na^{40}K molecules. Close to the rotational manifold of a narrow electronic transition, we determine tune-out frequencies where the polarizability of one state vanishes while the other remains finite, and a magic frequency where both states experience equal polarizability. The proximity of these frequencies of only 10GHz allows for dynamic switching between different trap configurations in a single experiment, while still maintaining sufficiently low scattering rates.
Highlights
Trapping potentials for ultracold atoms and molecules are based on spatially dependent energy shifts of their internal states produced by magnetic, electric, or optical fields
We extend these concepts to rotational states of ultracold polar molecules [19,20,21,22,23,24,25,26,27,28]
Such molecules offer unique possibilities for quantum engineering due to their strong long-range dipolar interactions and long single-particle lifetime [29,30,31,32,33]. Manipulating their rotational degrees of freedom is important for experimental control of dipolar interactions
Summary
Trapping potentials for ultracold atoms and molecules are based on spatially dependent energy shifts of their internal states produced by magnetic, electric, or optical fields. In far-detuned optical dipole traps, rotational magic conditions only exist at special light polarizations or intensities [3,41,42,43,44].
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