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

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Summary

Introduction

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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Conclusion

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