Abstract
We show that the lifetime of ultracold ground-state ^{87}Rb^{133}Cs molecules in an optical trap is limited by fast optical excitation of long-lived two-body collision complexes. We partially suppress this loss mechanism by applying square-wave modulation to the trap intensity, such that the molecules spend 75% of each modulation cycle in the dark. By varying the modulation frequency, we show that the lifetime of the collision complex is 0.53±0.06 ms in the dark. We find that the rate of optical excitation of the collision complex is 3_{-2}^{+4}×10^{3} W^{-1} cm^{2} s^{-1} for λ=1550 nm, leading to a lifetime of <100 ns for typical trap intensities. These results explain the two-body loss observed in experiments on nonreactive bialkali molecules.
Highlights
We show that the lifetime of ultracold ground-state 87Rb133Cs molecules in an optical trap is limited by fast optical excitation of long-lived two-body collision complexes
By varying the modulation frequency, we show that the lifetime of the collision complex is 0.53 Æ 0.06 ms in the dark
We find that the rate of optical excitation of the collision complex is 3þ−24 × 103 W−1 cm2 s−1 for λ 1⁄4 1550 nm, leading to a lifetime of < 100 ns for typical trap intensities
Summary
Loss of Ultracold 87Rb133Cs Molecules via Optical Excitation of Long-Lived Two-Body Collision Complexes We show that the lifetime of ultracold ground-state 87Rb133Cs molecules in an optical trap is limited by fast optical excitation of long-lived two-body collision complexes.
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