Ultracold field-linked tetratomic molecules.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 38297128.
- Also identified by DOI 10.1038/s41586-023-06986-6 and PMC identifier 10849947.
- Licence recorded as CC BY.
- The licence permits redistribution, so the abstract is shown in full and the full text is available from the publisher.
Abstract
Ultracold polyatomic molecules offer opportunities<sup>1</sup> in cold chemistry<sup>2,3</sup>, precision measurements<sup>4</sup> and quantum information processing<sup>5,6</sup>, because of their rich internal structure. However, their increased complexity compared with diatomic molecules presents a challenge in using conventional cooling techniques. Here we demonstrate an approach to create weakly bound ultracold polyatomic molecules by electroassociation<sup>7</sup> (F.D. et al., manuscript in preparation) in a degenerate Fermi gas of microwave-dressed polar molecules through a field-linked resonance<sup>8-11</sup>. Starting from ground-state NaK molecules, we create around 1.1 × 10<sup>3</sup> weakly bound tetratomic (NaK)<sub>2</sub> molecules, with a phase space density of 0.040(3) at a temperature of 134(3) nK, more than 3,000 times colder than previously realized tetratomic molecules<sup>12</sup>. We observe a maximum tetramer lifetime of 8(2) ms in free space without a notable change in the presence of an optical dipole trap, indicating that these tetramers are collisionally stable. Moreover, we directly image the dissociated tetramers through microwave-field modulation to probe the anisotropy of their wavefunction in momentum space. Our result demonstrates a universal tool for assembling weakly bound ultracold polyatomic molecules from smaller polar molecules, which is a crucial step towards Bose-Einstein condensation of polyatomic molecules and towards a new crossover from a dipolar Bardeen-Cooper-Schrieffer superfluid<sup>13-15</sup> to a Bose-Einstein condensation of tetramers. Moreover, the long-lived field-linked state provides an ideal starting point for deterministic optical transfer to deeply bound tetramer states<sup>16-18</sup>.