Abstract
Counterflow superfluidity is an anomalous quantum phase that was predicted two decades ago in the context of a two-component Bose–Hubbard model. In this phase, although both components exhibit fluidity, their correlated counterflow currents cancel each other out, resulting in the system behaving as an incompressible Mott insulator. However, realizing and identifying this phase experimentally has proven challenging due to the stringent requirements for a single set-up, including defect-free state preparation, minimal heating during coherent manipulations, and spin- and site-resolved detection of the phases. Here, we report on the observation of counterflow superfluidity in a binary Bose mixture in optical lattices. After preparing a low-entropy spin-Mott state by conveying two spin-1/2 bosonic atoms at every single lattice site to form a doublon, we adiabatically drove the system to the counterflow superfluid phase at approximately 1 nK. We observed features of antipair correlations through site- and spin-resolved quantum-gas microscopy in both real and momentum spaces. Finally, we measured long-range off-diagonal spin correlations in the rotated basis, revealing a correlation length approaching the system size. These techniques and observations demonstrated here provide accessibility to Borromean counterfluids.
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Data availability
All the data are available from the corresponding authors upon reasonable request. Source data are provided with this paper. The data are also available via figshare at https://doi.org/10.6084/m9.figshare.27084313 (ref. 64).
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Acknowledgements
We acknowledge fruitful discussions with L.-X. Liu and N. Prokof’ev. This work was supported by the National Natural Science Foundation of China (Grant No. 12125409), the Innovation Programme for Quantum Science and Technology (Grant No. 2021ZD0302004) and the Anhui Initiative in Quantum Information Technologies. Y.D. acknowledged funds from the National Natural Science Foundation of China (Grant No. 12275263), the Innovation Programme for Quantum Science and Technology (Grant No. 2021ZD0301900) and Natural Science Foundation of Fujian Province of China (Grant No. 2023J02032). Y.-G.Z. acknowledged the support of the Fundamental Research Funds for the Central Universities, the CPS-Huawei MindSpore Fellowship and the China Postdoctoral Science Foundation (Grant No. 2023TQ0102).
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Y.-G.Z., Z.-S.Y. and J.-W.P. conceived the research and designed the experiments. Y.-G.Z., A.L., Y.-C.S., M.-G.H., Z.-H.Z., Y.L., W.-Y.Z. and H.S. performed the experiments and collected the data. Y.-G.Z. and A.L. analysed the data. Y.D., Z.-S.Y. and J.-W.P. supervised the research. All authors participated in writing the manuscript.
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Extended data
Extended Data Fig. 1 Four-particle dynamics in double wells.
We prepared the atoms into \(\left\vert {S}_{z}=0\right\rangle\) state in an array of double wells by imposing the y long lattice. Then the y short lattice is quenched to 10Er to start the dynamics in double wells. The dashed line is a sinusoidal curve fitting from which we inferred the anisotropy u.
Extended Data Fig. 2 TOF measurement of the noise correlations.
a and b show the noise correlations in the spin-Mott and CSF phases, respectively. Purple circles indicate the noise correlation of the both atoms while blue circles are that of the \(\left\vert \downarrow \right\rangle\) atoms. The inter-component noise correlations (orange circles) are obtained from the relation g↑↓(δy) = [g(δy) − 2g↓↓(δy)]/2 + 1/4.
Extended Data Fig. 3 Full-count statistics of the local magnetization in the spin-Mott (left panel) and xy-ferromagnet phases.
The distributions of the magnetization are broadened due to the superexchange process in the xy-ferromagnet phase.
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Zheng, YG., Luo, A., Shen, YC. et al. Counterflow superfluidity in a two-component Mott insulator. Nat. Phys. 21, 208–213 (2025). https://doi.org/10.1038/s41567-024-02732-5
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DOI: https://doi.org/10.1038/s41567-024-02732-5