Abstract
Solving the Fermi–Hubbard model is a central task in the study of strongly correlated materials. Digital quantum computers can, in principle, be suitable for this purpose, but have so far been limited to quasi-one-dimensional models. This is because of exponential overheads caused by the interplay of noise and the non-locality of the mapping between fermions and qubits. Here we use a trapped-ion quantum computer to experimentally demonstrate that a recently developed local encoding can overcome this problem. In particular, we show that suitable reordering of terms and application of circuit identities—a scheme called corner hopping—substantially reduces the cost of simulating fermionic hopping. This enables the efficient preparation of the ground state of a 6 × 6 spinless Fermi–Hubbard model encoded in 48 physical qubits. We also develop two error mitigation schemes for systems with conserved quantities, based on local postselection and on extrapolation of local observables, respectively. Our results suggest that Fermi–Hubbard models beyond classical simulability can be addressed by digital quantum computers without large increases in gate fidelity.
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Data availability
The numerical data that support the findings of this study, including a full list of shots, are available via Zenodo at https://doi.org/10.5281/zenodo.13624900 (ref. 47). Source data are provided with this paper.
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Acknowledgements
This work was made possible by a large group of people, and we thank the entire Quantinuum team for their many contributions. We are grateful for helpful discussions with and feedback from M. Iqbal, G. Greene-Diniz and S.-H. Lin. E.G. acknowledges support by the Bavarian Ministry of Economic Affairs, Regional Development and Energy (StMWi) under project Bench-QC (grant no. DIK0425/01). K.H. and H.D. acknowledge support by the German Federal Ministry of Education and Research (BMBF) through the project EQUAHUMO (grant no. 13N16069) within the funding programme quantum technologies – from basic research to market. The bulk of the experimental data reported in this work, including all circuits described in Fig. 3, was produced by the Quantinuum H2-1 trapped-ion quantum computer, powered by Honeywell, on 10–14 June 2024.
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R.N. designed the adiabatic path, generated all circuits, carried out a large part of the data analysis and invented the local stabilizer filtering technique. K.H. performed many of the classical statevector and matrix product state calculations. S.M., D.G., P.S., M.M., T.G. and N.H. built the experiment and took the data. K.G., R.N. and K.H. made a library that was heavily used to automatically visualize and create circuits from fermionic encodings specified by edge and vertex operators. E.G. contributed to the theory of the stabilizer-based zero noise extrapolation as well as the visualization. R.N., K.H., K.G., E.G. and H.D. conceived the experimental design. H.D. contributed to the compilation scheme, data analysis and initial hypothesis and drafted the initial manuscript, to which all authors contributed.
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H.D. is a shareholder of Quantinuum. The other authors declare no competing interests.
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Supplementary Figs. 1–15, Discussion and Tables 1 and 2.
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Source Data Fig. 4
As requested, data for all panels in Fig. 4 merged in one file. Contains data for all panels with data, namely, Fig. 4b (Energy density vs number of Trotter layers on 4 × 4), 4c (Energy density vs number of Trotter layers on 6 × 6) and 4d (Signal attenuation vs system size).
Source Data Fig. 5
As requested, data for all panels in Fig. 5 merged in one file. Contains data for all panels with data, namely, Fig. 5a (Energy densities of initial and final states), 5b (Temperature corresponding to energy density in a), 5c (Charge-density correlations for the state created using Jordan–Wigner) and 5d (Charge-density correlations for the state created using the compact encoding).
Source Data Fig. 6
As requested, data for all panels in Fig. 6 merged in one file. Contains data for all panels with data, namely, Fig. 6e (The amount of noise on observables with different weight in the Jordan–Wigner encoding), 6f (The Coulomb energy density in the compact encoding with and without global filtering error mitigation) and 6g (Coulomb energy density output of different noise mitigation schemes and their associated retained bit rates).
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Nigmatullin, R., Hémery, K., Ghanem, K. et al. Experimental demonstration of breakeven for a compact fermionic encoding. Nat. Phys. 21, 1319–1325 (2025). https://doi.org/10.1038/s41567-025-02931-8
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DOI: https://doi.org/10.1038/s41567-025-02931-8