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. 2021 Jul 23;12:4490. doi: 10.1038/s41467-021-24726-0

Fig. 1. Illustration of the experimental setup and the structure of the Hilbert space.

Fig. 1

a Schematic of the tilted 1D Fermi-Hubbard model (with odd o and even e sites) with tunneling J, on-site interaction U and spin-dependent tilt Δ, Δ (spin-up red, spin-down blue). b Dominant resonant tunneling processes for different regimes. c Finite-time connectivity Cϵ (for a cut-off ϵ = 10%) defined as the fraction of states that participate in the dynamics up to an evolution time TN=1000τ (main text, “Methods”). The calculation was performed for a Néel-ordered singlon CDW initial state, using exact diagonalization (ED) with system size L = 13 and Δ = Δ ≡ Δ. In the large-tilt limit, Δ/J → , we find emergent strongly-fragmented effective Hamiltonians for regime ① and ② (see Supplementary Note 3 and 4).