(19), involves the exact energy and momentum eigenstates, the computation of which remains a com- plex, unsolved problem for spatial dimensionsd >1 and allu >0

Theu-unitary operator ˆVu that defines the quasiparticle operators ˜c† ⃗ rj ,σ = ˆV † u c† ⃗ rj ,σ ˆVu, ˜c⃗ rj ,σ = ˆV † u c⃗ rj ,σ ˆVu, Eq

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cond-mat.str-el · 2026-04-28 · unverdicted · novelty 7.0 · 2 refs

Seven exact theorems for the Hubbard model on bipartite lattices d>1 are established from the [SU(2)×SU(2)×U(1)]/Z₂² symmetry.

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Exact results for the Hubbard model on bipartite lattices in spatial dimensions $d>1$: Seven theorems from the full [SU(2)$\times$SU(2)$\times$U(1)]/$\mathbb{Z}_2^2$ symmetry cond-mat.str-el · 2026-04-28 · unverdicted · none · ref 6 · 2 links
Seven exact theorems for the Hubbard model on bipartite lattices d>1 are established from the [SU(2)×SU(2)×U(1)]/Z₂² symmetry.