Abstract In 1983, F. Duncan M. Haldane predicted a singlet ground state for isolated integer- spin one-dimensional antiferromagnets with low single-ion anisotropy D. Since then, a lot of …
We show how to perform exact diagonalizations of SU (N) Fermi-Hubbard models on L-site clusters separately in each irreducible representation (irrep) of SU (N). Using the …
K Wamer, M Lajkó, F Mila, I Affleck - Nuclear Physics B, 2020 - Elsevier
Abstract Recently, SU (3) chains in the symmetric and self-conjugate representations have been studied using field theory techniques. For certain representations, namely rank-p …
We provide numerical evidence of the Nagaoka's theorem in the SU (N) Fermi-Hubbard model on various cluster geometries, such as the square, the honeycomb, and the triangular …
We compute the dynamical spin structure factor S (k, ω) of the SU (3) Heisenberg chain variationally using a truncated Hilbert space spanned by the Gutzwiller projected particle …
H Su, Y Yao, A Furusaki - arXiv preprint arXiv:2406.05407, 2024 - arxiv.org
We show that the ground-state expectation value of twisting operator is a topological order parameter for $\text {U}(1) $-and $\mathbb {Z} _ {N} $-symmetric symmetry-protected …
We calculate the Haldane gap of the SU (3) spin [3 0 0] Heisenberg model using variational uniform fully symmetric SU (3) matrix product states, and find that the minimal gap Δ/J …
We numerically demonstrate that, although it is critical, the two-box symmetric SU (3) chain possesses edge states in the adjoint representation whose excitation energy scales with the …
T Botzung, P Nataf - arXiv preprint arXiv:2403.11588, 2024 - arxiv.org
We provide numerical evidence of the Nagaoka's theorem in the $\mathrm {SU}(N) $ Fermi- Hubbard model on various cluster geometries, such as the square, the honeycomb and the …