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(2009)
31 A. K. Kolezhuk
K. Peeters (2011)
Group Theory for Physicists
(1999)
Nersesyan
We numerically study the quantum magnetism of ultracold alkali and alkaline-earth fermion systems with large hyperfine spin F = 3 2 , which are characterized by a generic S p ( N ) symmetry with N = 4 . The methods of exact diagonalization (ED) and density matrix renormalization group are employed for the large size one-dimensional (1D) systems, and the ED method is applied to a two-dimensional (2D) square lattice on small sizes. We focus on the magnetic exchange models in the Mott-insulating state at quarter-filling. Both 1D and 2D systems exhibit rich phase diagrams depending on the ratio between the spin exchanges J 0 and J 2 in the bond spin singlet and quintet channels, respectively. In one dimension, the ground states exhibit a long-range-ordered dimerization with a finite spin gap at J 0 / J 2 > 1 and a gapless spin-liquid state at J 0 / J 2 ⩽ 1 , respectively. In the former and latter cases, the correlation functions exhibit the two-site and four-site periodicities, respectively. In two-dimensions, various spin-correlation functions are calculated up to the size of 4 × 4 . The Néel-type spin correlation dominates at large values of J 0 / J 2 , while a 2 × 2 plaquette correlation is prominent at small values of this ratio. Between them, a columnar spin-Peierls dimerization correlation peaks. We infer the competition among the plaquette ordering, the dimer ordering, and the Néel ordering in the 2D system.
Physical Review B – American Physical Society (APS)
Published: Aug 1, 2011
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