Spin parity and broken symmetry in finite spin-1/2 chains with frustrated exchange: quantum transition from high to low spin
Abstract
Exact diagonalization of finite spin-1/2 chains with periodic boundary conditions is applied to the ground state (gs) of chains with ferromagnetic (F) exchange J1 < 0between first neighbors, antiferromagnetic (AF) exchange J2 = α J1 > 0between second neighbors, and axial anisotropy 0 1. In zero field, the gs is in the Sz = 0 sector for the relevant parameters and is doubly degenerate at multiple points γm = (αm, m) in the α, plane. Degeneracy under inversion at sites or spin parity or both leads, respectively, to a bond order wave (BOW), to staggered magnetization or to vector chiral (VC) order. Exact results up to N = 28 spins directly yield order parameters and spin correlation functions whose weak N dependencies allow inferences about infinite chains. The high-spin gs at J2 = 0 changes discontinuously at γ1 = (-1/4, 1) to a singlet in the isotropic ( = 1) chain. The transition from high to low spin S(α, ) is continuous for < B = 0.95 0.01 on the degeneracy line α1(). The gs has staggered magnetization between A = 0.72 and B, and a BOW for < A. When both inversion and spin parity are reversed at γm, the correlation functions C(p) for spins separated by p sites are identical. C(p) minima are shifted by π/2 from the minima of VC order parameters at separation p, consistent with right and left-handed helices along the z axis and spins in the xy plane. Degenerate gs of finite chains are related to quantum phase diagrams of extended α, chains, with good agreement for order parameters along the line α1().
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