Abstract
We study the ground-state properties of the bond-alternating S=1/2 quantum spin chain whose Hamiltonian is H= ( + +λ) +βt⋅. When β=0, the ground state is a collection of local singlets with a finite excitation gap. In the limit of strong ferromagnetic coupling β→-∞, this is equivalent to the S=1 XXZ Hamiltonian. It has several ground-state phases in the λ-β plane including the Haldane phase which has a finite excitation gap above the ground. They are characterized by a full breakdown, partial breakdowns, and a nonbreakdown of the hidden discrete × symmetry. The ground-state phase diagram is obtained by series expansions.
- Received 22 February 1993
DOI:https://doi.org/10.1103/PhysRevB.48.9555
©1993 American Physical Society