Decoupled phase of frustrated spin-1/2 antiferromagnetic chains with and without long range order in the ground state
arXiv:1309.7542 · doi:10.1103/PhysRevB.88.134412
Abstract
The quantum phases of one-dimensional spin chains are discussed for models with two parameters, frustrating exchange between second neighbors and normalized nonfrustrating power-law exchange with exponent and distance dependence . The ground state (GS) at has long-range order (LRO) for , long-range spin fluctuations for . The models conserve total spin , have singlet GS for any , and decouple at to linear Heisenberg antiferromagnets on sublattices and of odd and even-numbered sites. Exact diagonalization of finite chains gives the sublattice spin , the magnetic gap to the lowest triplet state and the excitation to the lowest singlet with opposite inversion symmetry to the GS. An analytical model that conserves sublattice spin has a first order quantum transition at from a GS with perfect LRO to a decoupled phase with for and no correlation between spins in different sublattices. The model with has a first order transition to a decoupled phase that closely resembles the analytical model. The bond order wave (BOW) phase and continuous quantum phase transitions of finite models with are discussed in terms of GS degeneracy where , excited state degeneracy where , and . The decoupled phase at large frustration has nondegenerate GS for any exponent and excited states related to sublattice excitations.
10 pages 8 figures
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- Matrix product state approach to a frustrated spin chain with long-range interactions
- Quantum phase diagram of a frustrated spin-1/2 system on a Trellis Ladder
- Frustrated spin-1/2 ladder with ferro- and antiferromagnetic legs
- Spin Peierls transition of and extended models with ferromagnetic .Sublattice dimerization and thermodynamics of zigzag chains in -TeVO