Inversion Phenomena of the Anisotropies of the Hamiltonian and the Wave-Function in the Distorted Diamond Type Spin Chain
arXiv:cond-mat/0108528 · doi:10.1016/S0022-3697(02)00070-7
Abstract
We investigate the ground-sate phase diagram of the XXZ version of the S=1/2 distorted diamond chain by use of the degenerate perturbation theory near the truncation point. In case of the XY-like interaction anisotropy, the phase diagram consists of the Neel phase and the spin-fluid phase. For the Ising-like interaction anisotropy case, it consists of three phases: the ferrimagnetic phase, the Neel phase and the spin-fluid phase. The magnetization in the ferrimagnetic phase is 1/3 of the saturation magnetization. The remarkable nature of the phase diagram is the existence of the Neel phase, although the interaction anisotropy is XY-like. And also, the spin-fluid phase appears in spite of the Ising-like interaction anisotropy. We call these regions "inversion regions".
7 pages, 4 figures
References in corpus (1)
Cited by in corpus (11)
- Geometric frustration in the class of exactly solvable Ising-Heisenberg diamond chains
- Phase diagram of the asymmetric tetrahedral Ising-Heisenberg chain
- Unconventional Neel and dimer orders in a spin-1/2 frustrated ferromagnetic chain with easy-plane anisotropy
- Spin Frustration in an Exactly Solvable Ising-Heisenberg Diamond Chain
- Inversion phenomenon and phase diagram of the distorted diamond chain with the interaction anisotropy
- Ground-State Phase Diagram of an Anisotropic S=1/2 Ladder with Different Leg Interactions
- Frustrated S=1/2 Two-Leg Ladder with Different Leg Interactions
- Navigating the phase diagram of quantum many-body systems in phase space
- Coupled Cluster Treatment of the Alternating Bond Diamond Chain
- Magnetization Plateau of the Distorted Diamond Spin Chain
- Ground-State Phase Diagram of (1/2,1/2,1) Mixed Diamond Chains with Single-Site Anisotropy