Field-driven quantum phase transitions in spin chains
arXiv:1603.04359 · doi:10.1103/PhysRevB.95.174436
Abstract
We study the magnetization process of a 1D extended Heisenberg model, the - model, as a function of an external magnetic field. In this model, represents the traditional antiferromagnetic Heisenberg exchange and is the strength of a competing four-spin interaction. Without external field, this system hosts a twofold-degenerate dimerized (valence-bond solid) state above a critical value where . The dimer order is destroyed and replaced by a partially polarized translationally invariant state at a critical field value. We find magnetization jumps (metamagnetism) between the partially polarized and fully polarized state for , where we have calculated exactly. For two magnons (flipped spins on a fully polarized background) attract and form a bound state. Quantum Monte Carlo studies confirm that the bound state corresponds to the first step of an instability leading to a finite magnetization jump for . Our results show that neither geometric frustration nor spin-anisotropy are necessary conditions for metamagnetism. Working in the two-magnon subspace, we also find evidence pointing to the existence of metamagnetism in the unfrustrated - chain (, ), but only if is spin-anisotropic. We also investigate quantum-critical scaling near the transition into the fully polarized state for at . While the expected `zero-scale-factor' universality is clearly seen for and ; closer to we find that extremely low temperatures are required to observe the asymptotic behavior, due to the influence of the tricritical point at , which leads to a cross-over at a temperature between logarithmic tricritical scaling and zero-scale-factor universality, with when .
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