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Physical Review B

Quantum spherical spin model on the AB2 chain

M. H. Oliveira, Mauricio D. Coutinho-Filho, Ernesto P. Raposo

Published Dec 12, 2005• 9 citations
Publisher

Abstract

A quantum spherical spin model with an antiferromagnetic coupling $J$ on the $A{B}_{2}$ chain is studied, whose topology is of interest in the context of ferrimagnetic polymers and oxocuprates. A ferrimagnetic long-range order is found at the only critical point $g=T=h=0$, where $T$ denotes the temperature, $h$ the magnetic field, and $g$ the quantum coupling constant in energy units. The approach to the critical point, with diverging correlation length $\ensuremath{\xi}$ and cell susceptibility ${\ensuremath{\chi}}_{\text{cell}}$, is characterized through several paths in the ${g,T,h}$ parameter space: for $(T∕J)\ensuremath{\rightarrow}0$ and $g=h=0$, ${\ensuremath{\chi}}_{\text{cell}}\ensuremath{\sim}1∕{T}^{2}$, as also found in several classical and quantum spherical and Heisenberg models; for $(h∕J)\ensuremath{\rightarrow}0$ and $g=T=0$, ${\ensuremath{\chi}}_{\text{cell}}\ensuremath{\sim}1∕h$; and for $(g∕J)\ensuremath{\rightarrow}0$ and $T=h=0$, $\mathrm{ln}\phantom{\rule{0.2em}{0ex}}{\ensuremath{\chi}}_{\text{cell}}\ensuremath{\sim}1∕\sqrt{g}$, thus evidencing an essential singularity due to quantum fluctuations. In any path chosen the relation ${\ensuremath{\chi}}_{\text{cell}}\ensuremath{\sim}{\ensuremath{\xi}}^{2}$ is satisfied. For finite $g$ and $T$ a field-induced short-range ferrimagnetism occurs to some extent in the ${g,T,h}$ space, as confirmed by the analysis of the local spin averages, cell magnetization with a rapid increase for very low fields, and spin-spin correlation functions. The asymptotic limits of the correlation functions are also provided with respect to $g$, $T$, $h$, and spin distance. The analysis of the entropy and specific heat reveals that the quantum fluctuations fix the well-known drawback of classical spherical models concerning the third law of thermodynamics.

DOI
10.1103/physrevb.72.214420

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We present an extensive study of the AB2{\mathrm{AB}}_{2}AB2​ polymeric Hubbard chains with experimental motivation in inorganic and organic compounds. In the half-filled strong-coupling limit, these systems can be mapped onto a quantum antiferromagnetic spin-1/2AB21/2 {\mathrm{AB}}_{2}1/2AB2​ Heisenberg model that presents a zero-temperature quantum phase transition to a ferrimagnetic ground state. We derive the spin-wave modes with the same correct ferromagnetic dispersion relation calculated through two different techniques. We also build an Euclidean integral formulation in the coherent state representation which naturally gives rise to Wess-Zumino terms of topological origin. The low-energy infrared behavior of the AB2{\mathrm{AB}}_{2}AB2​ chains is properly described through a renormalization group analysis by the semiclassical fixed point of a one-dimensional quantum nonrelativistic nonlinear $\ensuremath{\sigma}$ model with critical dynamical exponent z=2.z=2.z=2. Their low-temperature behavior is shown to be the same of a quantum ferromagnetic spin-1/2 Heisenberg chain, as evidenced by the temperature dependence of the correlation length, susceptibility, and specific heat. On the other hand, a quantum critical fixed point is also found, with the same zero-temperature critical behavior of a classical Heisenberg system in D=d+z=3D=d+z=3D=d+z=3 dimensions. Its low-temperature critical properties are related to the latter through the crossover exponent $\ensuremath{\varphi}=z{\ensuremath{\nu}}_{3},$ where ${\ensuremath{\nu}}_{3}$ is the correlation length exponent of the D=3D=3D=3 classical Heisenberg model. Sufficiently strong quantum critical fluctuations destroy the ordered ground state of the quantum z=2z=2z=2 nonlinear $\ensuremath{\sigma}$ model (but not that of the quantum AB2{\mathrm{AB}}_{2}AB2​ Heisenberg spin systems, in agreement with a theorem by Lieb), giving rise to a quantum disordered phase at zero temperature. These results are supported by a connection between the quantum AB2{\mathrm{AB}}_{2}AB2​ Heisenberg and generalized quantum rotor models.
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