Universal low-temperature magnetic properties of the classical and quantum dimerized ferromagnetic spin chain

TL;DR

This paper demonstrates that low-temperature magnetic properties of classical and quantum dimerized ferromagnetic spin chains are equivalent to those of uniform chains with an effective exchange, extending known classical-quantum correspondence to dimerized systems.

Contribution

It shows that dimerization effectively reduces to a uniform chain with a modified exchange integral at low temperatures for both classical and quantum models.

Findings

Classical dimerized model reduces to a uniform model with effective exchange J(1-δ^2).

Quantum dimerized chain Hamiltonian reduces to that of a uniform chain in the long-wavelength limit.

Low-temperature magnetic properties of classical and quantum dimerized chains are equivalent.

Abstract

Low-temperature magnetic properties of both classical and quantum dimerized ferromagnetic spin chains are studied. It is shown that at low temperatures the classical dimerized model reduces to the classical uniform model with the effective exchange integral $J_{0}=J(1-\delta^{2})$, where $\delta$ is the dimerization parameter. The partition function and spin correlation function are calculated by means of mapping to the continuum limit, which is justified at low temperatures. In the continuum limit the calculation of the partition function and spin correlation function is reduced to the eigenvalue problem of quantum rotator in gravitational field. Quantum model is studied using Dyson-Maleev representation of the spin operators. It is shown that in the long-wavelength limit the Hamiltonian of the quantum dimerized chain reduces to that of the uniform ferromagnetic chain with the effective exchange integral $J_{0}=J(1-\delta^{2})$. This fact implies that the known equivalence of the low-temperature magnetic properties of classical and quantum ferromagnetic chains remains for the dimerized chains. The considered model can be generalized to include the next-neighbor antiferromagnetic interaction.