Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:cond-mat/0501600 · Physica A Statistical Mechanics and its Applications

Thermodynamics of the spin ladder as a composite chain model

Onofre Rojas, E.V. Corrêa Silva, S. M. de Souza, M. T. Thomaz

Published Jun 10, 2005• 2 citations
arXivHTMLPDF
DOI
10.1016/j.physa.2005.02.091

Related papers

Quantum compass model on a chain, ladder and finite square clusters

Wojciech Brzezicki, Adolfo Avella, Ferdinando Mancini

I show the exact solutions for the quantum compass model on a chain and ladder which are based on mapping to quantum Ising models in certain subspaces. I discuss the ground state and thermodynamic properties of both models. I show the spin transformation that maps L×L quantum compass model to (L−1)×(L−1) spin model and its applications to compass clusters of the sizes 4×4 and 5×5. I discuss the ground‐state and thermodynamic properties of these models.

AIP conference proceedings•Jan 1, 2010•2 citations

Thermodynamics of spin ladders

Matthias Troyer, Beat Frischmuth, Beat Ammon

APS•Mar 1, 1996•0 citations

Effect of an interchain magnetic interaction on the dimerized state of a two-XY-quantum-spin-chain ladder

Laurent Hubert, A. Caillé

The model that we study is a two-XY-quantum-spin-chain system with Ising interchain magnetic interaction. This model, referred to as the spin-ladder model, is used as a first step to model the thermodynamic properties of low-dimensional spin system. Similarities between the spin-ladder model and the one-dimensional Hubbard model are used in our analysis. As a consequence we can qualitatively understand the heat capacity and spin susceptibilty and show that both measurements are necessary to analyze a spin-ladder system. We also show that the strong-interchain-coupling limit of the spin-ladder model is equivalent to a one-chain spin Heisenberg Hamiltonian. Furthermore, the spin-Peierls transition is investigated for small (\ensuremath{\Vert}I/2J\ensuremath{\Vert}\ensuremath{\ll}1) and large (\ensuremath{\Vert}I/2J\ensuremath{\Vert}\ensuremath{\gg}1) interchain coupling, and we show its occurrence at relatively small spin-phonon coupling (\ensuremath{\lambda}\ensuremath{\lesssim}0.6). From the results obtained for the small- and large-interchain-interaction limits, we propose the conjecture that the in-phase dimerization persists for all values of the interaction parameter at zero temperature.

Physical review. B, Condensed matter•Jun 1, 1991•5 citations

Thermodynamic properties of a spin half ladder system

H. Y. Shik, Ru Chen

物理学前沿:英文版•May 22, 2010•0 citations

High-temperature expansion of the tetrahedral spin-1/2 and spin-2 XXZ models

Onofre Rojas, E.V. Corrêa Silva, S. M. de Souza +1 more

We apply the cummulant method to obtain the high-temperature expansion of the Helmholtz free energy of the tetrahedral spin-1/2 and spin-2 XXZ models. The tetrahedral model is written as a composite spin-1 XXZ model, and some of its thermodynamic functions are compared to those of the ordinary spin-1 XXZ model. The composite spin-1 model is then mapped onto a fermion model, and it is shown that the contribution of the string Hamiltonian to thermodynamic functions at high temperatures cannot be neglected. The high-temperature expansion of the Helmholtz free energy of the anisotropic spin-$2$ XXZ chain is obtained up to order ${\ensuremath{\beta}}^{6}.$ Our results fit well the numerical quantum Monte Carlo data calculated by Yamamoto [Phys. Rev. B 53, 3364 (1996)] for the isotropic antiferromagnetic Heisenberg chain. We complement his high-temperature expansions for thermodynamic functions with terms of higher order in $\ensuremath{\beta}.$

Physical Review B•Apr 5, 2004•9 citations

Thermodynamics of quantum spin chains

Alessandro Cuccoli, V. Tognetti, Ruggero Vaia +1 more

Springer eBooks•Apr 7, 2008•0 citations
The model that we study is a two-XY-quantum-spin-chain system with Ising interchain magnetic interaction. This model, referred to as the spin-ladder model, is used as a first step to model the thermodynamic properties of low-dimensional spin system. Similarities between the spin-ladder model and the one-dimensional Hubbard model are used in our analysis. As a consequence we can qualitatively understand the heat capacity and spin susceptibilty and show that both measurements are necessary to analyze a spin-ladder system. We also show that the strong-interchain-coupling limit of the spin-ladder model is equivalent to a one-chain spin Heisenberg Hamiltonian. Furthermore, the spin-Peierls transition is investigated for small (\ensuremath{\Vert}I/2J\ensuremath{\Vert}\ensuremath{\ll}1) and large (\ensuremath{\Vert}I/2J\ensuremath{\Vert}\ensuremath{\gg}1) interchain coupling, and we show its occurrence at relatively small spin-phonon coupling (\ensuremath{\lambda}\ensuremath{\lesssim}0.6). From the results obtained for the small- and large-interchain-interaction limits, we propose the conjecture that the in-phase dimerization persists for all values of the interaction parameter at zero temperature.
We apply the cummulant method to obtain the high-temperature expansion of the Helmholtz free energy of the tetrahedral spin-1/2 and spin-2 XXZ models. The tetrahedral model is written as a composite spin-1 XXZ model, and some of its thermodynamic functions are compared to those of the ordinary spin-1 XXZ model. The composite spin-1 model is then mapped onto a fermion model, and it is shown that the contribution of the string Hamiltonian to thermodynamic functions at high temperatures cannot be neglected. The high-temperature expansion of the Helmholtz free energy of the anisotropic spin-222 XXZ chain is obtained up to order ${\ensuremath{\beta}}^{6}.$ Our results fit well the numerical quantum Monte Carlo data calculated by Yamamoto [Phys. Rev. B 53, 3364 (1996)] for the isotropic antiferromagnetic Heisenberg chain. We complement his high-temperature expansions for thermodynamic functions with terms of higher order in $\ensuremath{\beta}.$