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Autori principali: Mayrhofer, R. David, Schoenzeit, Megan, Chubukov, Andrey V.
Natura: Preprint
Pubblicazione: 2025
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Accesso online:https://arxiv.org/abs/2507.16026
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author Mayrhofer, R. David
Schoenzeit, Megan
Chubukov, Andrey V.
author_facet Mayrhofer, R. David
Schoenzeit, Megan
Chubukov, Andrey V.
contents We present the results of a mean-field analysis of the temperature evolution of a ferromagnetic Stoner transition in a two-dimensional (2D) system with an isotropic dispersion $\varepsilon_k \propto k^{2α}$, which for $α>1$ models flat dispersions in various multi-layer graphene systems in a displacement field. This study is an extension to a finite $T$ of previous studies at $T=0$, which found both first-order and second-order Stoner transitions, depending on the value of $α$ and special behavior at $α=1$ and $α=2$. We find that the Stoner transition at a finite $T$ displays new features not seen at $T=0$. The most interesting one is the reentrant behavior, where the ordered state emerges as temperature is increased. This behavior develops at $α>1.4$ and the range where it holds increases with $α$. We conjecture that the reentrant behavior is the fundamental feature of the Stoner transition in 2D, not sensitive to the details of the electronic structure.
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institution arXiv
publishDate 2025
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spellingShingle Stoner Transition at Finite Temperature in a 2D Isotropic Fermi Liquid
Mayrhofer, R. David
Schoenzeit, Megan
Chubukov, Andrey V.
Strongly Correlated Electrons
We present the results of a mean-field analysis of the temperature evolution of a ferromagnetic Stoner transition in a two-dimensional (2D) system with an isotropic dispersion $\varepsilon_k \propto k^{2α}$, which for $α>1$ models flat dispersions in various multi-layer graphene systems in a displacement field. This study is an extension to a finite $T$ of previous studies at $T=0$, which found both first-order and second-order Stoner transitions, depending on the value of $α$ and special behavior at $α=1$ and $α=2$. We find that the Stoner transition at a finite $T$ displays new features not seen at $T=0$. The most interesting one is the reentrant behavior, where the ordered state emerges as temperature is increased. This behavior develops at $α>1.4$ and the range where it holds increases with $α$. We conjecture that the reentrant behavior is the fundamental feature of the Stoner transition in 2D, not sensitive to the details of the electronic structure.
title Stoner Transition at Finite Temperature in a 2D Isotropic Fermi Liquid
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2507.16026