Micromagnetic simulations of the size dependence of the Curie temperature in ferromagnetic nanowires and nanolayers

We solve the Landau-Lifshitz-Gilbert equation in the finite-temperature regime, where thermal fluctuations are modeled by a random magnetic field whose variance is proportional to the temperature. By rescaling the temperature proportionally to the computational cell size Δx (T→TΔx/aeff, where aeff i...

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Published inJournal of magnetism and magnetic materials Vol. 598; p. 172040
Main Authors Courtès, Clémentine, Boileau, Matthieu, Côte, Raphaël, Hervieux, Paul-Antoine, Manfredi, Giovanni
Format Journal Article
LanguageEnglish
Published Elsevier B.V 15.05.2024
Elsevier
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Online AccessGet full text
ISSN0304-8853
1873-4766
1873-4766
DOI10.1016/j.jmmm.2024.172040

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Abstract We solve the Landau-Lifshitz-Gilbert equation in the finite-temperature regime, where thermal fluctuations are modeled by a random magnetic field whose variance is proportional to the temperature. By rescaling the temperature proportionally to the computational cell size Δx (T→TΔx/aeff, where aeff is the lattice constant) [M. B. Hahn, J. Phys. Comm., 3:075009, 2019], we obtain Curie temperatures TC that are in line with the experimental values for cobalt, iron and nickel. For finite-sized objects such as nanowires (1D) and nanolayers (2D), the Curie temperature varies with the smallest size d of the system. We show that the difference between the computed finite-size TC and the bulk TC follows a power-law of the type: (ξ0/d)λ, where ξ0 is the correlation length at zero temperature, and λ is a critical exponent. We obtain values of ξ0 in the nanometer range, also in accordance with other simulations and experiments. The computed critical exponent is close to λ=2 for all considered materials and geometries. This is the expected result for a mean-field approach, but slightly larger than the values observed experimentally. •Simulation of temperature effects using a stochastic Landau-Lifshitz-Gilbert equation.•Accurate determination of the Curie temperature for Cobalt, Nickel, and Iron.•Determination of the scaling law of the Curie temperature with the size of the system, for nanowire and nanolayer geometries.
AbstractList We solve the Landau-Lifshitz-Gilbert equation in the finite-temperature regime, where thermal fluctuations are modeled by a random magnetic field whose variance is proportional to the temperature. By rescaling the temperature proportionally to the computational cell size ∆x (T → T ∆x/a_{eff} , where a eff is the lattice constant) [M. B. Hahn, J. Phys. Comm., 3:075009, 2019], we obtain Curie temperatures T_C that are in line with the experimental values for cobalt, iron and nickel. For finite-sized objects such as nanowires (1D) and nanolayers (2D), the Curie temperature varies with the smallest size d of the system. We show that the difference between the computed finite-size T_C and the bulk T_C follows a power-law of the type: (ξ_0 /d)^{λ} , where ξ_0 is the correlation length at zero temperature, and λ is a critical exponent. We obtain values of ξ_0 in the nanometer range, also in accordance with other simulations and experiments. The computed critical exponent is close to λ = 2 for all considered materials and geometries. This is the expected result for a mean-field approach, but slightly larger than the values observed experimentally.
We solve the Landau-Lifshitz-Gilbert equation in the finite-temperature regime, where thermal fluctuations are modeled by a random magnetic field whose variance is proportional to the temperature. By rescaling the temperature proportionally to the computational cell size Δx (T→TΔx/aeff, where aeff is the lattice constant) [M. B. Hahn, J. Phys. Comm., 3:075009, 2019], we obtain Curie temperatures TC that are in line with the experimental values for cobalt, iron and nickel. For finite-sized objects such as nanowires (1D) and nanolayers (2D), the Curie temperature varies with the smallest size d of the system. We show that the difference between the computed finite-size TC and the bulk TC follows a power-law of the type: (ξ0/d)λ, where ξ0 is the correlation length at zero temperature, and λ is a critical exponent. We obtain values of ξ0 in the nanometer range, also in accordance with other simulations and experiments. The computed critical exponent is close to λ=2 for all considered materials and geometries. This is the expected result for a mean-field approach, but slightly larger than the values observed experimentally. •Simulation of temperature effects using a stochastic Landau-Lifshitz-Gilbert equation.•Accurate determination of the Curie temperature for Cobalt, Nickel, and Iron.•Determination of the scaling law of the Curie temperature with the size of the system, for nanowire and nanolayer geometries.
ArticleNumber 172040
Author Boileau, Matthieu
Hervieux, Paul-Antoine
Côte, Raphaël
Manfredi, Giovanni
Courtès, Clémentine
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  surname: Manfredi
  fullname: Manfredi, Giovanni
  email: giovanni.manfredi@ipcms.unistra.fr
  organization: University of Strasbourg, CNRS, IPCMS, UMR 7504, F-67000 Strasbourg, France
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Keywords Nanowire
Micromagnetism
Landau-Lifshitz-Gilbert equation
Finite-size effect
Nanolayer
Curie temperature
Finite-size effects
Language English
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Snippet We solve the Landau-Lifshitz-Gilbert equation in the finite-temperature regime, where thermal fluctuations are modeled by a random magnetic field whose...
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SubjectTerms Condensed Matter
Curie temperature
Finite-size effect
Landau-Lifshitz-Gilbert equation
Mathematics
Micromagnetism
Nanolayer
Nanowire
Numerical Analysis
Physics
Strongly Correlated Electrons
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Title Micromagnetic simulations of the size dependence of the Curie temperature in ferromagnetic nanowires and nanolayers
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