Weak Mean Attractors and Invariant Measures of Fractional Stochastic Delay FitzHugh-Nagumo Systems on RN

This article is devoted to the study of mean attractors and invariant measures for the fractional stochastic FitzHugh-Nagumo systems on <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:math> with locally Lipschitz noise. When the diffusion coefficients are locally Lipschitz, we establish the global-in-time well-posedness and the existence of Itô’s energy equalities for the stochastic systems. In addition, we establish the existence and uniqueness of weak pullback mean random attractors of the mean random dynamical systems generated by the solution operators in the product Bochner space: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="block" overflow="scroll"> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>,</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mrow> <mml:mo maxsize="1.2em" minsize="1.2em">(</mml:mo> </mml:mrow> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>;</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mo stretchy="false">(</mml:mo> <mml:mo>−</mml:mo> <mml:mi>ρ</mml:mi> <mml:mo>,</mml:mo> <mml:mn>0</mml:mn> <mml:mo stretchy="false">)</mml:mo> <mml:mo>;</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo stretchy="false">)</mml:mo> <mml:mrow> <mml:mo maxsize="1.2em" minsize="1.2em">)</mml:mo> </mml:mrow> </mml:math> over the complete filtered probability space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mo stretchy="false">(</mml:mo> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>,</mml:mo> <mml:mo fence="false" stretchy="false">{</mml:mo> <mml:msub> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mi>t</mml:mi> </mml:msub> <mml:msub> <mml:mo fence="false" stretchy="false">}</mml:mo> <mml:mrow> <mml:mi>t</mml:mi> <mml:mo>∈</mml:mo> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> </mml:mrow> </mml:msub> <mml:mo>,</mml:mo> <mml:mi>P</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> , where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mi>ρ</mml:mi> <mml:mo>≥</mml:mo> <mml:mn>0</mml:mn> </mml:math> is the time-delay parameter. When the diffusion and drift terms are globally Lipschitz continuous, we address the existence, uniqueness and exponentially mixing of invariant measures for the autonomous stochastic FitzHugh-Nagumo systems on <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:math> under a large damping condition. This work deepens and extends the results of Wang, Guo and Wang (Science China Mathematics, 64 (11): 2395–2436, 2021).

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Journal
Asymptotic Analysis
Published
2025-03-19
DOI
https://doi.org/10.1177/09217134251317875
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1
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Stability and Controllability of Differential Equations
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article

Weak Mean Attractors and Invariant Measures of Fractional Stochastic Delay FitzHugh-Nagumo Systems on RN

Shuang Wu, Xiaolan Qin, Hailang Bai, Dexin Li
1 citations
Asymptotic Analysis
Stability and Controllability of Differential Equations
1.21
article

Weak Mean Attractors and Invariant Measures of Fractional Stochastic Delay FitzHugh-Nagumo Systems on RN

Shuang Wu, Xiaolan Qin, Hailang Bai, Dexin Li
article en
1 citations

Abstract

This article is devoted to the study of mean attractors and invariant measures for the fractional stochastic FitzHugh-Nagumo systems on <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:math> with locally Lipschitz noise. When the diffusion coefficients are locally Lipschitz, we establish the global-in-time well-posedness and the existence of Itô’s energy equalities for the stochastic systems. In addition, we establish the existence and uniqueness of weak pullback mean random attractors of the mean random dynamical systems generated by the solution operators in the product Bochner space: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="block" overflow="scroll"> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>,</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mrow> <mml:mo maxsize="1.2em" minsize="1.2em">(</mml:mo> </mml:mrow> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>;</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mo stretchy="false">(</mml:mo> <mml:mo>−</mml:mo> <mml:mi>ρ</mml:mi> <mml:mo>,</mml:mo> <mml:mn>0</mml:mn> <mml:mo stretchy="false">)</mml:mo> <mml:mo>;</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo>×</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> <mml:mo stretchy="false">)</mml:mo> <mml:mrow> <mml:mo maxsize="1.2em" minsize="1.2em">)</mml:mo> </mml:mrow> </mml:math> over the complete filtered probability space <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mo stretchy="false">(</mml:mo> <mml:mi mathvariant="normal">Ω</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mo>,</mml:mo> <mml:mo fence="false" stretchy="false">{</mml:mo> <mml:msub> <mml:mrow> <mml:mi mathvariant="script">F</mml:mi> </mml:mrow> <mml:mi>t</mml:mi> </mml:msub> <mml:msub> <mml:mo fence="false" stretchy="false">}</mml:mo> <mml:mrow> <mml:mi>t</mml:mi> <mml:mo>∈</mml:mo> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> </mml:mrow> </mml:msub> <mml:mo>,</mml:mo> <mml:mi>P</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> , where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mi>ρ</mml:mi> <mml:mo>≥</mml:mo> <mml:mn>0</mml:mn> </mml:math> is the time-delay parameter. When the diffusion and drift terms are globally Lipschitz continuous, we address the existence, uniqueness and exponentially mixing of invariant measures for the autonomous stochastic FitzHugh-Nagumo systems on <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mi>N</mml:mi> </mml:msup> </mml:math> under a large damping condition. This work deepens and extends the results of Wang, Guo and Wang (Science China Mathematics, 64 (11): 2395–2436, 2021).

Asymptotic AnalysisVol. 142(3)
Guizhou Normal University (CN), Guangxi Minzu University (CN)
Openalex Percentile: Top 24%
Stability and Controllability of Differential Equations
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