PreprintCC BY 4.0arXiv
Stability of Magnetizable Piezoelectric Beam Systems with Two Fractional Infinite Memory Terms
Abstract
In this paper, we investigate a class of magnetizable piezoelectric beam systems with two fractional infinite memory terms, whose fractional orders are denoted by θ1, θ2 ∈ [0,1]. By introducing the Dafermos history variable, we construct an augmented state space and reformulate the system as an abstract evolution equation. The well-posedness of the system is established via semigroup theory. Through a frequency-domain analysis, we characterize the asymptotic behavior of the solutions. We show that the system is exponentially stable if θ1 = θ2 = 1, and is polynomially stable in all other cases, with the explicit decay rate t−1/(2−2θ0), where θ0 = min{θ1, θ2}. Furthermore, the optimality of the obtained decay rate is verified.
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BibTeX
@misc{zhou2026stability,
title = {{Stability of Magnetizable Piezoelectric Beam Systems with Two Fractional Infinite Memory Terms}},
author = {Jun Zhou and Linfeng Duan},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.06049},
eprint = {2609.06049},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.06049},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Stability of Magnetizable Piezoelectric Beam Systems with Two Fractional Infinite Memory Terms
AU - Jun Zhou
AU - Linfeng Duan
PY - 2026
DA - 2026/09/05
PB - arXiv
DO - 10.48550/arxiv.2609.06049
UR - https://arxiv.org/abs/2609.06049
AB - In this paper, we investigate a class of magnetizable piezoelectric beam systems with two fractional infinite memory terms, whose fractional orders are denoted by θ_1, θ_2 ∈ [0,1]. By introducing the Dafermos history variable, we construct an augmented state space and reformulate the system as an abstract evolution equation. The well-posedness of the system is established via semigroup theory. Through a frequency-domain analysis, we characterize the asymptotic behavior of the solutions. We show that the system is exponentially stable if θ_1 = θ_2 = 1, and is polynomially stable in all other cases, with the explicit decay rate t^−1/(2−2θ_0), where θ_0 = min{θ_1, θ_2}. Furthermore, the optimality of the obtained decay rate is verified.
ER -