<p>This paper addresses the regional boundary observability of linear time-fractional systems characterized by the Hilfer fractional derivative of order <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha \in ]0,1[,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">]</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">[</mo> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> with type <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(0 \le \beta \le 1.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≤</mo> <mi>β</mi> <mo>≤</mo> <mn>1</mn> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> The primary objective is to reconstruct the initial state of the system within a subregion <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\( \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> of the boundary <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\( \partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> of the evolution domain <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\( \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation>. To achieve this, we establish the connection between regional boundary observability on <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\( \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> and regional observability in a suitable subregion <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\( \omega _\texttt{r} \subset \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ω</mi> <mi mathvariant="monospace">r</mi> </msub> <mo>⊂</mo> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation>, defined such that <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\( \Gamma \subset \partial \omega _\texttt{r} \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Γ</mi> <mo>⊂</mo> <mi>∂</mi> <msub> <mi>ω</mi> <mi mathvariant="monospace">r</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. This method enables the recovery of the initial state within the subregion <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\( \omega _\texttt{r} \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ω</mi> <mi mathvariant="monospace">r</mi> </msub> </math></EquationSource> </InlineEquation> by utilizing an extended version of the Hilbert Uniqueness Method (HUM) tailored for fractional systems. Following this, the trace on <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\( \partial \omega _\texttt{r} \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <msub> <mi>ω</mi> <mi mathvariant="monospace">r</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> is restricted to <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\( \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>, allowing the determination of the initial state on <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\( \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>. We also propose an algorithm to recover the initial state in <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\( \omega _\texttt{r} \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ω</mi> <mi mathvariant="monospace">r</mi> </msub> </math></EquationSource> </InlineEquation> and ultimately on <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\( \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>, achieving a satisfactory reconstruction error. Notably, the reconstruction error associated with the initial state is remarkably low, affirming the efficacy of the approach employed in this investigation.</p>

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Regional boundary observability of time-fractional systems with Hilfer derivatives of order \(\alpha \) and type \(\beta \)

  • Hamza Ben Brahim,
  • Khalid Zguaid,
  • Fatima-Zahrae El Alaoui

摘要

This paper addresses the regional boundary observability of linear time-fractional systems characterized by the Hilfer fractional derivative of order \(\alpha \in ]0,1[,\) α ] 0 , 1 [ , with type \(0 \le \beta \le 1.\) 0 β 1 . The primary objective is to reconstruct the initial state of the system within a subregion \( \Gamma \) Γ of the boundary \( \partial \Omega \) Ω of the evolution domain \( \Omega \) Ω . To achieve this, we establish the connection between regional boundary observability on \( \Gamma \) Γ and regional observability in a suitable subregion \( \omega _\texttt{r} \subset \Omega \) ω r Ω , defined such that \( \Gamma \subset \partial \omega _\texttt{r} \) Γ ω r . This method enables the recovery of the initial state within the subregion \( \omega _\texttt{r} \) ω r by utilizing an extended version of the Hilbert Uniqueness Method (HUM) tailored for fractional systems. Following this, the trace on \( \partial \omega _\texttt{r} \) ω r is restricted to \( \Gamma \) Γ , allowing the determination of the initial state on \( \Gamma \) Γ . We also propose an algorithm to recover the initial state in \( \omega _\texttt{r} \) ω r and ultimately on \( \Gamma \) Γ , achieving a satisfactory reconstruction error. Notably, the reconstruction error associated with the initial state is remarkably low, affirming the efficacy of the approach employed in this investigation.