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A numerical method for reconstructing the potential in fractional Calderón problem with a single measurement

Xinyan Li

Abstract

In this paper, we develop a numerical method for determining the potential in one and two dimensional fractional Calderón problems with a single measurement. Finite difference scheme is employed to discretize the fractional Laplacian, and the parameter reconstruction is formulated into a variational problem based on Tikhonov regularization to obtain a stable and accurate solution. Conjugate gradient method is utilized to solve the variational problem. Moreover, we also provide a suggestion to choose the regularization parameter. Numerical experiments are performed to illustrate the efficiency and effectiveness of the developed method and verify the theoretical results.

A numerical method for reconstructing the potential in fractional Calderón problem with a single measurement

Abstract

In this paper, we develop a numerical method for determining the potential in one and two dimensional fractional Calderón problems with a single measurement. Finite difference scheme is employed to discretize the fractional Laplacian, and the parameter reconstruction is formulated into a variational problem based on Tikhonov regularization to obtain a stable and accurate solution. Conjugate gradient method is utilized to solve the variational problem. Moreover, we also provide a suggestion to choose the regularization parameter. Numerical experiments are performed to illustrate the efficiency and effectiveness of the developed method and verify the theoretical results.
Paper Structure (9 sections, 4 theorems, 74 equations, 4 figures)

This paper contains 9 sections, 4 theorems, 74 equations, 4 figures.

Key Result

Lemma 2.1

GhoSal Let $n\geq1,s\in(0,1)$, $\Omega$ be a bounded open set and $q\in L^{\infty}(\Omega)$. Suppose that Assumption ass1 holds. Let Then for any $f\in H^s(\mathbb{R}^n)$ and $g\in (\tilde{H}^s(\Omega))^*$, there is a unique solution $u\in H^s(\mathbb{R}^n)$ in fseghosh satisfying Moreover, the norm estimate holds with $C$ independent of $g$ and $f$.

Figures (4)

  • Figure 1: The numerical results for Example 4.1 with different noise level $\delta$, (a) the reconstruction results $q_{\alpha}^{\delta}(x)$ and real solution $q(x)$; (b) the relationship between $|log(\delta)|^{-1}$ and $\|q_{\alpha}^{\delta}-q\|_{L^{\infty}(\Omega)}$.
  • Figure 2: The numerical results for Example 4.2 with different noise level $\delta$, (a) the reconstruction results $q_{\alpha}^{\delta}(x)$ and real solution $q(x)$; (b) the relationship between $|log(\delta)|^{-1}$ and $\|q_{\alpha}^{\delta}-q\|_{L^{\infty}(\Omega)}$.
  • Figure 3: The numerical results of estimated potential for Example 4.3 with noise level $\delta={\rm 1E-7}$ and regularization parameter $\alpha={\rm 1E-14}$ along with the real potential $q(x)$.
  • Figure 4: The numerical results of two-dimensional fraction Calderón problem for Example 4.4, (a) the real potential $q(x,y)$; (b) the reconstruction potential $q_{\alpha}^{\delta}(x,y)$ with $\delta$=1E-6,$\alpha$=1E-13; (c) the reconstruction error $|q_{\alpha}^{\delta}(x,y)-q(x,y)|$; (d) the relationship between $|log(\delta)|^{-1}$ and $\|q_{\alpha}^{\delta}-q\|_{L^{\infty}(\Omega)}$ with $\alpha=0.1\delta^2$.

Theorems & Definitions (11)

  • Lemma 2.1
  • Proposition 2.2
  • proof
  • Remark 2.1
  • Remark 2.2
  • Remark 3.1
  • Theorem 3.1
  • proof
  • Remark 3.2
  • Theorem 3.2
  • ...and 1 more