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Let $\mathscr P:=\{\nabla p\,|\,\,p\in H^1(\Omega)\}$ be the space of the potential vector fields, and let $\mathscr L_\lambda:=\{\varkappa\nabla\tau\,|\,\,\varkappa\in L_2(\Omega)\}$ be the space of the vector fields parallel to $\nabla\tau$. The N-transform is a map from $\mathscr P$ to $\mathscr L_\lambda$ defined layer-wise (in accordance with $\Omega=\cup_{\tau\geqslant 0}\Gamma^\tau$) by $$ Nh\,\big|_{\Gamma^\tau}:=(P^\tau h)\big|_{\Gamma^{\tau-0}}, \qquad\tau>0, $$ where $P^\tau$ are the projections in $\mathscr P$ onto the subspaces $\mathscr P^\tau:=\{h\in\mathscr P\,|\,\,{\rm supp\,}h\subset\overline{\Omega^\tau}\}$. We show that $N$ is a unitary operator.
Let $p=p^f(x)$ be a solution to the Dirichlet problem: $\Delta_g p=0$ in $\Omega\setminus\Gamma$, $p=f$ on $\Gamma$. The DN-map $\Lambda$ is defined by $\Lambda f:=-\langle\nabla p^f,\nabla\tau\rangle$ on $\Gamma$. We show that the N-transform provides a certain factorization $\Lambda^{-1}=V^*V$ and discuss its possible usefulness for determination of $(\Omega,g)$ from $\Lambda$.
From: Mikhail Belishev [view email]
[v1]
Sun, 14 Jun 2026 16:26:19 UTC (12 KB)
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