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A nontrivial boundary-fixing radial gauge on the ball
Example
Assume the Axiom of Choice and let . On the unit ball take the constant matrix conductivity , the identity matrix. For , define by and define by the anisotropic conductivity pushforward formula. For or , let be the weak energy map on given by , where is the unique weak solution with boundary class and is any representative of . Then is a smooth diffeomorphism that fixes pointwise, is smooth and uniformly positive definite, and ; nevertheless .
Example references
Facts & Assumptions
Given: The Axiom of Choice; an integer ; the unit ball ; the identity matrix conductivity ; and .
The Axiom of Choice, as assumed by the local anisotropic DN map and gauge theorem. (The Axiom of Choice)
If is a smooth boundary-fixing diffeomorphism and is a smooth uniformly positive-definite symmetric conductivity, then for is smooth uniformly positive definite and . (A boundary-fixing diffeomorphism preserves the anisotropic DN map, Statement)
The weak DN map is the energy form on , defined using the unique weak solution and any representative of the second boundary datum. (Anisotropic conductivity and weak Dirichlet-to-Neumann map, Definition)
Verification
Write for . Then , , and . Thus is a strictly increasing bijection of to itself; preserves each radial ray, is bijective on the ball, and fixes the boundary pointwise.
At the origin and . At the radial derivative is and each tangential eigenvalue is . By continuity, stays positive on for some . The same radial formula extends to a smooth diffeomorphism from the ball of radius onto its image, which contains a neighborhood of ; its inverse is smooth there. Thus the inverse is smooth through the boundary and the differential is nonsingular on the closed ball.
Since , the pushforward formula in [F1] gives . Because and , this differs from , so the pushed-forward conductivity is nontrivial.
The hypotheses of [F1] hold for and , so . The example therefore exhibits a distinct smooth anisotropic conductivity with exactly the same boundary energy map, caused by the stated boundary-fixing change of variables.
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Sources
- Mikko Salo, The Calderón problem on Riemannian manifolds (2012) (standard reference, not scraped)
- Thierry Daudé, Niky Kamran, and François Nicoleau, A survey of non-uniqueness results for the anisotropic Calderón problem with disjoint data (2018) (standard reference, not scraped)