Reconstruction of non-self-adjoint anisotropic and complex inclusions in the Calder\'on problem
Pith reviewed 2026-05-08 16:30 UTC · model grok-4.3
The pith
Monotonicity methods detect inclusions in the partial data anisotropic Calderón problem under general non-self-adjoint perturbations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We generalize recent results on the monotonicity method, for inclusion detection in the partial data anisotropic Calderón problem, to very general non-self-adjoint perturbations. This involves a forward model that accounts for both the anisotropic real conductivity and the anisotropic permittivity, and the results hold in any spatial dimension d ≥ 2. We assume that the inclusion boundaries can be reached from the domain boundary via a set on which the background conductivity is self-adjoint, and that a definiteness condition holds near the inclusion boundaries. Away from the inclusion boundaries we allow general L^∞ non-self-adjoint perturbations. We only require unique continuation based on
What carries the argument
The monotonicity method, extended by replacing global self-adjointness with a reachability condition through a self-adjoint background set plus a local definiteness condition near inclusion boundaries.
If this is right
- Inclusions remain detectable even when non-self-adjoint perturbations are arbitrary away from their boundaries.
- The method continues to work with only partial boundary measurements in dimensions d ≥ 2.
- Unique continuation is required only for the self-adjoint part of the background conductivity.
- The same monotonicity argument applies to both conductivity and permittivity inclusions simultaneously.
Where Pith is reading between the lines
- The local character of the self-adjoint requirement may let the method apply to heterogeneous media where global symmetry fails.
- Numerical tests with deliberately non-self-adjoint complex admittivities could check whether the monotonicity signature survives in practice.
- Similar localization of self-adjointness might extend the approach to other inverse problems that currently demand full self-adjoint coefficients.
Load-bearing premise
Inclusion boundaries must be reachable from the domain boundary along a path where the background conductivity remains self-adjoint, together with a definiteness condition holding near those boundaries.
What would settle it
An explicit example of an inclusion that satisfies the reachability and definiteness conditions yet produces no detectable monotonicity signature when the non-self-adjoint perturbation is present.
read the original abstract
We generalize recent results on the monotonicity method, for inclusion detection in the partial data anisotropic Calder\'on problem, to very general non-self-adjoint perturbations. This involves a forward model that accounts for both the anisotropic real conductivity and the anisotropic permittivity, and the results hold in any spatial dimension $d \geq 2$. We assume that the inclusion boundaries can be reached from the domain boundary via a set on which the background conductivity is self-adjoint, and that a definiteness condition holds near the inclusion boundaries. Away from the inclusion boundaries we allow general $L^\infty$ non-self-adjoint perturbations. We only require unique continuation based on the self-adjoint part of the background conductivity, thus making the methods compatible with generic unique continuation results.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript generalizes recent results on the monotonicity method for inclusion detection in the partial-data anisotropic Calderón problem to very general non-self-adjoint perturbations. It introduces a forward model incorporating both anisotropic real conductivity and anisotropic permittivity, with results claimed to hold in any dimension d ≥ 2. The key hypotheses are that inclusion boundaries are reachable from the domain boundary via a set on which the background conductivity is self-adjoint, a definiteness condition holds near the inclusion boundaries, general L^∞ non-self-adjoint perturbations are permitted away from those boundaries, and unique continuation is required only for the self-adjoint part of the background conductivity.
Significance. If the central claims hold, the work meaningfully extends the applicability of monotonicity-based reconstruction to complex, lossy, and non-self-adjoint media without imposing smallness conditions on the perturbations or coercivity on the full operator. The restriction of unique continuation to the self-adjoint background component on a connecting set is a strength, as it aligns with generic unique-continuation theorems and avoids stronger global assumptions. This broadens the method's relevance for applications such as electrical impedance tomography in heterogeneous or complex materials.
minor comments (2)
- The introduction would benefit from a concise table or paragraph explicitly contrasting the new assumptions (definiteness only near boundaries, unique continuation only on the self-adjoint part) with those in the cited prior works on the monotonicity method.
- Notation for the anisotropic conductivity and permittivity tensors could be clarified in §2 by adding a short remark on how the complex-valued case reduces to the real anisotropic case when the imaginary part vanishes.
Simulated Author's Rebuttal
We thank the referee for the careful reading and positive assessment of the manuscript, including the recommendation for minor revision. The referee summary correctly identifies the main contributions and assumptions. No specific major comments were provided in the report.
Circularity Check
No significant circularity
full rationale
The paper generalizes the monotonicity method for partial-data anisotropic Calderón problems to non-self-adjoint perturbations by introducing a forward model with anisotropic conductivity and permittivity, plus explicit assumptions on boundary-reaching self-adjoint sets, definiteness near inclusions, and unique continuation restricted to the self-adjoint background part. These extensions are stated independently of the target reconstruction result and rely on standard external unique-continuation theorems rather than self-referential definitions or fitted inputs. No load-bearing step reduces by construction to a prior self-citation, ansatz, or renamed empirical pattern; the central claims remain externally verifiable against the stated hypotheses.
Axiom & Free-Parameter Ledger
axioms (3)
- domain assumption Inclusion boundaries can be reached from the domain boundary via a set on which the background conductivity is self-adjoint
- domain assumption A definiteness condition holds near the inclusion boundaries
- domain assumption Unique continuation holds based only on the self-adjoint part of the background conductivity
Reference graph
Works this paper leans on
-
[1]
G. Alessandrini. Strong unique continuation for general elliptic equations in 2D.J. Math. Anal., 386(2):669– 676, 2012
work page 2012
- [2]
-
[3]
V. Candiani, J. Dard´ e, H. Garde, and N. Hyv¨ onen. Monotonicity-based reconstruction of extreme inclusions in electrical impedance tomography.SIAM J. Math. Anal., 52(6):6234–6259, 2020
work page 2020
-
[4]
H. Garde and N. Hyv¨ onen. Series reversion in Calder´ on’s problem.Math. Comp., 91(336):1925–1953, 2022
work page 1925
- [5]
-
[6]
H. Garde and M. Vogelius. Reconstruction of cracks in Calder´ on’s inverse conductivity problem using energy comparisons.SIAM J. Math. Anal., 56(1):727–745, 2024
work page 2024
-
[7]
N. Garofalo and F.-H. Lin. Monotonicity properties of variational integrals,Ap weights and unique continuation. Indiana Univ. Math. J., 35(2):245–268, 1986
work page 1986
-
[8]
B. Harrach. Uniqueness and Lipschitz stability in electrical impedance tomography with finitely many elec- trodes.Inverse Problems, 35(2) article no. 024005, 2019
work page 2019
-
[9]
B. Harrach, E. Lee, and M. Ullrich. Combining frequency-difference and ultrasound modulated electrical impedance tomography.Inverse Problems, 31(9) article no. 095003, 2015. 16 H. GARDE, D. JOHANSSON, AND T. ZACHAROPOULOS
work page 2015
-
[10]
B. Harrach and J. K. Seo. Detecting inclusions in electrical impedance tomography without reference measure- ments.SIAM J. Appl. Math., 69(6):1662–1681, 2009
work page 2009
-
[11]
B. Harrach and J. K. Seo. Exact shape-reconstruction by one-step linearization in electrical impedance tomog- raphy.SIAM J. Math. Anal., 42(4):1505–1518, 2010
work page 2010
-
[12]
B. Harrach and M. Ullrich. Monotonicity-based shape reconstruction in electrical impedance tomography. SIAM J. Math. Anal., 45(6):3382–3403, 2013
work page 2013
-
[13]
A. Kirsch. The factorization method for a class of inverse elliptic problems.Math. Nachr., 278(3):258–277, 2005
work page 2005
-
[14]
J. M. Lee and G. Uhlmann. Determining anisotropic real-analytic conductivities by boundary measurements. Comm. Pure Appl. Math., 42(8):1097–1112, 1989
work page 1989
- [15]
- [16]
-
[17]
K. Miller. Nonunique continuation for uniformly parabolic and elliptic equations in self-adjoint divergence form with H¨ older continuous coefficients.Arch. Ration. Mech. Anal., 54:105–117, 1974
work page 1974
-
[18]
A. Tamburrino and G. Rubinacci. A new non-iterative inversion method for electrical resistance tomography. Inverse Problems, 18(6):1809–1829, 2002. (H. Garde)Department of Mathematics, Aarhus University, Aarhus, Denmark. Email address:garde@math.au.dk (D. Johansson)Department of Mathematics, Aarhus University, Aarhus, Denmark. Email address:johansson@math...
work page 2002
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.