REVIEW 2 major objections 6 minor 2 cited by
The Calder\'on problem for the logarithmic Schr\"odinger equation
T0 review · 2 major / 6 minor · reviewed 2026-08-11 · deepseek-v4-flash
Pith's one-line read Boundary measurements uniquely determine the potential of a logarithmic Schrödinger equation in every dimension.
desk verdict Solid first uniqueness theorem for the logarithmic Laplacian, but the constructive part has a real gap and a sign error that need fixing. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The key machinery is the unique continuation property (UCP) of the logarithmic Laplacian, stated as Proposition 4.1 and imported from a companion paper: if $u\in L^1_0(\mathbb{R}^n)$ and $u=L_{\Delta}u=0$ in a nonempty open set, then $u\equiv 0$ on $\mathbb{R}^n$. This UCP is used to prove the Runge approximation property (Proposition 4.2), which asserts that solutions generated by boundary data supported in a small exterior set are dense in $L^2(\Omega)$. The Runge approximation, together with the integral identity and a localized-potentials lemma, forms the backbone of both the global uniqueness theorem and the constructive monotonicity-based recovery.
What would settle it
Find a nonzero function $u\in L^1_0(\mathbb{R}^n)$ and a nonempty open set $D$ such that $u=L_{\Delta}u=0$ in $D$ but $u\not\equiv 0$; this would directly contradict Proposition 4.1 and invalidate the Runge approximation used in the proof of Theorem 1.1.
Extended reading notes
Core claim
The central claim is that the logarithmic Laplacian, despite being a near-zero-order nonlocal operator, admits a unique continuation property and a Runge approximation property strong enough to solve the inverse problem. Under the spectral condition $\lambda_1(\Omega)+q\ge \lambda_0>0$, the paper shows that equality of the partial Dirichlet-to-Neumann maps, $\langle\Lambda_{q_1}f,g\rangle=\langle\Lambda_{q_2}f,g\rangle$ for all smooth $f,g$ supported in nonempty open sets $W_1,W_2\Subset\Omega^c$, forces $q_1=q_2$ in $\Omega$. The proof uses an integral identity that relates the difference of DN maps to the integral of $(q_1-q_2)u_1u_2$, combined with Runge approximation to localize the solutions inside $\Omega$. The paper also establishes an if-and-only-if monotonicity relation, which yields a constructive formula for recovering nonnegative potentials when $\lambda_1(\Omega)>0$.
Load-bearing premise
The proof relies on the unique continuation property for the logarithmic Laplacian: if a function and its logarithmic Laplacian both vanish in a nonempty open set, the function must vanish everywhere. If this property fails, the main uniqueness theorem collapses.
Editorial extensions
If this is right
- If the main theorem is correct, then for bounded Lipschitz domains and $L^\infty$ potentials satisfying the spectral condition, the logarithmic Schrödinger operator is identified from boundary measurements in any dimension, matching the strength of known results for the fractional Laplacian.
- The if-and-only-if monotonicity relation provides a constructive algorithm for recovering nonnegative potentials pointwise, using only comparisons with simpler (density-one simple function) potentials.
- The paper opens the door to studying inverse problems for operators of zero or negative order, where classical elliptic regularity and CGO solutions are not available.
- The UCP-based Runge approximation may be transferable to other inverse problems involving operators with logarithmic symbols, such as fractional Laplacians near $s=0$.
Reading between the lines
- A natural extension is to ask whether the potential can be recovered from a single measurement, which the paper remarks would require a measurable UCP for the logarithmic Laplacian; this is open for rough potentials.
- The monotonicity method could be adapted to detect inclusions or obstacles inside $\Omega$ from boundary measurements, analogous to known monotonicity-based obstacle detection for fractional and classical Schrödinger equations.
- Because the logarithmic Laplacian approximates the fractional Laplacian as $s\to 0^+$, the uniqueness result here may inform the behavior of inverse problems for very small fractional order $s$, where positive-order theory degenerates.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies the Calderón problem for the logarithmic Schrödinger operator L_Δ + q, where L_Δ is the logarithmic Laplacian. After formulating a well-posed exterior boundary value problem and a Dirichlet-to-Neumann map under the spectral condition λ1(Ω)+q≥λ0>0, the authors prove a global uniqueness result (Theorem 1.1): equality of the DN maps on arbitrary nonempty open sets W1,W2⊂Ω_e forces q1=q2 in Ω. The proof uses an integral identity, the unique continuation property for L_Δ cited from [CHW23], and a Runge approximation result. The second half develops a constructive uniqueness theory: an if-and-only-if monotonicity relation between potentials and DN maps (Theorem 1.2) and a reconstruction formula for nonnegative potentials using density-one simple functions (Theorem 1.4). The paper claims all results hold in any space dimension.
Significance. If completed, the paper would provide the first global uniqueness result for the logarithmic Schrödinger operator, a genuinely near-zero-order nonlocal operator, and would extend the monotonicity-based reconstruction method to this setting. The main proof of Theorem 1.1 is concise and dimension-independent, and it rests on a clearly identified external UCP rather than on ad hoc assumptions. A particular strength is that the dependence on the UCP is made explicit in Proposition 4.1 and Remark 4.4. The constructive part is more fragile: Lemma 5.1, which is load-bearing for Theorems 1.2 and 1.4, has a proof gap and an omitted hypothesis, and Theorem 1.2 contains a sign error. These issues appear repairable within the scope of the paper, but they must be fixed before the constructive claims are justified.
major comments (2)
- [§5.1, Lemma 5.1] The proof of Lemma 5.1 is not valid as written for arbitrary measurable M. It asserts that ‖~u_k‖_{L^2(Ω\M)}>0 'follows from the UCP of Proposition 4.1', but Proposition 4.1 is an open-set UCP: it applies only when the function vanishes on a nonempty open set. For a general measurable M the complement Ω\M may have empty interior, so the cited UCP does not apply; this is exactly the 'measurable UCP' that Remark 4.4 declares open. Additionally, the statement of Lemma 5.1 omits the spectral condition (1.9), although the proof invokes the Runge approximation of Proposition 4.2, which requires that condition. Since Theorem 1.2(iii)⇒(i) applies the lemma with M={x: q1(x)−q2(x)≥δ} and Theorem 1.4 relies on Theorem 1.2, the constructive uniqueness results are not justified as stated. The gap appears repairable: one can choose Runge approximations to χ_M/√|M| plus a small bump supported in Ω\M, then take a diagonal sequence, which removes the need for a measurable UCP (the case where Ω\M has measure zero can be handled by direct scaling).
- [§1, Theorem 1.2 and §5.2] The sign in condition (1.12) is reversed. The monotonicity direction (ii) and the proof of (iii)⇒(i) require the inequality ⟨(Λ_{q2}−Λ_{q1})f,f⟩≥0; as printed, (1.12) is ⟨(Λ_{q1}−Λ_{q2})f,f⟩≥0. With the printed sign, condition (ii) does not imply (iii), the definition (1.13) of Λ_{q1}≤Λ_{q2} is incoherent, and the contradiction derived in (5.6) does not contradict (1.12). This is a typographical but load-bearing error: The statement and the definition must be corrected so that the monotonicity relation Λ_{q1}≤Λ_{q2} in W means ⟨(Λ_{q2}−Λ_{q1})f,f⟩≥0 for f∈C_c^∞(W).
minor comments (6)
- [§2.1, eq. (2.13)] In the Cauchy-Schwarz estimate after (2.13), the second factor should be ‖v‖_{H(R^n)}, not ‖u‖_{H(R^n)}.
- [§2.1, proof of Lemma 2.1] The phrase 'equivalent on H^1_0(Ω)' should read 'equivalent on H_0(Ω)'.
- [§5.2, eq. (5.4)] The displayed inequality is missing a closing parenthesis: it should read ⟨(Λ_{q2}−Λ_{q1})f,f⟩, not ⟨(Λ_{q2}−Λ_{q1}f,f⟩.
- [§5.1, Lemma 5.1] The statement should require M⊂Ω to have positive measure, since the target function χ_M/√(∫_M 1 dx) is otherwise undefined.
- [Remark 4.4] The phrase 'positive measures' should be 'positive measure'.
- [§3, proof of Lemma 3.1] The sentence beginning 'Let f ∈ H_T(Ω_e)' is missing a period before 'By definition'.
Circularity Check
No significant circularity: the uniqueness argument reduces to an external UCP and standard Runge approximation, not to its own conclusion.
full rationale
The derivation chain for Theorem 1.1 is: DN-map equality, integral identity (3.14), Runge approximation (Prop. 4.2), L2-density of solutions, and then q1 = q2 a.e. Prop. 4.2 is derived from the unique continuation property in Prop. 4.1, which is cited from [CHW23, Theorem 5.1] rather than proved in this paper. That UCP is a parameter-free statement about the logarithmic Laplacian whose hypotheses (u in L1_0, u = L_Delta u = 0 in a nonempty open set) do not include the inverse problem, the DN map, or the potentials being recovered; it is therefore independent support even though one of the present authors is also an author of [CHW23]. Similarly, Theorem 1.4 uses the density-one representation lemma [HL19, Lemma 4.4]; that lemma is measure-theoretic and does not presuppose the DN-map conclusion. No parameter is fitted and no prediction is defined in terms of the quantity to be recovered, so no step reduces by construction to its own input. The genuine concerns here are correctness risks rather than circularity: Lemma 5.1 applies the open-set UCP of Prop. 4.1 to the complement Omega\M for an arbitrary measurable set M, where Omega\M may have empty interior (Remark 4.4 itself flags the missing measurable UCP), and the printed inequality (1.12) in Theorem 1.2 has the opposite sign from the monotonicity inequality (5.4) when q2 >= q1. These are substantive proof and statement issues, but they are not circularity, so the circularity score is 0.
Assumptions & free parameters
assumptions (4)
- domain assumption Unique continuation property for L_Δ: if u∈L^1_0(R^n) and u=L_Δu=0 in a nonempty open set, then u≡0 in R^n.
- domain assumption Spectral condition (1.9): λ1(Ω)+q(x)≥λ0>0 for a.e. x∈Ω.
- domain assumption Density-one representation (5.7): q(x)=sup{φ(x): φ∈Σ_{+,0}, φ≤q} for a.e. x.
- standard math Spectral theory of the logarithmic Laplacian: L_Δ has discrete eigenvalues λk(Ω) on a bounded domain, as in [CW19, Theorem 1.2].
Cite this review
Pith. "Pith review of The Calder\'on problem for the logarithmic Schr\"odinger equation." pith.science (2026). https://pith.science/paper/QKCYOIX3
@misc{pith2026241217775,
author = {Pith},
title = {Pith review of: The Calder\'on problem for the logarithmic Schr\"odinger equation},
year = {2026},
howpublished = {\url{https://pith.science/paper/QKCYOIX3}},
note = {Machine review of arXiv:2412.17775}
}
abstract
We study the Calder\'on problem for a logarithmic Schr\"odinger type operator of the form $L_{\Delta} +q$, where $L_{\Delta}$ denotes the logarithmic Laplacian, which arises as formal derivative $\frac{d}{ds} \big|_{s=0}(-\Delta)^s$ of the family of fractional Laplacian operators. This operator enjoys remarkable nonlocal properties, such as the unique continuation and Runge approximation. Based on these tools, we can uniquely determine bounded potentials using the Dirichlet-to-Neumann map. Additionally, we can build a constructive uniqueness result by utilizing the monotonicity method. Our results hold for any space dimension.
Forward citations
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The paper claims an anisotropic Calderon uniqueness theorem for a logarithmic Laplacian of order 2+, but the central Paley-Wiener argument is invalid.
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Reviewed August 11, 2026 · model on record in the stance chip above.
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