REVIEW 1 major objections 2 cited by
An inverse source problem for the Monge--Ampere equation from large boundary data
T0 review · 1 major / 0 minor · reviewed 2026-06-27 · grok-4.3
Pith's one-line read The Dirichlet-to-Neumann map determines the positive source uniquely for the Monge-Ampere equation with convex solutions.
desk verdict The paper proves uniqueness for the source in the Monge-Ampère equation from the DN map by reducing via large boundary data to X-ray injectivity; the reduction step is the part that needs verification. 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
A family of large boundary values that reduces the inverse source problem for the Monge-Ampere equation to the injectivity of the Euclidean X-ray transform.
What would settle it
Two distinct positive smooth sources f and g on the same domain that produce identical Dirichlet-to-Neumann maps for every sufficiently large convex boundary datum would falsify the claim.
Extended reading notes
Core claim
In the smooth classical regime, the Dirichlet-to-Neumann map associated with convex solutions to det D²u = f(x) determines the positive source f uniquely. The proof constructs a family of large boundary values that reduces the inverse source problem to the injectivity of the Euclidean X-ray transform.
Load-bearing premise
A family of sufficiently large boundary values can be constructed to reduce the inverse source problem to the injectivity of the X-ray transform.
Editorial extensions
If this is right
- The positive source f is uniquely recoverable from the Dirichlet-to-Neumann map alone.
- The uniqueness holds for convex solutions in the smooth classical regime on uniformly convex domains.
- The reduction via large boundary data transfers known injectivity results from the X-ray transform directly to the nonlinear problem.
Reading between the lines
- Numerical reconstruction procedures could proceed by first extracting line integrals from the large-data measurements and then inverting the X-ray transform.
- The same large-boundary reduction strategy may extend to inverse source problems for other fully nonlinear elliptic equations.
- The approach indicates that sufficiently strong boundary perturbations can effectively linearize the recovery of coefficients in certain nonlinear settings.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies an inverse source problem for the Monge-Ampère equation det D²u = f(x) on a bounded smooth uniformly convex domain Ω. In the smooth classical regime, it claims to prove that the Dirichlet-to-Neumann map associated with convex solutions uniquely determines the positive source f. The argument constructs a family of large boundary values φ_t, produces corresponding convex solutions u_t, and reduces the inverse problem to the known injectivity of the Euclidean X-ray transform in a suitable scaled limit as t → ∞.
Significance. If the reduction is rigorously justified, the result would establish a uniqueness theorem for an inverse source problem in the Monge-Ampère setting by connecting it to the X-ray transform, a standard tool in integral geometry. This could be of interest in optimal transport and geometric PDEs, particularly if the construction preserves uniform convexity and controls error terms without additional assumptions on f beyond positivity and smoothness.
major comments (1)
- [Abstract / reduction argument] The central reduction step (abstract, final sentence) asserts that a specific family of large boundary values φ_t yields convex u_t whose DN map, after scaling, recovers the X-ray transform of log f (or an equivalent functional). However, the manuscript provides no explicit construction of φ_t, no scaling law, and no error estimates showing that boundary curvature effects and lower-order terms vanish while preserving injectivity inside the C^{2,α} convex regime. This leaves the validity of the reduction unverified and load-bearing for the uniqueness claim.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for identifying the need for greater explicitness in the central reduction argument. We address this point below and will incorporate the requested details in a revised version.
read point-by-point responses
-
Referee: [Abstract / reduction argument] The central reduction step (abstract, final sentence) asserts that a specific family of large boundary values φ_t yields convex u_t whose DN map, after scaling, recovers the X-ray transform of log f (or an equivalent functional). However, the manuscript provides no explicit construction of φ_t, no scaling law, and no error estimates showing that boundary curvature effects and lower-order terms vanish while preserving injectivity inside the C^{2,α} convex regime. This leaves the validity of the reduction unverified and load-bearing for the uniqueness claim.
Authors: We agree that the reduction requires a more self-contained and explicit presentation to allow verification of the limit process. In the revision we will add an explicit construction of the family φ_t (of the form t·ψ + lower-order correction chosen to preserve uniform convexity of the domain and the solution), state the precise scaling (normalization by t together with the associated change of variables for the DN map), and supply error estimates (via a new lemma) showing that curvature and lower-order contributions vanish in the t→∞ limit while remaining inside the C^{2,α} convex regime. These additions will make the passage to the Euclidean X-ray transform of log f fully rigorous and verifiable. revision: yes
Circularity Check
No circularity; reduction to external X-ray injectivity is independent.
full rationale
The paper reduces the inverse source problem to injectivity of the Euclidean X-ray transform via a family of large boundary values. This is an external, standard result (not derived or fitted inside the paper). No self-definitional steps, fitted inputs renamed as predictions, or load-bearing self-citations appear in the provided abstract or description. The derivation chain is self-contained against external benchmarks.
Assumptions & free parameters
assumptions (2)
- domain assumption Domain is bounded, smooth, and uniformly convex.
- domain assumption Solutions are convex (classical smooth regime).
Cite this review
Pith. "Pith review of An inverse source problem for the Monge--Ampere equation from large boundary data." pith.science (2026). https://pith.science/paper/4EMRZLJL
@misc{pith2026260607064,
author = {Pith},
title = {Pith review of: An inverse source problem for the Monge--Ampere equation from large boundary data},
year = {2026},
howpublished = {\url{https://pith.science/paper/4EMRZLJL}},
note = {Machine review of arXiv:2606.07064}
}
abstract
We study an inverse source problem for the Monge--Ampere equation \[ \det D^2u=f(x) \] on a bounded smooth uniformly convex domain. In the smooth classical regime, we prove that the Dirichlet-to-Neumann map associated with convex solutions determines the positive source uniquely. The proof uses a family of large boundary values and reduces the inverse source problem to the injectivity of the Euclidean X-ray transform.
Forward citations
Cited by 2 Pith papers
-
Affine section tomography for inverse source problems in $k$-Hessian equations with restricted large boundary data
Restricted large-data nonlinear DN maps for k-Hessian equations recover a positive source uniquely through the affine q-plane Radon transform of its zero extension.
-
Gauge rigidity in an inverse problem for the prescribed Gaussian curvature equation
If two positive curvatures share the same first boundary jet and induce the same nonlinear DN map on a common open class of admissible boundary data, then the curvatures coincide throughout a planar domain.
Reference graph
Works this paper leans on
-
[1]
T. Brander. Calder´ on problem for thep-Laplacian: first order derivative of conductiv- ity on the boundary.Proceedings of the American Mathematical Society, 144(1):177– 189, 2016
2016
-
[2]
Brander, B
T. Brander, B. Harrach, M. Kar, and M. Salo. Monotonicity and enclosure methods for thep-Laplace equation.SIAM Journal on Applied Mathematics, 78(2):742–758, 2018
2018
-
[3]
Brander, M
T. Brander, M. Kar, and M. Salo. Enclosure method for thep-Laplace equation. Inverse Problems, 31(4):045001, 2015. 23
2015
-
[4]
L. A. Caffarelli, L. Nirenberg, and J. Spruck. The Dirichlet problem for nonlinear second-order elliptic equations. I. Monge–Amp` ere equation.Communications on Pure and Applied Mathematics, 37(3):369–402, 1984
1984
-
[5]
C. I. Cˆ arstea and A. Feizmohammadi. An inverse boundary value problem for certain anisotropic quasilinear elliptic equations.Journal of Differential Equations, 284:318– 349, 2021
2021
-
[6]
C. I. Cˆ arstea and A. Feizmohammadi. A density property for tensor products of gradients of harmonic functions and applications.Journal of Functional Analysis, 284(2):109740, 2023
2023
-
[7]
C. I. Cˆ arstea and A. Feizmohammadi. Two uniqueness results in the inverse boundary value problem for the weightedp-Laplace equation.Forum of Mathematics, Sigma, 13:e147, 2025
2025
- [8]
Show all 37 references
-
[9]
C. I. Cˆ arstea, T. Ghosh, and G. Nakamura. An inverse boundary value problem for the inhomogeneous porous medium equation.SIAM Journal on Applied Mathematics, 85(1):278–293, 2025
2025
-
[10]
C. I. Cˆ arstea, T. Ghosh, and G. Uhlmann. An inverse problem for the porous medium equation with partial data and a possibly singular absorption term.SIAM Journal on Mathematical Analysis, 55(1):162–185, 2023
2023
-
[11]
C. I. Cˆ arstea and M. Kar. Recovery of coefficients for a weightedp-Laplacian perturbed by a linear second order term.Inverse Problems, 37(1):015013, 2021
2021
-
[12]
C. I. Cˆ arstea, M. Lassas, T. Liimatainen, and L. Oksanen. An inverse problem for the Riemannian minimal surface equation.Journal of Differential Equations, 379:626–648, 2024
2024
-
[13]
C. I. Cˆ arstea and P. Zimmermann. Reconstruction of coefficients in the double phase problem, 2025. arXiv:2504.01691
2025
-
[14]
Egger, J.-F
H. Egger, J.-F. Pietschmann, and M. Schlottbom. Simultaneous identification of dif- fusion and absorption coefficients in a quasilinear elliptic problem.Inverse Problems, 30(3):035009, 2014
2014
-
[15]
Feizmohammadi and L
A. Feizmohammadi and L. Oksanen. An inverse problem for a semi-linear elliptic equation in Riemannian geometries.Journal of Differential Equations, 269(6):4683– 4719, 2020
2020
-
[16]
C.-Y. Guo, M. Kar, and M. Salo. Inverse problems forp-Laplace type equations under monotonicity assumptions.Rendiconti dell’Istituto di Matematica dell’Universit` a di Trieste, 48:79–99, 2016
2016
-
[17]
C. E. Guti´ errez.The Monge–Amp` ere Equation, volume 89 ofProgress in Nonlinear Differential Equations and Their Applications. Birkh¨ auser, Cham, second edition, 2016
2016
-
[18]
D. F. Hervas and Z. Sun. An inverse boundary value problem for quasilinear elliptic equations.Communications in Partial Differential Equations, 27(11–12):2449–2490, 2002. 24
2002
-
[19]
V. Isakov. On uniqueness in inverse problems for semilinear parabolic equations. Archive for Rational Mechanics and Analysis, 124(1):1–12, 1993
1993
-
[20]
Isakov and A
V. Isakov and A. I. Nachman. Global uniqueness for a two-dimensional semilinear ellip- tic inverse problem.Transactions of the American Mathematical Society, 347(9):3375– 3390, 1995
1995
-
[21]
Isakov and J
V. Isakov and J. Sylvester. Global uniqueness for a semilinear elliptic inverse problem. Communications on Pure and Applied Mathematics, 47(10):1403–1410, 1994
1994
-
[22]
Kang and G
H. Kang and G. Nakamura. Identification of nonlinearity in a conductivity equation via the Dirichlet-to-Neumann map.Inverse Problems, 18(4):1079–1088, 2002
2002
-
[23]
Kar and J.-N
M. Kar and J.-N. Wang. Size estimates for the weightedp-Laplace equation with one measurement.Discrete and Continuous Dynamical Systems - B, 26(4):2011–2024, 2021
2011
-
[24]
Y. Kian, K. Krupchyk, and G. Uhlmann. Partial data inverse problems for quasilinear conductivity equations.Mathematische Annalen, 385(3–4):1611–1638, 2023
2023
-
[25]
Krupchyk and G
K. Krupchyk and G. Uhlmann. Partial data inverse problems for semilinear elliptic equations with gradient nonlinearities.Mathematical Research Letters, 27(6):1801– 1824, 2020
2020
-
[26]
Kurylev, M
Y. Kurylev, M. Lassas, and G. Uhlmann. Inverse problems for Lorentzian manifolds and non-linear hyperbolic equations.Inventiones Mathematicae, 212(3):781–857, 2018
2018
-
[27]
Lassas, T
M. Lassas, T. Liimatainen, Y.-H. Lin, and M. Salo. Inverse problems for elliptic equa- tions with power type nonlinearities.Journal de Math´ ematiques Pures et Appliqu´ ees, 145:44–82, 2021
2021
-
[28]
Lassas, T
M. Lassas, T. Liimatainen, Y.-H. Lin, and M. Salo. Partial data inverse problems and simultaneous recovery of boundary and coefficients for semilinear elliptic equations. Revista Matem´ atica Iberoamericana, 37(4):1553–1580, 2021
2021
-
[29]
Liimatainen and Y.-H
T. Liimatainen and Y.-H. Lin. An inverse problem for the Monge–Amp` ere equation,
-
[30]
Malgrange.Ideals of Differentiable Functions, volume 3 ofTata Institute of Fun- damental Research Studies in Mathematics
B. Malgrange.Ideals of Differentiable Functions, volume 3 ofTata Institute of Fun- damental Research Studies in Mathematics. Oxford University Press, London, 1966. Published for the Tata Institute of Fundamental Research, Bombay
1966
-
[31]
Mu˜ noz and G
C. Mu˜ noz and G. Uhlmann. The Calder´ on problem for quasilinear elliptic equations. Annales de l’Institut Henri Poincar´ e C, Analyse Non Lin´ eaire, 37(5):1143–1166, 2020
2020
-
[32]
Natterer.The Mathematics of Computerized Tomography, volume 32 ofClassics in Applied Mathematics
F. Natterer.The Mathematics of Computerized Tomography, volume 32 ofClassics in Applied Mathematics. Society for Industrial and Applied Mathematics, Philadelphia, 2001
2001
-
[33]
Salo and X
M. Salo and X. Zhong. An inverse problem for thep-Laplacian: boundary determina- tion.SIAM Journal on Mathematical Analysis, 44(4):2474–2495, 2012
2012
-
[34]
R. Shankar. Recovering a quasilinear conductivity from boundary measurements.In- verse Problems, 37(1):015014, 2021. 25
2021
-
[35]
Z. Sun. On a quasilinear inverse boundary value problem.Mathematische Zeitschrift, 221:293–305, 1996
1996
-
[36]
Z. Sun. An inverse boundary-value problem for semilinear elliptic equations.Electronic Journal of Differential Equations, 2010(37):1–5, 2010
2010
-
[37]
Sun and G
Z. Sun and G. Uhlmann. Inverse problems in quasilinear anisotropic media.American Journal of Mathematics, 119(4):771–797, 1997. 26
1997
Reviewed June 27, 2026 · model on record in the stance chip above.
Discussion (0). Sign in to comment.