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arxiv: 2506.11560 · v2 · submitted 2025-06-13 · 🧮 math.AP · cs.NA· math-ph· math.MP· math.NA

On scattering for NLS: rigidity properties and numerical simulations via the lens transform

Pith reviewed 2026-05-19 09:50 UTC · model grok-4.3

classification 🧮 math.AP cs.NAmath-phmath.MPmath.NA
keywords nonlinear Schrödinger equationscattering operatorlens transformnumerical simulationslong-range scatteringrigidity properties
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The pith

The lens transform compactifies space-time to enable efficient and reliable numerical computation of the NLS scattering operator.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The authors demonstrate that the lens transform overcomes the computational challenges of the infinite-time scattering operator for the defocusing nonlinear Schrödinger equation. By compactifying the space-time domain, their method provides an efficient way to simulate the long-time nonlinear evolution. They prove new identities and properties of the operator to underpin the numerical approach. Experiments confirm consistency with analytical results and extend to long-range scattering, generating conjectures about fixed points and existence in focusing cases. This matters to readers interested in bridging analysis and computation for dispersive equations.

Core claim

By exploiting the space-time compactification provided by the lens transform, the paper develops a highly efficient and reliable methodology for computing the scattering operator associated with the defocusing nonlinear Schrödinger equation. Several new identities and theoretical properties of the scattering operator are introduced and proved, with numerical experiments validating the approach against known analytics and addressing long-range scattering for the one-dimensional cubic case, while formulating conjectures on fixed and rotating points and existence in long-range defocusing and focusing settings.

What carries the argument

The lens transform, which compactifies the infinite time interval into a bounded domain for simulating the scattering behavior of NLS solutions.

If this is right

  • The scattering operator can be computed numerically in regimes previously inaccessible due to infinite time.
  • Numerical results agree with known analytical properties of the scattering operator.
  • Long-range scattering in one-dimensional cubic NLS is simulated successfully.
  • Conjectures are proposed for fixed and rotating points of the operator and its existence in long-range focusing cases.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Similar compactification techniques could apply to scattering problems in other nonlinear wave equations.
  • The conjectures might motivate rigorous proofs if the numerical evidence is strong enough.
  • This numerical method provides a tool to test theoretical predictions and explore parameter spaces in scattering theory.

Load-bearing premise

The lens transform preserves the essential asymptotic information of solutions without introducing significant numerical artifacts or altering the scattering behavior in the regimes studied.

What would settle it

A computation showing that the numerical scattering operator does not preserve quantities like the L2 norm or fails to match known scattering data in the defocusing case would disprove the method's validity.

Figures

Figures reproduced from arXiv: 2506.11560 by Georg Maierhofer (DAMTP), R\'emi Carles (IRMAR).

Figure 1
Figure 1. Figure 1: The action of the scattering operator on different initial conditions. of each conserved quantity in u+ with that of u−, where we use the following notation: I1(u) = ∥u∥L2 , I2(u) = ∥∇u∥ 2 L2 , I3(u) = Im Z Rd u(x)∇u(x)dx, I4(u) = Z Rd x|u(x)| 2 dx. The results are shown in [PITH_FULL_IMAGE:figures/full_fig_p014_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: The error in conservation laws (1.11)-(1.14) for a range of randomly chosen initial conditions. 3.3. Rotating-points in the L 2 -critical case. As discussed in Section 2.3, the scattering operator S has a selection of fixed/rotating points which are given as so￾lutions to (2.4). We can solve this equation numerically by expanding the unknown [PITH_FULL_IMAGE:figures/full_fig_p014_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: The action of the scattering operator on rotating point initial conditions. Note since rotating points provide a known reference value for Su, we can use this information to verify the convergence properties of our methodology. In Fig￾ure 4 we observe the error committed in our approximation of S for both of the aforementioned fixed points as a function of the timestep in the lens-transformed system (1.17)… view at source ↗
Figure 4
Figure 4. Figure 4: Convergence behaviour of our method for known ref￾erence values in the rotating point case. supercritical case σ > 2/d. To test this we performed the following steps for a given σ > 2/d. (1) Based on the continuity arguments outlined in Appendix C we solve (2.4) for the specific value of σ > 2/d, and use this to initialise u−; (2) For this value of u− we try to find the optimal θ such that θ0 = argminθ∈[0,… view at source ↗
Figure 5
Figure 5. Figure 5: The error observed in pseudo-rotating points in the supercritical r´egime. -50 -40 -30 -20 -10 0 10 20 30 40 50 x -0.25 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0.15 0.2 0.25 Re Su! Re u! (a) Real part. -50 -40 -30 -20 -10 0 10 20 30 40 50 x -0.25 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0.15 0.2 0.25 Im Su! Im u! (b) Imaginary part. 10-2 10-1 100 :=2 ! tlens 10-2 10-1 100 101 E s tim a t e o f kjvj2 ! limt !v :=2 jvj2kL2… view at source ↗
Figure 6
Figure 6. Figure 6: The action of the scattering operator and convergence of the numerical method in long-range case [PITH_FULL_IMAGE:figures/full_fig_p017_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: The time-evolution of the Σ-norm of the lens￾transformed variable v with τlens = 2−14 , ∥v0∥∞ = 10 [PITH_FULL_IMAGE:figures/full_fig_p019_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: The L∞-norm evolution for v0 = αϕ1/2 with τlens = 2 −14, M = 8096 [PITH_FULL_IMAGE:figures/full_fig_p021_8.png] view at source ↗
read the original abstract

We analyse the scattering operator associated with the defocusing nonlinear Schr{\"o}dinger equation which captures the evolution of solutions over an infinite time-interval under the nonlinear flow of this equation. The asymptotic nature of the scattering operator (involving unbounded time) makes its computation particularly challenging. We overcome this by exploiting the space-time compactification provided by the lens transform, marking the first use of this technique in numerical simulations. This results in a highly efficient and reliable methodology for computing the scattering operator in various regimes. In developing this approach we introduce and prove several new identities and theoretical properties of the scattering operator. We support our construction with several numerical experiments which we show to agree with known analytical properties of the scattering operator, and also address the case of long-range scattering for the one-dimensional cubic Schr{\"o}dinger equation. Our simulations permit us to further explore regimes beyond current analytical understanding, and lead us to formulate new conjectures concerning fixed and rotating points of the operator, as well as its existence in the long-range setting for both defocusing and focusing cases.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. This paper introduces the use of the lens transform for numerical computation of the scattering operator associated with the defocusing nonlinear Schrödinger equation. By compactifying space-time, the method allows efficient simulation over infinite time intervals. New theoretical identities are proved, numerical experiments validate against known analytical results including long-range 1D cubic scattering, and new conjectures on fixed/rotating points and long-range existence are proposed.

Significance. The significance lies in bridging analytical and numerical approaches to scattering problems in NLS. If the lens transform preserves asymptotic behavior without artifacts, this could become a standard tool for exploring scattering in various regimes. The paper's strength is in providing both proofs of new properties and numerical support for conjectures, with validation against independent analytical knowledge rather than circular fitting.

major comments (1)
  1. Numerical experiments section: the central claim of a 'highly efficient and reliable methodology' for the scattering operator rests on the lens transform introducing no significant artifacts, yet the manuscript provides no quantitative convergence studies, error bars, or comparisons to alternative discretizations to confirm preservation of asymptotic information in the long-range 1D cubic regime.
minor comments (2)
  1. The abstract and introduction would benefit from explicit mention of the spatial dimensions and power nonlinearities considered in the main numerical tests beyond the general defocusing case.
  2. Notation for the transformed variables in the theoretical identities section could be clarified with a short table or diagram to aid readers unfamiliar with the lens transform.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their positive assessment of the manuscript and for the constructive comment, which we address below. We agree that additional quantitative validation will strengthen the presentation of the numerical methodology.

read point-by-point responses
  1. Referee: Numerical experiments section: the central claim of a 'highly efficient and reliable methodology' for the scattering operator rests on the lens transform introducing no significant artifacts, yet the manuscript provides no quantitative convergence studies, error bars, or comparisons to alternative discretizations to confirm preservation of asymptotic information in the long-range 1D cubic regime.

    Authors: We thank the referee for highlighting this point. The current numerical experiments are validated by direct agreement with known analytical results for long-range scattering in the 1D cubic case, providing independent confirmation that the lens transform preserves the relevant asymptotic information. We nevertheless acknowledge that quantitative convergence studies, error bars, and comparisons to alternative discretizations would offer stronger support for the absence of artifacts. In the revised manuscript we will add such studies, including mesh-refinement tests and error estimates focused on the long-range 1D cubic regime. revision: yes

Circularity Check

0 steps flagged

No significant circularity

full rationale

The paper derives new theoretical identities and proves preservation properties of the scattering operator under the lens transform in a self-contained manner. Numerical experiments recover known external analytical features (including long-range 1D cubic cases) and generate new conjectures, rather than fitting parameters or redefining inputs by construction. No load-bearing step reduces to the paper's own outputs or unverified self-citations; the methodology is validated against independent benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review provides no explicit free parameters, axioms, or invented entities; full manuscript required for complete ledger.

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Reference graph

Works this paper leans on

51 extracted references · 51 canonical work pages · 1 internal anchor

  1. [1]

    J. E. Barab. Nonexistence of asymptotically free solutions for nonlinear Schr¨ odinger equation. J. Math. Phys. , 25:3270–3273, 1984

  2. [2]

    Ben Abdallah, F

    N. Ben Abdallah, F. Castella, and F. M´ ehats. Time averaging for the strongly confined nonlin- ear Schr¨ odinger equation, using almost periodicity.J. Differential Equations, 245(1):154–200, 2008

  3. [3]

    B. F. Bunck. A fast algorithm for evaluation of normalized hermite functions. BIT Numerical Mathematics, 49(2):281–295, 2009

  4. [4]

    N. Burq, V. Georgiev, N. Tzvetkov, and N. Visciglia. H 1 scattering for mass-subcritical NLS with short-range nonlinearity and initial data in Σ. Ann. Henri Poincar´ e, 24(4):1355–1376, 2023

  5. [5]

    Burq and L

    N. Burq and L. Thomann. Almost sure scattering for the one dimensional nonlinear Schr¨ odinger equation, volume 1480 of Mem. Am. Math. Soc. Providence, RI: American Math- ematical Society (AMS), 2024

  6. [6]

    N. Burq, L. Thomann, and N. Tzvetkov. Long time dynamics for the one dimensional non linear Schr¨ odinger equation.Ann. Inst. Fourier, 63(6):2137–2198, 2013

  7. [7]

    R. Carles. Geometric optics and long range scattering for one-dimensional nonlinear Schr¨ odinger equations.Comm. Math. Phys. , 220(1):41–67, 2001

  8. [8]

    R. Carles. Critical nonlinear Schr¨ odinger equations with and without harmonic potential. Math. Models Methods Appl. Sci. , 12(10):1513–1523, 2002

  9. [9]

    R. Carles. Remarks on nonlinear Schr¨ odinger equations with harmonic potential.Ann. Henri Poincar´ e, 3(4):757–772, 2002

  10. [10]

    R. Carles. Rotating points for the conformal NLS scattering operator. Dyn. Partial Differ. Equ., 6(1):35–51, 2009

  11. [11]

    R. Carles. Time splitting and error estimates for nonlinear Schr¨ odinger equations with a potential. Preprint, archived at https://hal.science/hal-04677959, 2024

  12. [12]

    Carles and I

    R. Carles and I. Gallagher. Analyticity of the scattering operator for semilinear dispersive equations. Comm. Math. Phys. , 286(3):1181–1209, 2009

  13. [13]

    Carles and L

    R. Carles and L. Gosse. Numerical aspects of nonlinear Schr¨ odinger equations in the presence of caustics. Math. Models Methods Appl. Sci. , 17(10):1531–1553, 2007

  14. [14]

    Carles and T

    R. Carles and T. Ozawa. On the wave operators for the critical nonlinear Schr¨ odinger equation critical nonlinear Schr¨ odinger equation.Math. Res. Lett., 15(1):185–195, 2008

  15. [15]

    Carles and C

    R. Carles and C. Su. Numerical study of the logarithmic Schr¨ odinger equation with repulsive harmonic potential. Discrete Contin. Dyn. Syst., Ser. B , 28(5):3136–3159, 2023

  16. [16]

    Cazenave

    T. Cazenave. Semilinear Schr¨ odinger equations, volume 10 ofCourant Lecture Notes in Math- ematics. New York University Courant Institute of Mathematical Sciences, New York, 2003

  17. [17]

    Cazenave and F

    T. Cazenave and F. Weissler. Rapidly decaying solutions of the nonlinear Schr¨ odinger equa- tion. Comm. Math. Phys. , 147:75–100, 1992

  18. [18]

    Chen and J

    G. Chen and J. Murphy. Recovery of the nonlinearity from the modified scattering map. Int. Math. Res. Not. , 2024(8):6632–6655, 2024

  19. [19]

    J. Cronin. Fixed points and topological degree in nonlinear analysis . Mathematical Surveys, No. 11. American Mathematical Society, Providence, RI, 1964

  20. [20]

    https://dlmf.nist.gov/, Release 1.2.4 of 2025-03-15

    NIST Digital Library of Mathematical Functions . https://dlmf.nist.gov/, Release 1.2.4 of 2025-03-15. F. W. J. Olver, A. B. Olde Daalhuis, D. W. Lozier, B. I. Schneider, R. F. Boisvert, C. W. Clark, B. R. Miller, B. V. Saunders, H. S. Cohl, and M. A. McClain, eds

  21. [21]

    Duyckaerts, F

    T. Duyckaerts, F. Merle, and S. Roudenko. Maximizers for the Strichartz norm for small solutions of mass-critical NLS. Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) , 10(2):427–476, 2011

  22. [22]

    Ehrenfest

    P. Ehrenfest. Bemerkung ¨ uber die angenaherte G¨ ultigkeit der klassischen Mechanik innerhalb der Quantenmechanik. Zeitschrift f¨ ur Physik, 45(7-8):455–457, 1927

  23. [23]

    Gauckler

    L. Gauckler. Convergence of a split-step Hermite method for the Gross-Pitaevskii equation. IMA J. Numer. Anal. , 31(2):396–415, 2011

  24. [24]

    J. Ginibre. Introduction aux ´ equations de Schr¨ odinger non lin´ eaires. In French. Cours de DEA,

  25. [25]

    Archived at http://sites.mathdoc.fr/PMO/PDF/G_GINIBRE-48

    Paris Onze ´Edition. Archived at http://sites.mathdoc.fr/PMO/PDF/G_GINIBRE-48. pdf

  26. [26]

    Ginibre and G

    J. Ginibre and G. Velo. On a class of nonlinear Schr¨ odinger equations. I The Cauchy problem, general case. J. Funct. Anal., 32:1–32, 1979

  27. [27]

    Ginibre and G

    J. Ginibre and G. Velo. On a class of nonlinear Schr¨ odinger equations. II Scattering theory, general case. J. Funct. Anal., 32:33–71, 1979

  28. [28]

    Hayashi and P

    N. Hayashi and P. Naumkin. Asymptotics for large time of solutions to the nonlinear Schr¨ odinger and Hartree equations.Amer. J. Math. , 120(2):369–389, 1998. RIGIDITY PROPERTIES AND NUMERICS FOR NLS SCATTERING 27

  29. [29]

    Hayashi and P

    N. Hayashi and P. Naumkin. Domain and range of the modified wave operator for Schr¨ odinger equations with a critical nonlinearity. Comm. Math. Phys. , 267(2):477–492, 2006

  30. [30]

    Hayashi and Y

    N. Hayashi and Y. Tsutsumi. Remarks on the scattering problem for nonlinear Schr¨ odinger equations. In Differential equations and mathematical physics (Birmingham, Ala., 1986) , volume 1285 of Lectures Notes in Math. , page 162–168. Springer, Berlin, 1987

  31. [31]

    B. Helffer. Th´ eorie spectrale pour des op´ erateurs globalement elliptiques, volume 112 of Ast´ erisque. Soci´ et´ e Math´ ematique de France, Paris, 1984. With an English summary

  32. [32]

    Kato and F

    J. Kato and F. Pusateri. A new proof of long-range scattering for critical nonlinear Schr¨ odinger equations.Differ. Integral Equ., 24(9-10):923–940, 2011

  33. [33]

    Kavian and F

    O. Kavian and F. Weissler. Self-similar solutions of the pseudo-conformally invariant nonlinear Schr¨ odinger equation.Michigan Math. J. , 41(1):151–173, 1994

  34. [34]

    Modified wave operators for the defocusing cubic nonlinear Schr\"odinger equation in one space dimension with large scattering data

    M. Kawamoto and H. Mizutani. Modified wave operators for the defocusing cubic nonlinear Schr¨ odinger equation in one space dimension with large scattering data. Preprint, archived at https://arxiv.org/abs/2506.01871, 2025

  35. [35]

    Killip, J

    R. Killip, J. Murphy, and M. Visan. The scattering map determines the nonlinearity. Proc. Amer. Math. Soc., 151(6):2543–2557, 2023

  36. [36]

    Killip, J

    R. Killip, J. Murphy, and M. Visan. Determination of Schr¨ odinger nonlinearities from the scattering map. Nonlinearity, 38(1):015021, 2025

  37. [37]

    Maierhofer and M

    G. Maierhofer and M. Webb. A note on stable Hermite transforms, 2025. In preparation

  38. [38]

    J. Mawhin. Topological degree methods in nonlinear boundary value problems , volume 40 of Reg. Conf. Ser. Math. American Mathematical Society (AMS), Providence, RI, 1979

  39. [39]

    Nakanishi and T

    K. Nakanishi and T. Ozawa. Remarks on scattering for nonlinear Schr¨ odinger equations. NoDEA Nonlinear Differential Equations Appl. , 9(1):45–68, 2002

  40. [40]

    T. Ozawa. Long range scattering for nonlinear Schr¨ odinger equations in one space dimension. Comm. Math. Phys. , 139:479–493, 1991

  41. [41]

    Poiret, D

    A. Poiret, D. Robert, and L. Thomann. Probabilistic global well-posedness for the supercrit- ical nonlinear harmonic oscillator. Anal. PDE, 7(4):997–1026, 2014

  42. [42]

    J. Rauch. Partial Differential Equations , volume 128 of Graduate Texts in Math. Springer- Verlag, New York, 1991

  43. [43]

    A. V. Rybin, G. G. Varzugin, M. Lindberg, J. Timonen, and R. K. Bullough. Similarity solutions and collapse in the attractive Gross-Pitaevskii equation. Phys. Rev. E (3) , 62(5, part A):6224–6228, 2000

  44. [44]

    H. Sasaki. The inverse scattering problem for Schr¨ odinger and Klein-Gordon equations with a nonlocal nonlinearity. Nonlinear Anal., Theory Methods Appl., Ser. A, Theory Methods , 66(8):1770–1781, 2007

  45. [45]

    R. M. Slevinsky, S. Olver, et al. Fasttransforms.jl. https://github.com/ JuliaApproximation/FastTransforms.jl, 2025. Version 0.17.0

  46. [46]

    T. Tao. A pseudoconformal compactification of the nonlinear Schr¨ odinger equation and ap- plications. New York J. Math. , 15:265–282, 2009

  47. [47]

    Thalhammer, M

    M. Thalhammer, M. Caliari, and C. Neuhauser. High-order time-splitting Hermite and Fourier spectral methods. J. Comput. Phys. , 228(3):822–832, 2009

  48. [48]

    Townsend, S

    A. Townsend, S. Olver, et al. Fastgaussquadrature.jl. https://github.com/ JuliaApproximation/FastGaussQuadrature.jl, 2024. Version 1.0.2

  49. [49]

    Tsutsumi

    Y. Tsutsumi. Scattering problem for nonlinear Schr¨ odinger equations.Ann. Inst. H. Poincar´ e Phys. Th´ eor., 43(3):321–347, 1985

  50. [50]

    Tsutsumi and K

    Y. Tsutsumi and K. Yajima. The asymptotic behavior of nonlinear Schr¨ odinger equations. Bull. Amer. Math. Soc. (N.S.) , 11(1):186–188, 1984

  51. [51]

    M. Webb. Quantumtimesteppers.jl. https://github.com/marcusdavidwebb/ QuantumTimeSteppers.jl, 2025. Accessed on 07/05/2025. (R. Carles) CNRS, IRMAR - UMR 6625, Rennes, France Email address: Remi.Carles@math.cnrs.fr (G. Maierhofer) Department of Applied Mathematics and Theoretical Physics, Uni- versity of Cambridge, United Kingdom Email address: gam37@cam.ac.uk