REVIEW 2 major objections 6 minor 71 references
Resonances and computations
T0 review · 2 major / 6 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read The review argues that resonance-based integrators, which embed the nonlinear frequency interactions of a dispersive PDE into the discretisation, reliably approximate solutions from much rougher initial data than splitting and exponential…
desk verdict A readable survey of the authors' resonance-based integrators; the advertised low-regularity convergence, however, is proven only for filtered variants, not the displayed schemes. 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 machine that carries the argument is a decorated tree series: each tree encodes one iterated Duhamel integral, with frequencies decorating the edges and nodes, together with the associated elementary differential in the initial data and a symmetry factor. The decisive algebraic input is the resonance decomposition of the dispersion relation, $L = L_{\mathrm{dom}} + L_{\mathrm{low}}$, where $L_{\mathrm{dom}}$ is exactly integrable; for KdV, $L_{\mathrm{low}} = 3k_1 k_2 (k_1+k_2)$ via the factorisation identity, and for NLS, $L_{\mathrm{dom}} = 2k_1^2$ with $L_{\mathrm{low}}$ the remainder. A coproduct on decorated trees, defined by admissible cuts, organises the calculation of $L_{\mathrm{low}}$ for each tree and leads to a Birkhoff-type factorisation of the discretisation map, which is how schemes of arbitrary order are constructed in a systematic way. For the error analysis, the paper introduces a frequency cutoff $\Pi_\tau$ projecting onto $|k| \leq \tau^{-1/3}$, so that discrete Bourgain-type spaces reproduce the frequency interactions of the continuous problem, and it surveys the discrete bilinear estimates that convert the local error into global $L^2$ convergence.
What would settle it
Run the resonance-based first-order scheme (28) on periodic KdV with initial data in $H^s$ for $s$ between $-1$ and $0$, comparing the $L^2$ error at a fixed time against a highly resolved spectral solution; if the error fails to decay at the predicted order in $\tau$ as $\tau \to 0$, the low-regularity guarantee collapses. Alternatively, replace the KdV dispersion $k^3$ by $k^4$, so that $k^4 - k_1^4 - k_2^4$ does not factor into linear terms, and check whether the first Duhamel iterate can still be integrated exactly; failure of that factorisation would mark the boundary of the method's range.
Extended reading notes
Core claim
On the paper's own terms, the core discovery is that the obstacle to rough-data approximation is not the oscillation itself but the way classical schemes linearise it. For KdV, the identity $k^3 - k_1^3 - k_2^3 = 3k_1 k_2 (k_1+k_2)$ turns the phase in the first Duhamel iterate into a product that can be integrated exactly and written back in physical space using only inverse derivatives. The same structural splitting, $L = L_{\mathrm{dom}} + L_{\mathrm{low}}$ with $L_{\mathrm{dom}}$ exactly integrable and expressible by ordinary differential operators, is claimed to hold for a wide class of dispersive equations, including cubic NLS where $L_{\mathrm{dom}} \neq 0$ and must be integrated exactly while $L_{\mathrm{low}}$ is Taylor expanded. The paper argues that with a decorated-tree series tracking frequencies and iterated integrals, this resonance analysis extends to arbitrarily high order, producing schemes whose local error is controlled by powers of the low part $L_{\mathrm{low}}$ rather than the full dispersion operator $L$.
Load-bearing premise
The advertised gains stand on two pillars: the equation's frequency law must split into an exactly integrable dominant part and a milder remainder, and the error analysis needs a discrete bilinear estimate together with a frequency cutoff; the first is verified for KdV and NLS, the second is quoted from earlier papers rather than proved here.
Editorial extensions
If this is right
- For periodic KdV, the first-order resonance scheme (28) has local error $O(\tau^2 \partial_x^2 u)$ and the second-order scheme (29) has $O(\tau^3 \partial_x^4 u)$, compared with the five and six additional derivatives demanded respectively by Strang splitting and second-order exponential integrators.
- The same resonance analysis applies to cubic NLS with a nonzero dominant part $L_{\mathrm{dom}} = 2k_1^2$, giving schemes that combine exact integration of the dominant phase with Taylor expansion of the lower part.
- Symmetric, time-reversible low-regularity schemes such as the midpoint variants (30) can be derived by choosing symmetric Duhamel iterations and interpolation points, preserving the symmetries of the continuous problem at the discrete level.
- With the frequency cutoff $|k| \leq \tau^{-1/3}$, the filtered scheme can be analysed in discrete Bourgain-type spaces, yielding $L^2$ error estimates at low regularity for KdV, as surveyed in Section 4.
- The decorated-tree formalism with its coproduct gives a recursive formula for the regularity-embedding operator appearing in the local error, so higher-order resonance-based schemes can be built without hand computation.
Reading between the lines
- Because the decisive step is algebraic, one testable extension is to search for other dispersive equations whose frequency-interaction polynomials factor into linear terms; for those, the same exact-integration trick should lower the regularity requirement without changing the decorated-tree machinery.
- The role of the cutoff suggests a practical tuning knob: choosing the Fourier cutoff as a function of the actual regularity of the data, rather than fixing it at $\tau^{-1/3}$, might allow adaptive schemes that degrade gracefully as the data become rougher, a direction the review does not pursue.
- The Hopf-algebraic formulation implies that the resonance-based schemes could be combined with renormalisation-type procedures, which is where structure preservation (symmetry and ultimately symplecticity in higher dimensions) would most plausibly be achieved; the paper notes that symplectic low-regularity schemes in dimension greater than one remain open.
- A numerical experiment comparing the filtered resonance scheme against a spectral reference for KdV at Sobolev exponents below zero would directly test how far the low-regularity claim extends past the $H^s$, $s>0$ regime covered by the $L^2$ analysis; the paper's formalism suggests the method may still behave, but the review does not claim this.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This survey-style paper advertises a class of resonance-based integrators for nonlinear dispersive PDEs, with periodic KdV as the running example. It contrasts the regularity requirements of splitting and exponential integrators with the new schemes, derives first- and second-order resonance-based schemes via a decorated-tree formalism, presents an implicit symmetric variant, and sketches an L2 error analysis at low regularity using discrete Bourgain spaces. The central claim is that embedding the nonlinear frequency interactions into the discretisation yields reliable approximation for much rougher data than classical methods can handle.
Significance. If the advertised low-regularity convergence were established for the schemes as displayed, this would be a valuable contribution: it would extend rigorous numerical approximation of dispersive PDEs below the regularity thresholds of splitting and exponential integrators, and the decorated-tree formalism offers a systematic route to higher-order and structure-preserving variants. The paper is clearly written, gives explicit schemes, and is honest that the deeper analytic estimates and the general local-error theorem are imported from earlier papers ([14, 61, 66]). However, the paper's own Remark 2 states that a frequency cutoff is needed for the discrete Bourgain analysis, and the convergence theory in Section 4 is explicitly carried out only for a filtered version of the scheme, while the schemes displayed in Section 3 contain no such cutoff. As it stands, the low-regularity claim is therefore proved only for filtered variants, not for the methods as written.
major comments (2)
- [Section 3, Corollaries 1–2 (Eqs. (28)–(30)) and Section 4, Remark 2 (Eqs. (47)–(48))] The low-regularity L2 convergence analysis in Section 4 is performed only for a 'filtered version of (30)' with the sharp frequency projection Π_τ onto |k| ≤ τ^{-1/3}, and Remark 2 states that this cutoff is 'crucial in our estimates'. The schemes displayed in Corollaries 1 and 2 contain no such projection. Consequently, the discrete Bourgain bilinear estimate (47) and the factorisation (20) do not apply to the methods as presented, and the abstract and Section 2.3 overstate what is proved: the advertised rough-data reliability is established only for the filtered variants. Please either add the cutoff to the displayed schemes or explicitly qualify the abstract and Section 2.3 so that the low-regularity convergence claim is restricted to the filtered schemes, with the unfiltered Corollaries presented as formal local-error constructions.
- [Section 3, Corollary 1 (Eq. (29)) and Section 4, Eq. (47)] The second-order scheme (29) contains a smooth filter Ψ satisfying |τ Ψ(iτ∂_x^2)∂_x^2| ≤ 1, but this is not the sharp projection Π_τ used in the discrete Bourgain estimate (47). If the intended interpretation is that Ψ is a regularisation that can replace Π_τ, the equivalence is not shown; if not, the L2 convergence theory does not cover (29). This distinction should be made explicit, and the role of the filter in the proof should be clarified.
minor comments (6)
- [Abstract] There is a typo: 'inpiration' should be 'inspiration'.
- [Section 2.1] There are typos: 'separetely' should be 'separately' and 'symetrised' should be 'symmetrised'.
- [Section 3] There are typos: 'Unfortunatly' should be 'Unfortunately', 'descritisation' should be 'discretisation', and 'teh context' should be 'the context'.
- [Section 4] The phrase 'Lady Windamere's fan argument' should be 'Lady Windermere's fan argument'.
- [References] There are duplicate entries in the reference list: '[37, 37]' appears in the introduction and '[66, 66]' appears near the end of Section 4; please deduplicate.
- [Section 3, Corollary 1] The filter function Ψ is introduced with a norm condition ‖τΨ(iτ∂_x^2)∂_x^2‖_F ≤ 1, but the space/norm denoted by F is not defined; please clarify.
Circularity Check
No demonstrable circularity: the resonance reduction is an explicit algebraic identity and the error analysis cites prior published proofs rather than the target claim.
full rationale
The paper is a review of the authors' own resonance-based integrator program, and it is heavily self-cited, but none of its central steps reduces to its inputs by construction. The key mechanism for KdV is the explicit algebraic factorization k^3 - k1^3 - k2^3 = 3 k1 k2 (k1+k2), displayed in Eq. (20), which is derived in the text from the Duhamel formulation and is not an input-output tautology. The general local-error result is stated as Theorem 1 and explicitly attributed to prior work [14]; the discrete Bourgain bilinear estimate (47) is attributed to [61, 66]. These are self-citations, but they refer to externally published, peer-reviewed proofs and are not presented as consequences of the current paper's conclusion. No parameter is fitted to a subset of data and then renamed as a prediction; no uniqueness theorem is imported from the authors' prior work to forbid alternatives; and the decorated-tree formalism is presented as a bookkeeping device, not as a substitute for proof. A genuine caveat exists: Section 4 analyzes a filtered version of the scheme (Remark 2, Eq. (47)), while Corollaries 1 and 2 display unfiltered schemes, so the low-regularity convergence proof does not directly cover the displayed schemes as written. That is a rigor/scope gap, not circularity. The modest score of 2 reflects only the self-citation-heavy survey format, not any identified circular reduction.
Assumptions & free parameters
free parameters (2)
- Filter function Ψ =
unspecified; any filter with Ψ(0)=1 and ||τ Ψ(iτ ∂_x^2) ∂_x^2|| ≤ 1
- Frequency cutoff exponent =
τ^{-1/3}
assumptions (5)
- domain assumption The iterated Duhamel expansion is encoded in a convergent decorated tree series with truncation error O(t^{F+1}) (Eq. 19).
- standard math The dispersion relation for KdV satisfies the factorization k^3 - k1^3 - k2^3 = 3 k1 k2 (k1+k2) (Eq. 20).
- ad hoc to paper The operator L admits a decomposition L = L_dom + L_low with L_dom of a form that can be mapped back to physical space (Eq. 22 and discussion).
- domain assumption The discrete Bourgain spaces satisfy Lemma 1, Lemma 2 and the bilinear estimate (47) uniformly in τ.
- ad hoc to paper The frequency cutoff Π_τ at |k| ≤ τ^{-1/3} does not alter the resonance structure and enables the discrete Bourgain estimates (Remark 2).
Cite this review
Pith. "Pith review of Resonances and computations." pith.science (2026). https://pith.science/paper/QDKNJ5WU
@misc{pith2026250419647,
author = {Pith},
title = {Pith review of: Resonances and computations},
year = {2026},
howpublished = {\url{https://pith.science/paper/QDKNJ5WU}},
note = {Machine review of arXiv:2504.19647}
}
read the original abstract
The computation of time dynamics arising in nonlinear time-dependent partial differential equations is an ongoing challenge in numerical analysis, especially once roughness comes into play. Classical numerical schemes in general fail to resolve the oscillatory behaviour in the solution which leads to numerical instabilities and loss of convergence. Dispersive equations, e.g., nonlinear Schr\"odinger, Korteweg--de Vries and wave equations, thereby pose in particular a big problem as in contrast to the parabolic setting, no strong smoothing can be expected, i.e., if the initial data is rough, the solution stays rough which makes their approximation a delicate task. In this review we give an overview on a new numerical ansatz which aims to tackle the time dynamics of nonlinear dispersive partial differential equations even for very rough data. This is achieved by a resonance analysis and decorated tree formalism that draws its inpiration from the combinatorics used in the theory of regularity structures for solving singular SPDEs. One can hope to see this formalism applied in other contexts for dispersive PDEs and beyond.
Reference graph
Works this paper leans on
-
[1]
J-P . Berrut, L.N. Trefethen, Barycentric Lagrange Interpolation. SIAM Review 46 (2004)
work page 2004
-
[2]
J. Bernier, B. Gr ´ebert, Long Time Dynamics for Generalized Korteweg–de Vries and Be n- jamin–Ono Equations. Arch Rational Mech Anal 241:1139–1241 (2021)
work page 2021
-
[3]
Y . Alama Bronsard, Y . Bruned, K. Schratz. Low regularity integrators via decorated trees. arXiv:2202.01171
-
[4]
Y . Alama Bronsard, Y . Bruned, G. Maierhofer, K. Schratz. Symmetric resonance based integrators and forest formulae. arXiv:2305.16737
-
[5]
Y . Alama Bronsard, Y . Bruned, K. Schratz. Approximations of Dispersive PDEs in the Presence of Low-Regularity Randomness. Found. Comput. Math. 24, (2024), 1819–1869
work page 2024
-
[6]
J. Armstrong-Goodall, Y . Bruned. Resonance based schemes for SPDEs. arXiv:2312.16690
-
[7]
Low regularity symplectic schemes for stochastic NLS
J. Armstrong-Goodall, Y . Bruned. Low regularity symplectic schemes for stochastic NLS. arXiv:2410.22359
-
[8]
J. Bourgain, Fourier transform restriction phenomena for certain latti ce subsets and appli- cations to nonlinear evolution equations. Part II: The KDV E quation. Geom. Funct. Anal. 3:209–262 (1993)
work page 1993
Show all 71 references
-
[9]
Bruned, A
Y . Bruned, A. Chandra, I. Chevyrev, M. Hairer, Renormalising SPDEs in regularity structures. J. Eur. Math. Soc. (JEMS), 23, no. 3, (2021), 869-947
2021
-
[10]
Bringmann Y
B. Bringmann Y . Deng, A. Nahmod, H. Yue . Invariant Gibbs measures for the three dimen- sional cubic nonlinear wave equation . Invent. Math. 236, (2024), 1133–1411
2024
-
[11]
Bruned, M
Y . Bruned, M. Hairer, L. Zambotti, Algebraic renormalisation of regularity structures. Invent. Math. 215, no. 3, (2019), 1039–1156
2019
-
[12]
Y . Bruned. Composition and substitution of Regularity Structures B-series . arXiv:2310.14242
-
[13]
Y . Bruned. Derivation of normal forms for dispersive PDEs via arborific ation . arXiv:2409.03642
-
[14]
Bruned, K
Y . Bruned, K. Schratz. Resonance based schemes for dispersive equations via decorated trees. Forum of Mathematics, Pi, 10, E2
-
[15]
Bruned, L
Y . Bruned, L. Tolomeo. Cancellations for dispersive PDEs with random initial data . arXiv:2412.17051
-
[16]
J. C. Butcher, An algebraic theory of integration methods. Math. Comp. 26, (1972), 79–106
1972
-
[17]
Celledoni, D
E. Celledoni, D. Cohen, B. Owren, Symmetric exponential integrators with an application to the cubic Schr ¨odinger equation. Found. Comput. Math. 8, (2008), 303–317
2008
-
[18]
Christ, Power series solution of a nonlinear Schr¨odinger equation
M. Christ, Power series solution of a nonlinear Schr¨odinger equation. In Mathematical aspects of nonlinear dispersive equations, volume 163 of Ann. of Math. Stud., pages 131–155. Princeton Univ. Press, Princeton, NJ, 2007
2007
-
[19]
Chartier, E
P . Chartier, E. Hairer, G. Vilmart, Algebraic structures of B-series. Found. Comput. Math. 10, no. 4, (2010), 407–427
2010
-
[20]
Colliander, M
J. Colliander, M. Keel, G. Staffilani, H. Takaoka and T. Tao . Sharp global well-posedness for KdV and modified KdV on R and T. J. Amer. Math. Soc. 16 (2003), no. 3, 705–749
2003
-
[21]
Connes, D
A. Connes, D. Kreimer, Hopf algebras, renormalization and noncommutative geomet ry. Comm. Math. Phys. 199, no. 1, (1998), 203–242
1998
-
[22]
Connes, D
A. Connes, D. Kreimer, Renormalization in quantum field theory and the Riemann-Hil bert problem I: the Hopf algebra structure of graphs and the main t heorem. Commun. Math. Phys. 210, (2000), 249–73
2000
-
[23]
Y . Deng, Z. Hani. Full derivation of the wave kinetic equation . Invent. math. 233, (2023), 543-724
2023
-
[24]
Y . Deng, Z. Hani. Derivation of the wave kinetic equation: Full range of scali ng laws . arXiv:2301.07063
-
[25]
Deng, A.R
Y . Deng, A.R. Nahmod, H. Yue. Random tensors, propagation of randomness, and nonlinear dispersive equations. Invent. math. 228, (2022), 539–686
2022
-
[26]
Ecalle Les fonctions r ´esurgentes
J. Ecalle Les fonctions r ´esurgentes. Tome I, II and III [Mathematical Publications of Orsay 81 and 85]. Universit´e de Paris-Sud, D ´epartement de Math ´ematique, Orsay, 1981 and 1985. 24 Yvain Bruned, Fr ´ed´eric Rousset, and Katharina Schratz
1981
-
[27]
Ecalle Singularit´es non abordables par la g ´eom´etrie
J. Ecalle Singularit´es non abordables par la g ´eom´etrie. (French) [Singularities that are inac- cessible by geometry] Ann. Inst. Fourier (Grenoble) 42 (199 2), no. 1-2, 73–164
-
[28]
Ecalle, B
J. Ecalle, B. Vallet. The arborification-coarborification transform: analytic, combinatorial, and algebraic aspects. Ann. Fac. Sci. Toulouse (6) 13, no. 3, (2004), 575–657
2004
-
[29]
Engquist, A
B. Engquist, A. Fokas, E. Hairer, A. Iserles, Highly Oscillatory Problems. Cambridge Univer- sity Press, 2009
2009
-
[30]
Fauvet and F
F. Fauvet and F. Menous, Ecalle’s arborification coarborification transforms and Co nnes Kreimer Hopf algebra, Annales Sc. de l’Ecole Normale Sup. 50, no. 1, (2017), 39-83
2017
-
[31]
Faou, Geometric Numerical Integration and Schr ¨odinger Equations
E. Faou, Geometric Numerical Integration and Schr ¨odinger Equations. European Math. Soc. Publishing House, Z¨ urich 2012
2012
-
[32]
Z. Guo, S. Kwon, T. Oh, Poincar´e-Dulac normal form reduction for unconditional well- posedness of the periodic cubic NLS , Comm. Math. Phys. 322, no. 1, (2013), 19–48
2013
-
[33]
Gubinelli, Controlling rough paths
M. Gubinelli, Controlling rough paths. J. Funct. Anal. 216, no. 1, (2004), 86–140
2004
-
[34]
Gubinelli, Ramification of rough paths
M. Gubinelli, Ramification of rough paths. J. Differ. Equ. 248, no. 4, (2010), 693 – 721
2010
-
[35]
Gubinelli, Rough solutions for the periodic Korteweg-de Vries equation
M. Gubinelli, Rough solutions for the periodic Korteweg-de Vries equation. Comm. Pure Appl. Anal. 11, no. 4, (2012), 709–733
2012
-
[36]
Hairer, A theory of regularity structures
M. Hairer, A theory of regularity structures. Invent. Math. 198, no. 2, (2014), 269–504
2014
-
[37]
Hairer, C
E. Hairer, C. Lubich, G. Wanner, Geometric numerical integration. Structure-preserving a l- gorithms for ordinary differential equations. second ed., vol. 31 of Springer Series in Compu- tational Mathematics, Springer-Verlag, Berlin, 2006
2006
-
[38]
Holden, K
H. Holden, K. H. Karlsen, N. H. Risebro, T. Tao, Operator splitting methods for the Korteweg- de Vries equation. Math. Comp. 80, (2011), 821–846
2011
-
[39]
Holden, K
H. Holden, K. H. Karlsen, K.-A. Lie, N. H. Risebro, Splitting for Partial Differential Equations with Rough Solutions. European Math. Soc. Publishing House, Z¨ urich, 2010
2010
-
[40]
Holden, C
H. Holden, C. Lubich, N. H. Risebro, Operator splitting for partial differential equations with Burgers nonlinearity. Math. Comp. 82:173–185 (2012)
2012
-
[41]
Hochbruck, J
M. Hochbruck, J. Leibold, A. Ostermann, On the convergence of Lawson methods for semilinear stiff problems. Numer. Math. 145, (2020), 553–580
2020
-
[42]
Hochbruck, A
M. Hochbruck, A. Ostermann, Exponential integrators. Acta Numer. 19, (2010), 209–286
2010
-
[43]
Hofmanov ´a, K
M. Hofmanov ´a, K. Schratz, An oscillatory integrator for the KdV equation, Numer. Math. 136, (2017), 1117-1137
2017
-
[44]
Hundsdorfer, J
W. Hundsdorfer, J. Verwer, Numerical Solution of Time-Dependent Advection- Diffusion - Reaction Equations. Springer, Berlin, 2003
2003
-
[45]
Ignat, E
L. Ignat, E. Zuazua, Numerical dispersive schemes for the nonlinear Schr ¨odinger equation. SIAM J. Numer. Anal. 47, no. 2, (2009), 1366–1390
2009
-
[46]
Jahnke, C
T. Jahnke, C. Lubich, Error bounds for exponential operator splittings. BIT, 40, (2000), 735– 744
2000
-
[47]
L. Ji, A. Ostermann, F. Rousset, K. Schratz, Low regularity full error estimates for the cubic nonlinear Schr¨odinger equation. SIAM J. Numer. Anal. 62, (2024), 2071–2086
2024
-
[48]
Encyclopedia of Applied and Computational Mathematics
S. Jin, Schr¨odinger equation: Computation, Invited contribution to Springer “Encyclopedia of Applied and Computational Mathematics”, ed. by B. Engquist , pp. 1299-1301, 2015
2015
-
[49]
C. E. Kenig, G. Ponce and L. Vega. A bilinear estimate with applications to the KdV equation. J. Amer. Math. Soc. 9 (1996), no. 2, 573–603
1996
-
[50]
Klein, Fourth order time-stepping for low dispersion Korteweg-de Vries and nonlinear Schr¨odinger equation
C. Klein, Fourth order time-stepping for low dispersion Korteweg-de Vries and nonlinear Schr¨odinger equation. ETNA 29, (2008), 116–135. http://eudml.org/doc/117659
2008
-
[51]
B. Li, S. Ma, K. Schratz, A semi-implicit low-regularity integrator for Navier-Stokes equations. SIAM J. Numer. Anal. 60, (2022), 2273–2292
2022
-
[52]
Linares, G
F. Linares, G. Ponce, Introduction to Nonlinear Dispersive Equations.Second edition. Springer, New Y ork, 2015
2015
-
[53]
D. Levy, G. Puppo, G. Russo, Compact central WENO schemes for multidimensional conser- vation laws, SIAM J. Sci. Comp. 22:656–672 (2000)
2000
-
[54]
V .T. Luan, A. Ostermann, Exponential B-series: The stiff case SIAM J. Numer. Anal. 51, no. 6, (2013), 3431–3445
2013
-
[55]
Lubich, On splitting methods for Schr ¨odinger–Poisson and cubic nonlinear Schr ¨odinger equations
C. Lubich, On splitting methods for Schr ¨odinger–Poisson and cubic nonlinear Schr ¨odinger equations. Math. Comp. 77:2141–2153 (2008) Resonances and computations 25
2008
-
[56]
T. J. Lyons, Differential equations driven by rough signals. Rev. Mat. Iberoamericana 14, no. 2, (1998), 215–310
1998
-
[57]
McLachlan, G.R.W
R.I. McLachlan, G.R.W. Quispel, splitting methods. Acta Numer. 11, (2002), 341–434
2002
-
[58]
Maierhofer, K
G. Maierhofer, K. Schratz. Bridging the gap/colon.up symplecticity and low regularity in Runge-Kutta resonance-based schemes. arXiv:2205.05024
-
[59]
Murua, J.M
A. Murua, J.M. Sanz-Serna, Word Series for Dynamical Systems and Their Numerical Inte- grators. Found. Comp. Math. 17, (2017), 675–712
2017
-
[60]
Ostermann, F
A. Ostermann, F. Rousset, K. Schratz, Error estimates of a Fourier integrator for the cubic Schr¨odinger equation at low regularity. Found. Comput. Math. 21, (2021), 725-765
2021
-
[61]
Ostermann, F
A. Ostermann, F. Rousset, K. Schratz, Fourier integrator for periodic NLS: low regularity estimates via discrete Bourgain spaces. J. Eur. Math. Soc. (JEMS), 25, No. 10, (2023), 3913– 3952
2023
-
[62]
Ostermann, F
A. Ostermann, F. Rousset, K. Schratz, Error estimates at low regularity of splitting schemes for NLS. Math. Comp. 91 (2021), no. 333, 169–182
2021
-
[63]
Ostermann, K
A. Ostermann, K. Schratz, Low regularity exponential-type integrators for semiline ar Schr¨odinger equations, Found. Comput. Math. 18, (2018), 731–755
2018
-
[64]
Ostermann, C
A. Ostermann, C. Su, Two exponential-type integrators for the ”good” Boussines q equation. Numer. Math. 143, (2019), 683–712
2019
-
[65]
Rousset, K
F. Rousset, K. Schratz, A general framework of low regularity integrators. SIAM J. Numer. Anal. 59, no. 3, (2021), 1735–1768
2021
-
[66]
Rousset, K
F. Rousset, K. Schratz, Convergence error estimates at low regularity for time disc retizations of KdV. Pure Appl. Anal. 4 (2022), no. 1, 127–152
2022
-
[67]
Rousset, K
F. Rousset, K. Schratz, Resonances as a computational tool. Found. Comput. Math. 2024 (online first) 10.1007/s10208-024-09665-8
2024 doi
-
[68]
Sanz-Serna, M.P
J.M. Sanz-Serna, M.P . Calvo, Numerical Hamiltonian Problems. Chapman and Hall, London, 1994
1994
-
[69]
Schratz, Y
K. Schratz, Y . Wang, X. Zhao, Low-regularity integrators for nonlinear Dirac equations. Math. Comp. 90, (2021), 189-214
2021
-
[70]
Tao, Nonlinear dispersive equations
T. Tao, Nonlinear dispersive equations. Local and global analysis . Amer. Math. Soc., Provi- dence RI, 2006
2006
-
[71]
Unterberger
J. Unterberger. H¨older-Continuous Rough Paths by Fourier Normal Ordering. Comm. Math. Phys. 298, (2010), 1–36
2010
Reviewed August 16, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.