pith. sign in

arxiv: 2411.16628 · v3 · submitted 2024-11-25 · 🧮 math.DS

On linear response for discontinuous perturbations of smooth endomorphisms

Pith reviewed 2026-05-23 17:14 UTC · model grok-4.3

classification 🧮 math.DS
keywords linear responsephysical measuresdiscontinuous perturbationssmooth endomorphismsuniform mixingstandard pairsdynamical systemsstatistical stability
0
0 comments X

The pith

Uniform mixing on standard pairs makes the physical measure Lipschitz in the perturbation parameter for discontinuous perturbations of smooth endomorphisms.

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

The paper studies families of maps formed by applying discontinuous perturbations to smooth endomorphisms. When these families obey uniform mixing conditions expressed via standard pairs, the associated physical measures vary Lipschitz continuously with the size of the perturbation. The analysis also addresses linear response, which tracks the first-order change in the measure, and confirms that the abstract mixing conditions hold in at least one concrete example. This supplies a route to statistical stability results in the presence of discontinuities that would otherwise obstruct direct application of smooth perturbation techniques.

Core claim

If a family of discontinuous perturbations of smooth endomorphisms satisfies uniform mixing assumptions on standard pairs, then the physical measure is Lipschitz continuous in the perturbation parameter, and linear response holds for the family.

What carries the argument

Uniform mixing assumptions on standard pairs, which provide quantitative decay of correlations sufficient to bound the variation of the physical measure with the parameter.

If this is right

  • The physical measure changes at most linearly under small changes to the perturbation parameter.
  • A linear response formula for the derivative of the measure with respect to the parameter can be obtained from the mixing assumptions.
  • The result applies whenever the abstract mixing conditions can be verified directly, including in the concrete example treated in the paper.
  • Statistical stability of the physical measure extends to this class of discontinuous perturbations.

Where Pith is reading between the lines

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

  • The same mixing framework could be checked in other discontinuous settings, such as billiards with moving obstacles, to obtain Lipschitz continuity there as well.
  • If the mixing rate can be made explicit, quantitative bounds on the Lipschitz constant become available for numerical checks.
  • The approach may connect to random perturbations by treating noise as a special case of the discontinuous family.

Load-bearing premise

The perturbed family satisfies uniform mixing assumptions on standard pairs.

What would settle it

A concrete family of discontinuous perturbations that obeys the uniform mixing conditions on standard pairs yet has a physical measure whose variation with the parameter is not Lipschitz would falsify the main claim.

Figures

Figures reproduced from arXiv: 2411.16628 by Giovanni Canestrari.

Figure 1
Figure 1. Figure 1: On the left M+ 1,t in red, M+ 2,t in blue, M+ 3,t in green and M+ 4,t in brown, for t = 1/8. On the right, there are the corresponding images. We denote by L A t the transfer operator associated with (5.3). For r0 > 0 that will be specified shortly, we define C u =  (ξ, η) ∈ R 2 : ξη > 0 [PITH_FULL_IMAGE:figures/full_fig_p021_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: S − 0 (left), S − t (center), S − 0 ∪ S− t (right), t = 1 8 . In red and blue, the sets Rt and Bt respectively. Lemma 5.3. For any ϕ ∈ C0 (M), limt→0 R M(ϕ ◦ FA,t − ϕ)dm t = m(ϕ) − Z 1 0 ϕ(s, s)ds. Proof. By a direct computation (see also (Fig.1)), for all t ∈ (0, 1/8], (5.13) L A t 1 − 1 t = 1 1 − t 1M\Ht − 1 t 1Ht , where Ht is the white portion of M in the right side of (Fig.1), i.e., Ht = Dt ∪ Rt, Dt =… view at source ↗
read the original abstract

We consider discontinuous perturbations of smooth endomorphisms and show that if the perturbed family satisfies uniform mixing assumptions on standard pairs the physical measure is Lipschitz in the parameter defying the perturbation. We also study the problem of linear response for this class of perturbations. Finally we discuss the applicability of the abstract assumptions proving linear response for a concrete example.

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 / 0 minor

Summary. The paper proves an abstract result: if a family of discontinuous perturbations of smooth endomorphisms satisfies uniform mixing assumptions on standard pairs (with rates independent of the perturbation parameter), then the physical measures vary Lipschitz continuously with the parameter and linear response holds. It then discusses applicability of the assumptions to a concrete example, claiming linear response for that case.

Significance. The conditional abstract theorem extends linear response theory to a class of discontinuous perturbations under verifiable mixing hypotheses on standard pairs. This is a useful technical contribution in dynamical systems if the mixing conditions can be checked with parameter-independent constants, as the paper attempts for its example.

major comments (1)
  1. [Section discussing applicability to the concrete example] The section discussing the concrete example: the claim that the example satisfies the uniform mixing assumptions on standard pairs with rates independent of the perturbation parameter is asserted but not supported by explicit bounds or a self-contained verification. This verification is load-bearing for transferring the abstract Lipschitz and linear-response conclusions to the example; without it the applicability statement remains conditional on an unconfirmed hypothesis.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading and the constructive comment on the manuscript. We respond to the major comment below.

read point-by-point responses
  1. Referee: [Section discussing applicability to the concrete example] The section discussing the concrete example: the claim that the example satisfies the uniform mixing assumptions on standard pairs with rates independent of the perturbation parameter is asserted but not supported by explicit bounds or a self-contained verification. This verification is load-bearing for transferring the abstract Lipschitz and linear-response conclusions to the example; without it the applicability statement remains conditional on an unconfirmed hypothesis.

    Authors: We agree that the discussion of the concrete example in the manuscript asserts the applicability of the uniform mixing assumptions without providing fully explicit, self-contained bounds on the mixing rates that are independent of the perturbation parameter. While the section offers heuristic arguments and references to related estimates, it does not constitute a complete verification. In the revised manuscript we will expand this section with additional detailed estimates and calculations to establish the parameter-independent rates explicitly, thereby making the transfer of the abstract conclusions to the example rigorous and self-contained. revision: yes

Circularity Check

0 steps flagged

No circularity detected; central result is conditional on external mixing assumptions with no reduction to fitted inputs or self-citation chains

full rationale

The paper's main theorem states that if the perturbed family satisfies uniform mixing assumptions on standard pairs, then the physical measure is Lipschitz in the parameter and linear response holds. This is an implication derived from the assumptions rather than a self-definitional or fitted-input construction. The discussion of applicability to a concrete example is presented as a separate verification step. No quotes or equations in the provided material show any prediction reducing by construction to its inputs, any load-bearing self-citation, or an ansatz smuggled via prior work. The derivation chain remains self-contained against the stated assumptions.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The result rests on the uniform mixing assumption on standard pairs, which is treated as an external hypothesis rather than derived; no free parameters or invented entities are introduced in the abstract statement.

axioms (1)
  • domain assumption The perturbed family satisfies uniform mixing assumptions on standard pairs.
    This is the load-bearing hypothesis invoked to obtain Lipschitz continuity of the physical measure and linear response.

pith-pipeline@v0.9.0 · 5560 in / 1207 out tokens · 19042 ms · 2026-05-23T17:14:23.637436+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Quenched and annealed linear response for some partially hyperbolic skew products

    math.DS 2026-04 unverdicted novelty 7.0

    Establishes quenched and annealed linear response and statistical stability for partially hyperbolic skew products with parameter-dependent base maps, yielding new formulas for the response and moment derivatives.

  2. Linear response for Sinai billiards with small holes

    math.DS 2026-04 unverdicted novelty 7.0

    The conditional survival probability measure for a Sinai billiard with a small hole is differentiable with respect to hole size at zero, and the derivative is computed.

  3. Linear response for Sinai billiards with small holes

    math.DS 2026-04 unverdicted novelty 6.0

    The conditional survival probability measure for Sinai billiards with small holes is differentiable at t=0 and its derivative is computed.

Reference graph

Works this paper leans on

32 extracted references · 32 canonical work pages · cited by 2 Pith papers

  1. [1]

    Bahsoun, S

    W. Bahsoun, S. Galatolo, Linear response due to singularities. , Nonlinearity, 37 (2024)

  2. [2]

    Bahsoun, M

    W. Bahsoun, M. Ruziboev, B. Saussol, Linear response for random dynamical systems. , Adv. Math., 364, 107011–107044 (2020)

  3. [3]

    Baladi, On the susceptibility function of piecewise expanding inte rval maps

    V. Baladi, On the susceptibility function of piecewise expanding inte rval maps. , Commun. Math. Phys., 275, 839–859 (2007)

  4. [4]

    Baladi, Linear response, or else

    V. Baladi, Linear response, or else. , ArXiv e-prints (2014)

  5. [5]

    Baladi, S

    V. Baladi, S. Gou¨ ezel. Good Banach spaces for piecewise hyperbolic maps via interp olation. Ann. de l’Institut Henri Poincar´ e / Analyse non lin´ eaire,26, 1453–1481 (2009)

  6. [6]

    Baladi, S

    V. Baladi, S. Gou¨ ezel. Banach spaces for piecewise cone hyperbolic maps. J. Mod. Dyn., 4, 91–137 (2010)

  7. [7]

    Baladi, D

    V. Baladi, D. Smania, Linear response formula for piecewise expanding unimodal m aps. Nonlinearity, 21, (2008)

  8. [8]

    Baladi, M

    P. Baladi, M. Todd, Linear response for intermittent maps , Commun. Math. Phys., 347, 857–874 (2016)

  9. [9]

    Bonetto, D

    F. Bonetto, D. Daems, J. Lebowitz, Properties of stationary nonequilibrium states in the thermostated periodic Lorenz gas I: the one particle system ., J. Stat. Phys., 101, 35–60 (2000)

  10. [10]

    Butterley, C

    O. Butterley, C. Liverani. Smooth Anosov flows: correlation spectra and stability. J. Mod. Dyn., 1, 147–168 (2007)

  11. [11]

    Buzzi, Intrinsic ergodicity of affine maps in [0, 1]d

    J. Buzzi, Intrinsic ergodicity of affine maps in [0, 1]d. Monatsh. Math., 124, 97–118 (1997)

  12. [12]

    N. I. Chernov, Statistical properties of piecewise smooth hyperbolic sys tems in high dimen- sions., Discr. Cont. Dynam. Syst., 5, 425–448 (1999)

  13. [13]

    N. I. Chernov, D. Dolgopyat, Brownian Brownian Motion - I. , Memoirs of Amer. Math. Soc., 198, (2009)

  14. [14]

    N. I. Chernov, G. L. Eyink, J. L. Lebowitz, Ya. G. Sinai, Steady-state electrical conduction in the periodic Lorentz gas. , Commun. Math. Phys., 154, 569–601 (1993)

  15. [15]

    N. I. Chernov, R. Markarian, Chaotic billiards. , Math. Surveys and Monographs, 127, (2006)

  16. [16]

    De Lima, D

    A. De Lima, D. Smania, Central limit theorem for the modulus of continuity of avera ges of observables on transversal families of piecewise expand ing unimodal maps. , Journ. of the Inst. of Math. of Jussieu, 17, 673–733 (2018)

  17. [17]

    Demers, C

    M. Demers, C. Liverani, Stability of statistical properties in two-dimensional pi ecewise hy- perbolic maps., Trans. Amer. Math. Soc., 360, 4777–4814 (2008)

  18. [18]

    Demers, C

    M. Demers, C. Liverani, Projective cones for sequential dispersing billiards. , Commun. Math. Phys., 401, 841–923 (2023)

  19. [19]

    Demers, N

    M. Demers, N. Kiamari, C. Liverani, Transfer operators in hyperbolic dynamics. An intro- duction., 33 Colloquio Brasilero de Matematica. Brazilian Mathemat ics Colloquiums series, Editora do IMPA, (2021)

  20. [20]

    Dolgopyat, On differentiability of SRB states for partially hyperbolic systems., Invent

    D. Dolgopyat, On differentiability of SRB states for partially hyperbolic systems., Invent. Math., 155, 389–449 (2004)

  21. [21]

    Folland, Real analysis

    G.. Folland, Real analysis. , Pure and Applied Mathematics. John Wiley & Sons, Inc., New York, 2nd edition, (1999)

  22. [22]

    Keller, Stochastic stability in some chaotic dynamical systems

    G. Keller, Stochastic stability in some chaotic dynamical systems. , Monatsh. Math., 94, 313– 333 (1982)

  23. [23]

    Keller, C

    G. Keller, C. Liverani, Stability in the spectrum for transfer operators. , Ann. della Scuola Normale Superiore di Pisa, 28, 141-152 (1999)

  24. [24]

    Korepanov, Linear response for intermittent maps with summable and non summable decay of correlations., Nonlinearity, 29, 1735-1754 (2016)

    A. Korepanov, Linear response for intermittent maps with summable and non summable decay of correlations., Nonlinearity, 29, 1735-1754 (2016)

  25. [25]

    Rohlin, On the fundamental ideas of measure theory

    V. Rohlin, On the fundamental ideas of measure theory. , Amer. Math. Soc. Translation (1952)

  26. [26]

    Ruelle, Differentiation of SRB states

    D. Ruelle, Differentiation of SRB states. , Commun. Math. Phys., 187, 227–241 (1997)

  27. [27]

    Ruelle, Differentiation of SRB states

    D. Ruelle, Differentiation of SRB states. Correction and complements , Commun. Math. Phys., 234, 185–190 (2003)

  28. [28]

    Ruelle, Differentiation of SRB states for hyperbolic flows

    D. Ruelle, Differentiation of SRB states for hyperbolic flows. , Ergod. Theory Dyn. Syst., 28, 613–631 (2008)

  29. [29]

    Ruelle, A review of linear response theory for general differentiabl e dynamical systems

    D. Ruelle, A review of linear response theory for general differentiabl e dynamical systems. , Nonlinearity, 22, 855–870 (2009). 51

  30. [30]

    Ruelle, Linear response theory for diffeomorphisms with tangencies of stable and unsta- ble manifolds—a contribution to the Gallavotti-Cohen chao tic hypothesis

    D. Ruelle, Linear response theory for diffeomorphisms with tangencies of stable and unsta- ble manifolds—a contribution to the Gallavotti-Cohen chao tic hypothesis. , Nonlinearity, 31, 5683–5691 (2018)

  31. [31]

    C.L W ormell, On convergence of linear response formulae in some piecewis e hyperbolic maps., arXiv preprint arXiv:2206.09292, (2022)

  32. [32]

    C.L W ormell, Conditional mixing in deterministic chaos. , Ergod. Theory Dyn. Syst., 44, 1693–1723 (2024). (Giovanni Canestrari) Dipartimento di Fisica e Astronomia, Universit`a di Bologna, Via Irnerio 46, 40126 Bologna, Italy. Email address : giovanni.canestrari3@unibo.it 52