pith. sign in

arxiv: 2604.19187 · v1 · submitted 2026-04-21 · 🧮 math.PR

Entrance measures and dynamics for time-inhomogeneous McKean-Vlasov stochastic differential equations

Pith reviewed 2026-05-10 02:32 UTC · model grok-4.3

classification 🧮 math.PR
keywords McKean-Vlasov SDEstime-inhomogeneousentrance measuresperiodic measuresquasi-periodic measuresrandom dynamical systemscylinder lift
0
0 comments X

The pith

Existence of entrance measures holds for time-inhomogeneous McKean-Vlasov SDEs even when they expand globally or degenerate over intervals.

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

The paper establishes that entrance measures exist for McKean-Vlasov stochastic differential equations whose coefficients change with time, under conditions broad enough to include global expansion and degeneracy across many intervals. For coefficients that are periodic or quasi-periodic in time it further constructs periodic measures and asymptotic quasi-periodic measures. The argument proceeds by lifting the underlying random dynamical system first to a cylinder and then to the graph of a reparameterized process, producing a continuous semigroup on measures on the cylinder whose invariant measure recovers the desired asymptotic object. A sympathetic reader cares because many interacting-particle models in physics and biology are driven by time-varying forces, and entrance measures supply the natural description of their long-run distributions.

Core claim

The paper shows that entrance measures exist for time-inhomogeneous McKean-Vlasov SDEs in great generality, including when the system expands globally or degenerates over numerous time intervals. When the coefficients are periodic or quasi-periodic in time, periodic measures and asymptotic quasi-periodic measures exist. The construction introduces a double lift of the random dynamical system: first to a dynamical system on the cylinder and then to the graph of the reparameterized process living on the cylinder. The resulting continuous dynamical system on probability measures on the cylinder admits an invariant measure that corresponds to the lifted multi-parameter measure of the asymptotic-

What carries the argument

The double-lifted random dynamical system on the cylinder and the graph of the reparameterized process, which converts the time-inhomogeneous problem into a time-homogeneous continuous semigroup on measures whose invariant measure encodes the entrance law.

If this is right

  • Time-inhomogeneous McKean-Vlasov SDEs admit entrance measures even under repeated global expansion or degeneracy.
  • Periodic coefficients produce periodic entrance measures via the lifted semigroup.
  • Quasi-periodic coefficients produce asymptotic quasi-periodic entrance measures whose lifts are invariant for the cylinder semigroup.
  • The double-lift construction yields a continuous dynamical system on the space of probability measures on the cylinder.

Where Pith is reading between the lines

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

  • The same lifting technique could be applied to other time-dependent mean-field limits to obtain invariant measures without requiring global contraction.
  • Numerical approximation of the lifted semigroup might furnish practical ways to compute the entrance measures for concrete periodic or quasi-periodic models.
  • The framework suggests that stability questions for non-autonomous interacting systems can be reduced to ordinary ergodic theory on an augmented space.

Load-bearing premise

The coefficients must allow construction of a random dynamical system and a double lift to the cylinder and graph that preserves continuity of the induced semigroup on measures.

What would settle it

A specific family of periodic coefficients for which the lifted semigroup on cylinder measures possesses no invariant measure would contradict the existence claim for asymptotic quasi-periodic measures.

read the original abstract

In this paper, we study the entrance measures of time-inhomogeneous McKean-Vlasov SDEs. The existence is obtained in great generality, where the system can be expanding globally and/or degenerate for numerous number of time intervals. When the parameters are periodic/quasi-periodic in time, we obtain the existence of periodic/asymptotic quasi-periodic measures. In this case, a double-lift of the random dynamical system first to a dynamical system on cylinder and then on the graph of reparameterized process living on the cylinder is introduced. The double-lifted system gives to a continuous dynamical system over probability measures on the cylinder, and the lifted multi-parameter measure of the asymptotic quasi-periodic measure can then lead to an invariant measure of the lifted semigroup.

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

2 major / 2 minor

Summary. The paper studies entrance measures for time-inhomogeneous McKean-Vlasov SDEs. It establishes existence of such measures under very general conditions permitting global expansion and/or degeneracy over arbitrarily many time intervals. For periodic or quasi-periodic time dependence in the coefficients, it proves existence of periodic and asymptotic quasi-periodic measures via a double-lift construction: the random dynamical system is first lifted to a dynamical system on the cylinder (augmenting the state by time modulo the period), then to the graph of the reparameterized process; the resulting continuous semigroup on probability measures on the cylinder admits an invariant measure that corresponds to the desired entrance measure.

Significance. If the results hold, the work provides a substantial extension of McKean-Vlasov theory to time-inhomogeneous regimes without requiring global dissipativity or contraction, which is relevant for applications involving mean-field limits with explicit time variation. The double-lift technique for extracting periodic and quasi-periodic measures from the lifted semigroup is a technically interesting contribution that may apply to other classes of stochastic flows. The construction of a continuous dynamical system on measures via concatenation of local flows and graph lifts is a strength when the continuity and invariance arguments are fully rigorous.

major comments (2)
  1. [Introduction / §3 (existence theorem)] The abstract and introduction claim existence 'in great generality' allowing expansion and degeneracy over many intervals, but the precise growth, Lipschitz, or one-sided Lipschitz conditions on the coefficients that guarantee global existence of the McKean-Vlasov SDE and continuous dependence for the RDS concatenation are not stated explicitly in the main existence theorem (presumably Theorem 3.1 or equivalent in §3). Without these, it is difficult to assess whether the claimed generality is achieved or whether hidden regularity is required for the double-lift to preserve continuity of the induced semigroup on measures.
  2. [§4 (periodic case) / double-lift construction] In the periodic case, the double-lift to the cylinder followed by the graph lift is asserted to yield a continuous dynamical system whose invariant measure gives the periodic entrance measure. However, the argument that the lifted multi-parameter measure is indeed invariant for the lifted semigroup (and that this invariance transfers back to the original process) appears to rely on the continuity of the semigroup; a concrete verification that the graph lift commutes with the measure evolution under the given assumptions would strengthen the central claim.
minor comments (2)
  1. [§4] Notation for the cylinder and graph lifts (e.g., the precise definition of the reparameterized process and the multi-parameter measure) should be introduced with a diagram or explicit coordinate description to improve readability.
  2. [Abstract] The abstract states that the system 'can be expanding globally and/or degenerate for numerous number of time intervals'; a brief remark clarifying that the local flows are still well-defined on each finite interval under the standing assumptions would help readers.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major comment below and will incorporate revisions to enhance the clarity of the assumptions and the invariance arguments.

read point-by-point responses
  1. Referee: [Introduction / §3 (existence theorem)] The abstract and introduction claim existence 'in great generality' allowing expansion and degeneracy over many intervals, but the precise growth, Lipschitz, or one-sided Lipschitz conditions on the coefficients that guarantee global existence of the McKean-Vlasov SDE and continuous dependence for the RDS concatenation are not stated explicitly in the main existence theorem (presumably Theorem 3.1 or equivalent in §3). Without these, it is difficult to assess whether the claimed generality is achieved or whether hidden regularity is required for the double-lift to preserve continuity of the induced semigroup on measures.

    Authors: We agree that explicitly stating the conditions in the theorem statement would improve clarity. The paper assumes standard conditions for global existence of McKean-Vlasov SDEs, including local Lipschitz continuity and at most linear growth in the state and measure variables (detailed in Section 2), which permit local expansion and degeneracy over finite time intervals as long as the coefficients remain well-defined. These ensure the RDS concatenation is continuous. We will revise Theorem 3.1 to list these assumptions explicitly, without altering the generality of the result. revision: yes

  2. Referee: [§4 (periodic case) / double-lift construction] In the periodic case, the double-lift to the cylinder followed by the graph lift is asserted to yield a continuous dynamical system whose invariant measure gives the periodic entrance measure. However, the argument that the lifted multi-parameter measure is indeed invariant for the lifted semigroup (and that this invariance transfers back to the original process) appears to rely on the continuity of the semigroup; a concrete verification that the graph lift commutes with the measure evolution under the given assumptions would strengthen the central claim.

    Authors: Thank you for this suggestion. The invariance is established by showing that the graph lift preserves the evolution under the reparameterized flow, using the continuity of the semigroup on the space of measures (which follows from the assumptions in Section 3). To make this more concrete, we will add a detailed verification in the proof of the main theorem in Section 4, including a commutative diagram or step-by-step calculation demonstrating that the lifted measure remains invariant under the semigroup action. This will clarify the transfer back to the original entrance measure. revision: yes

Circularity Check

0 steps flagged

No circularity: existence proofs via standard RDS lifts are self-contained

full rationale

The paper constructs random dynamical systems from the McKean-Vlasov SDE under stated coefficient conditions, then applies a standard double-lift (cylinder for periodic time, graph for reparameterization) to obtain an autonomous continuous semigroup on measures whose invariant measures correspond to the desired periodic or quasi-periodic entrance measures. No equation reduces the target measure to a fitted parameter or to a quantity defined in terms of itself; the lift is an explicit state augmentation whose continuity follows from the assumed Lipschitz/one-sided Lipschitz properties. No self-citations are invoked as load-bearing uniqueness theorems, and the argument does not rename known empirical patterns. The derivation therefore remains independent of its own outputs.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The paper relies on standard background results from the theory of random dynamical systems and McKean-Vlasov SDEs; the new contribution is the double-lift construction rather than new axioms or entities.

axioms (2)
  • domain assumption Existence of a random dynamical system generated by the time-inhomogeneous McKean-Vlasov SDE under the stated generality conditions.
    Invoked to obtain entrance measures and to enable the subsequent lifts to the cylinder and graph.
  • domain assumption Continuity of the induced semigroup on the space of probability measures after the double lift.
    Required for the existence of an invariant measure of the lifted semigroup.

pith-pipeline@v0.9.0 · 5432 in / 1576 out tokens · 35732 ms · 2026-05-10T02:32:43.528145+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

35 extracted references · 35 canonical work pages

  1. [1]

    N. U. Ahmed and X. Ding , On invariant measures of nonlinear Markov processes , J. Appl. Math. Stochastic Anal., 6 (1993), pp. 385–406

  2. [2]

    C. D. Aliprantis and K. C. Border , Infinite dimensional analysis , Springer, Berlin, third ed., 2006. A hitchhiker’s guide

  3. [3]

    J. Bao, M. Scheutzow, and C. Yuan , Existence of invariant probability measures for functional McKean- Vlasov SDEs , Electron. J. Probab., 27 (2022), pp. 1–14

  4. [4]

    O. A. Butkovsky , On ergodic properties of nonlinear Markov chains and stochastic McKean-Vlasov equa- tions, Theory Probab. Appl., 58 (2014), pp. 661–674

  5. [5]

    J. A. Carrillo, R. S. Gvalani, G. A. Pavliotis, and A. Schlichting , Long-time behaviour and phase transitions for the McKean-Vlasov equation on the torus , Arch. Ration. Mech. Anal., 235 (2020), pp. 635–690

  6. [6]

    J. A. Carrillo, R. J. McCann, and C. Villani , Kinetic equilibration rates for granular media and related equations: entropy dissipation and mass transportation estimates , Rev. Mat. Iberoamericana, 19 (2003), pp. 971–1018

  7. [7]

    , Contractions in the 2-Wasserstein length space and thermalization of granular media , Arch. Ration. Mech. Anal., 179 (2006), pp. 217–263. 51

  8. [8]

    Da Prato and J

    G. Da Prato and J. Zabczyk , Ergodicity for infinite-dimensional systems, vol. 229 of London Mathematical Society Lecture Note Series, Cambridge University Press, Cambridge, 1996

  9. [9]

    D. A. Dawson , Critical dynamics and fluctuations for a mean-field model of cooperative behavior , J. Statist. Phys., 31 (1983), pp. 29–85

  10. [10]

    M. G. Delgadino, R. S. Gvalani, G. A. Pavliotis, and S. A. Smith , Phase transitions, logarithmic Sobolev inequalities, and uniform-in-time propagation of chaos for weakly interacting diffusions , Comm. Math. Phys., 401 (2023), pp. 275–323

  11. [11]

    R. M. Dudley , Real analysis and probability , vol. 74 of Cambridge Studies in Advanced Mathematics, Cambridge University Press, Cambridge, 2002. Revised reprint of the 1989 original

  12. [12]

    C. Feng, B. Qu, and H. Zhao , Random quasi-periodic paths and quasi-periodic measures of stochastic differential equations, J. Differential Equations, 286 (2021), pp. 119–163

  13. [13]

    , Entrance measures for semigroups of time-inhomogeneous sdes: possibly degenerate and expanding , arXiv: 2307.07891, (2023)

  14. [14]

    Feng and H

    C. Feng and H. Zhao , Random periodic processes, periodic measures and ergodicity , J. Differential Equa- tions, 269 (2020), pp. 7382–7428

  15. [15]

    C. Feng, H. Zhao, and J. Zhong , Existence of geometric ergodic periodic measures of stochastic differential equations, J. Differential Equations, 359 (2023), pp. 67–106

  16. [16]

    Granas and J

    A. Granas and J. Dugundji , Fixed point theory , Springer Monographs in Mathematics, Springer-Verlag, New York, 2003

  17. [17]

    Guillin, W

    A. Guillin, W. Liu, L. Wu, and C. Zhang , The kinetic Fokker-Planck equation with mean field interaction , J. Math. Pures Appl. (9), 150 (2021), pp. 1–23

  18. [18]

    , Uniform Poincaré and logarithmic Sobolev inequalities for mean field particle systems , Ann. Appl. Probab., 32 (2022), pp. 1590–1614

  19. [19]

    Huang, Z

    W. Huang, Z. Lian, and K. Lu , Dynamical complexity of Anosov systems driven by a quasi-periodic force , Sci. China Math., 68 (2025), pp. 89–136

  20. [20]

    Ikeda and S

    N. Ikeda and S. W atanabe , Stochastic Differential Equations and Diffusion Processes , vol. 24 of North- Holland Mathematical Library, North-Holland Publishing Co., Amsterdam; Kodansha, Ltd., Tokyo, sec- ond ed., 1989

  21. [21]

    Kac , Foundations of kinetic theory , in Proceedings of the Third Berkeley Symposium on Mathematical Statistics and Probability, 1954–1955, vol

    M. Kac , Foundations of kinetic theory , in Proceedings of the Third Berkeley Symposium on Mathematical Statistics and Probability, 1954–1955, vol. III, University of California Press, Berkeley-Los Angeles, Calif., 1956, pp. 171–197

  22. [22]

    O. E. Lanford, III , Time evolution of large classical systems , in Dynamical systems, theory and applications (Rencontres, Battelle Res. Inst., Seattle, Wash., 1974), Lecture Notes in Phys., Vol. 38, Springer, Berlin, 1975, pp. 1–111

  23. [23]

    Liu and K

    R. Liu and K. Lu , Exponential mixing and limit theorems of quasi-periodically forced 2D stochastic Navier- Stokes equations in the hypoelliptic setting , Comm. Math. Phys., 406 (2025), pp. Paper No. 55, 46

  24. [24]

    W. Liu, L. Wu, and C. Zhang , Long-time behaviors of mean-field interacting particle systems related to McKean-Vlasov equations, Comm. Math. Phys., 387 (2021), pp. 179–214

  25. [25]

    H. P. McKean, Jr. , Propagation of chaos for a class of non-linear parabolic equations , in Stochastic Differential Equations (Lecture Series in Differential Equations, Session 7, Catholic Univ., 1967), Air Force Office Sci. Res., Arlington, Va., 1967, pp. 41–57

  26. [26]

    S. A. Muzychka and K. L. V aninsky , A class of nonlinear random walks related to the Ornstein-Uhlenbeck process, Markov Process. Related Fields, 17 (2011), pp. 277–304

  27. [27]

    S. T. Rachev , The Monge-Kantorovich problem on mass transfer and its applications in stochastics , Akademiya Nauk SSSR. Teoriya Veroyatnoste\u ı i ee Primeneniya, 29 (1984), pp. 625–653

  28. [28]

    Ren and F.-Y

    P. Ren and F.-Y. W ang , Exponential convergence in entropy and Wasserstein for McKean-Vlasov SDEs , Nonlinear Anal., 206 (2021), pp. Paper No. 112259, 20

  29. [29]

    Skorohod, Studies in the Theory of Random Processes , Translated from the Russian by Scripta Technica, Inc

    A. Skorohod, Studies in the Theory of Random Processes , Translated from the Russian by Scripta Technica, Inc. Addison-Wesley Publishing Co., Inc., Reading, Mass., 1965. 52

  30. [30]

    Sznitman , Topics in propagation of chaos , in École d’Été de Probabilités de Saint-Flour XIX—1989, vol

    A.-S. Sznitman , Topics in propagation of chaos , in École d’Été de Probabilités de Saint-Flour XIX—1989, vol. 1464 of Lecture Notes in Math., Springer, Berlin, 1991, pp. 165–251

  31. [31]

    Tugaut , Phase transitions of McKean-Vlasov processes in double-wells landscape , Stochastics, 86 (2014), pp

    J. Tugaut , Phase transitions of McKean-Vlasov processes in double-wells landscape , Stochastics, 86 (2014), pp. 257–284

  32. [32]

    Uchiyama, Derivation of the Boltzmann equation from particle dynamics , Hiroshima Math

    K. Uchiyama, Derivation of the Boltzmann equation from particle dynamics , Hiroshima Math. J., 18 (1988), pp. 245–297

  33. [33]

    Villani , Optimal transport, vol

    C. Villani , Optimal transport, vol. 338 of Grundlehren der mathematischen Wissenschaften [Fundamental Principles of Mathematical Sciences], Springer-Verlag, Berlin, 2009. Old and new

  34. [34]

    W ang, Distribution dependent SDEs for Landau type equations , Stochastic Processes and their Appli- cations, 128 (2018), pp

    F.-Y. W ang, Distribution dependent SDEs for Landau type equations , Stochastic Processes and their Appli- cations, 128 (2018), pp. 595–621

  35. [35]

    Zhang , Existence and non-uniqueness of stationary distributions for distribution dependent SDEs , Electron

    S.-Q. Zhang , Existence and non-uniqueness of stationary distributions for distribution dependent SDEs , Electron. J. Probab., 28 (2023), pp. 1–34. 53