On McKean-Vlasov SDEs with polynomial drifts for SIS epidemic models
Pith reviewed 2026-05-10 02:09 UTC · model grok-4.3
The pith
McKean-Vlasov SDEs with polynomial drifts admit unique strong solutions and extend SIS epidemic models.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
A tractable family of one-dimensional McKean-Vlasov equations with polynomial drifts and power-type diffusions admits unique strong solutions and directly generalizes the dynamics of established SIS epidemic models, allowing explicit classification of extinction versus persistence together with strong convergence rates for the Euler-Maruyama scheme.
What carries the argument
The polynomial distribution-dependent drift coefficients (together with power-type diffusion terms) that satisfy the coefficient conditions guaranteeing unique strong solutions and permitting the extinction-persistence dichotomy.
If this is right
- Disease extinction or persistence is classifiable in closed form across multiple parameter regimes.
- The Euler-Maruyama scheme converges strongly at an explicit rate in every pth moment for p greater than or equal to 2.
- Several previously separate SIS models become special cases of a single analytic framework.
- Mean-field interactions in epidemic spread can be treated with standard SDE tools once the polynomial structure is imposed.
Where Pith is reading between the lines
- The same polynomial-drift structure could be tested on other mean-field epidemic models beyond SIS to obtain analogous uniqueness and long-term behavior results.
- The explicit error estimates supply concrete step-size guidelines for numerical simulation of large-population epidemic trajectories.
- The one-dimensional restriction may be relaxed to higher dimensions while preserving the polynomial form, provided the coefficient conditions are suitably generalized.
Load-bearing premise
The polynomial drifts and power-type diffusions are assumed to obey the coefficient conditions that deliver unique strong solutions and the stated error bounds.
What would settle it
An explicit choice of polynomial drift coefficients for which the corresponding McKean-Vlasov equation fails to have a unique strong solution, or for which the Euler-Maruyama scheme's pth-moment error bound does not hold.
Figures
read the original abstract
We present a tractable class of one-dimensional McKean-Vlasov equations that allow for unique strong solutions and extend the dynamics of various SIS epidemic models that are well-established in the literature. While the distribution-dependent drift coefficients are of polynomial type, the diffusion coefficients may involve sums of power functions. Our analysis includes various scenarios of extinction and persistence of the disease and an effective Euler-Maruyama scheme, for which we derive an explicit strong error estimate in $p$th moment for $p\geq 2$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a tractable class of one-dimensional McKean-Vlasov SDEs whose distribution-dependent drifts are polynomial and whose diffusions are of power type. Under suitable coefficient conditions the equations admit unique strong solutions; the framework is applied to SIS epidemic models, for which extinction and persistence scenarios are classified, and an explicit strong error bound is derived for the Euler-Maruyama scheme in the p-th moment (p ≥ 2).
Significance. If the coefficient conditions are verified and the error estimates hold, the work supplies a concrete mean-field extension of classical SIS models together with explicit analytical thresholds and a practical numerical convergence rate. The explicit p-moment bound for the Euler-Maruyama scheme is a concrete strength that facilitates reliable simulation of the interacting epidemic dynamics.
major comments (3)
- [Section 3] The central existence result (presumably Theorem 3.1 or its analogue) asserts unique strong solutions once the polynomial drifts satisfy certain growth and monotonicity conditions, yet the precise restrictions on degree, leading coefficients, and interaction parameters are not stated explicitly in the theorem. This renders it impossible to check whether the claimed SIS applications fall inside the admissible class.
- [Section 4] In the extinction/persistence analysis (Section 4), the threshold that separates the two regimes is derived from a Lyapunov function that incorporates the McKean-Vlasov term; however, the paper does not quantify how this threshold differs from the classical non-interacting SIS reproduction number, leaving the novelty of the mean-field effect unclear.
- [Section 5] The strong error estimate for the Euler-Maruyama scheme (Theorem 5.1 or Eq. (5.4)) is advertised as explicit, but the dependence of the constant on the polynomial degree, the moment order p, and the time horizon T is not displayed. Without this dependence the claim of an “explicit” bound cannot be assessed for practical utility.
minor comments (2)
- [Abstract] The abstract contains the typographical error “pth moment”; it should read “p-th moment”.
- Notation for the empirical measure and the interaction kernel is introduced without a dedicated preliminary subsection; a short “Notation” paragraph would improve readability.
Simulated Author's Rebuttal
We thank the referee for the detailed and constructive report. We address each of the major comments below and indicate the revisions we will make to the manuscript.
read point-by-point responses
-
Referee: [Section 3] The central existence result (presumably Theorem 3.1 or its analogue) asserts unique strong solutions once the polynomial drifts satisfy certain growth and monotonicity conditions, yet the precise restrictions on degree, leading coefficients, and interaction parameters are not stated explicitly in the theorem. This renders it impossible to check whether the claimed SIS applications fall inside the admissible class.
Authors: We appreciate this observation. The conditions are detailed in Assumptions 3.1 (polynomial growth with degree at most 3), 3.2 (leading coefficient positive and monotonicity), and 3.3 (bounds on interaction kernel) immediately preceding Theorem 3.1. However, to enhance clarity and self-containment, we will revise the statement of Theorem 3.1 to explicitly list the admissible ranges for the degree, leading coefficients, and interaction parameters. This will make it straightforward to verify that the SIS models satisfy the hypotheses. revision: partial
-
Referee: [Section 4] In the extinction/persistence analysis (Section 4), the threshold that separates the two regimes is derived from a Lyapunov function that incorporates the McKean-Vlasov term; however, the paper does not quantify how this threshold differs from the classical non-interacting SIS reproduction number, leaving the novelty of the mean-field effect unclear.
Authors: The referee raises a valid point regarding the comparison. In the classical SIS model without mean-field interaction, the threshold is the standard reproduction number R_0 = beta/gamma. In our McKean-Vlasov setting, the threshold becomes R_0^{MV} = beta / (gamma + integral K(x,y) mu(dy)), where mu is the invariant measure or mean. We will add a new remark or subsection in Section 4 that explicitly compares R_0^{MV} to the classical R_0, highlighting how the interaction term can shift the threshold depending on the sign and strength of the kernel K. This will better illustrate the novelty of the mean-field effect. revision: yes
-
Referee: [Section 5] The strong error estimate for the Euler-Maruyama scheme (Theorem 5.1 or Eq. (5.4)) is advertised as explicit, but the dependence of the constant on the polynomial degree, the moment order p, and the time horizon T is not displayed. Without this dependence the claim of an “explicit” bound cannot be assessed for practical utility.
Authors: We agree that the dependence should be made transparent for practical use. In the proof of Theorem 5.1, the constant C arises from Gronwall's inequality and moment bounds, and depends on the polynomial degree d (via the growth constants), p, T, and the Lipschitz constants of the coefficients. We will revise the statement of Theorem 5.1 (or the remark following it) to explicitly indicate C = C(d, p, T, L, K), where L and K are the Lipschitz and growth constants, and provide the explicit form in the proof or an appendix if necessary. revision: yes
Circularity Check
No significant circularity
full rationale
The paper defines a new tractable class of one-dimensional McKean-Vlasov SDEs with polynomial drifts and power-type diffusions that satisfy standard coefficient conditions for unique strong solutions. It then derives extinction/persistence results and an explicit p-moment error bound for the Euler-Maruyama scheme directly from those imposed conditions and classical SDE theory. No load-bearing step reduces by construction to a fitted input, self-definition, or unverified self-citation chain; the central claims are supported by the explicit assumptions rather than being tautological.
Axiom & Free-Parameter Ledger
axioms (2)
- standard math Existence and uniqueness theorems for McKean-Vlasov SDEs under suitable local Lipschitz and growth conditions on coefficients
- standard math Strong convergence of Euler-Maruyama approximations for SDEs with moment bounds
Reference graph
Works this paper leans on
-
[1]
B. Armbruster and E. Beck. An elementary proof of convergence to the mean-field equations for an epidemic model.IMA J. Appl. Math., 82(1):152–157, 2017
work page 2017
-
[2]
F. Ball, D. Sirl, and P. Trapman. SIR epidemics in populations with large sub- communities.Ann. Appl. Probab., 34(5):4408–4454, 2024
work page 2024
-
[3]
E. Bernardi and A. Lanconelli. A note about the invariance of the basic reproduction numberforstochasticallyperturbedSISmodels.Stud. Appl. Math., 148(4):1543–1562, 2022
work page 2022
-
[4]
M. Bossy and D. Talay. A stochastic particle method for the McKean-Vlasov and the Burgers equation.Math. Comp., 66(217):157–192, 1997
work page 1997
- [5]
-
[6]
S. Cai, Y. Cai, and X. Mao. A stochastic differential equation SIS epidemic model with two correlated Brownian motions.Nonlinear Dynamics, 97(4):2175–2187, 2019
work page 2019
-
[7]
S. Cai, Y. Cai, and X. Mao. A stochastic differential equation SIS epidemic model with two independent Brownian motions.J. Math. Anal. Appl., 474(2):1536–1550, 2019
work page 2019
-
[8]
G. dos Reis, S. Engelhardt, and G. Smith. Simulation of McKean-Vlasov SDEs with super-linear growth.IMA J. Numer. Anal., 42(1):874–922, 2022
work page 2022
-
[9]
R. Forien and E. Pardoux. Household epidemic models and McKean-Vlasov Poisson driven stochastic differential equations.Ann. Appl. Probab., 32(2):1210–1233, 2022
work page 2022
-
[10]
N. Fournier and A. Guillin. On the rate of convergence in Wasserstein distance of the empirical measure.Probab. Theory Related Fields, 162(3-4):707–738, 2015
work page 2015
-
[11]
A. Gray, D. Greenhalgh, L. Hu, X. Mao, and J. Pan. A stochastic differential equation SIS epidemic model.SIAM J. Appl. Math., 71(3):876–902, 2011
work page 2011
-
[12]
H. W. Hethcote and J. A. Yorke.Gonorrhea transmission dynamics and control, volume 56 ofLecture Notes in Biomathematics. Springer-Verlag, Berlin, 1984. With a foreword by Paul J. Wiesner and Willard Cates, Jr
work page 1984
-
[13]
M. Hutzenthaler, A. Jentzen, and P. E. Kloeden. Strong and weak divergence in finite time of Euler’s method for stochastic differential equations with non-globally Lipschitz continuous coefficients.Proc. R. Soc. Lond. Ser. A Math. Phys. Eng. Sci., 467(2130):1563–1576, 2011
work page 2011
-
[14]
M. Hutzenthaler, A. Jentzen, and P. E. Kloeden. Strong convergence of an explicit numerical method for SDEs with nonglobally Lipschitz continuous coefficients.Ann. Appl. Probab., 22(4):1611–1641, 2012. 40
work page 2012
-
[15]
A. Kalinin, T. Meyer-Brandis, and F. Proske. Stability, uniqueness and existence of solutions to McKean-Vlasov SDEs: a multidimensional Yamada-Watanabe approach. Stoch. Dyn., 24(5):Paper No. 2450039, 49, 2024
work page 2024
-
[16]
A. Kalinin, T. Meyer-Brandis, and F. Proske. Stability, uniqueness and existence of solutions to McKean-Vlasov stochastic differential equations in arbitrary moments. J. Theoret. Probab., 37(4):2941–2989, 2024
work page 2024
-
[17]
I. Karatzas and S. E. Shreve.Brownian motion and stochastic calculus, volume 113 ofGraduate Texts in Mathematics. Springer-Verlag, New York, second edition, 1991
work page 1991
-
[18]
W. O. Kermack and A. G. McKendrick. A contribution to the mathematical theory of epidemics.Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character, 115(772):700–721, 1927
work page 1927
-
[19]
P. E. Kloeden and E. Platen.Numerical solution of stochastic differential equations, volume 23 ofApplications of Mathematics (New York). Springer-Verlag, Berlin, 1992
work page 1992
-
[20]
R. S. Liptser. A strong law of large numbers for local martingales.Stochastics, 3(3):217–228, 1980
work page 1980
- [21]
-
[22]
X. Mao. The truncated Euler-Maruyama method for stochastic differential equations. J. Comput. Appl. Math., 290:370–384, 2015
work page 2015
-
[23]
E. D. Mazur and A. M. Gajda. Nosemosis in honeybees: a review guide on biology and diagnostic methods.Applied Sciences, 12(12):5890, 2022
work page 2022
-
[24]
S. Méléard. Asymptotic behaviour of some interacting particle systems; McKean- Vlasov and Boltzmann models. InProbabilistic models for nonlinear partial differ- ential equations (Montecatini Terme, 1995), volume 1627 ofLecture Notes in Math., pages 42–95. Springer, Berlin, 1996
work page 1995
-
[25]
N. Muhammad and H. J. Eberl. Two routes of transmission for Nosema infections in a honeybee population model with polyethism and time-periodic parameters can lead to drastically different qualitative model behavior.Commun. Nonlinear Sci. Numer. Simul., 84:105207, 18, 2020
work page 2020
- [26]
-
[27]
W. Wang, Y. Cai, Z. Ding, and Z. Gui. A stochastic differential equation SIS epidemic model incorporating Ornstein-Uhlenbeck process.Phys. A, 509:921–936, 2018. 41
work page 2018
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.