Prove2Me
Navigate
DiscoverCollectionsFormalpediaBlogsUsersMomentumMy Missions+
Prove2Me
⌕
Log in

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

Dynamical Systems

164 missions · 68 completed

Missions

Open96Completed68All164
Algorithmic Game TheoryLinear algebra·Captain: mikedeng1

Uncoupled Dynamics Do Not Lead to Nash Equilibrium 1: Near the Two-Player Unit-Disk Game Γ₀ of Section II, No Uncoupled Dynamic Is Nash-ConvergentResearch Paper

Motivation

Learning in games asks whether players who adjust their strategies over time, by simple rules, end up at a Nash equilibrium. Many adaptive dynamics share one informational feature: each player's adjustment depends on the current play and on that player's own payoff function, but not on the payoffs of the others. Hart and Mas-Colell (AER 2003) call such dynamics uncoupled, and show that this feature alone rules out guaranteed convergence to Nash equilibrium, even for families of games in which every game has exactly one equilibrium. Earlier non-convergence results, such as Shapley's example for fictitious play and the cycling examples of Jordan (1993) and Foster and Young (1998), concern particular dynamics; this one applies to the whole class of uncoupled dynamics. It is one reason the learning literature turned to weaker targets such as correlated equilibrium, which regret-based uncoupled procedures do reach (Hart and Mas-Colell, Econometrica 2000).

The paper proves its theorem in two settings: a two-player game with a continuum of strategies (§II and the Appendix) and a three-player game with two strategies each (§III). This mission formalizes the first setting.

Setting

There are two players, i=1,2i=1,2i=1,2, and j=3−ij=3-ij=3−i denotes the other player. Each player's strategy set is the closed unit disk D={z∈R2:∥z∥≤1}D=\{z\in\mathbb R^2:\|z\|\le1\}D={z∈R2:∥z∥≤1}, and a profile is x=(x1,x2)∈X:=D×Dx=(x^1,x^2)\in X:=D\times Dx=(x1,x2)∈X:=D×D. A game Γ=(u1,u2)\Gamma=(u^1,u^2)Γ=(u1,u2) is a pair of payoff functions on XXX. A profile xˉ\bar xxˉ is a (pure) Nash equilibrium if no player gains by changing only their own strategy. A dynamic for a family U\mathcal UU of games is a vector field F(x;Γ)F(x;\Gamma)F(x;Γ) on XXX for each Γ∈U\Gamma\in\mathcal UΓ∈U, read x˙=F(x;Γ)\dot x=F(x;\Gamma)x˙=F(x;Γ). It is uncoupled if FiF^iFi depends on the game only through uiu^iui: two games of U\mathcal UU in which player iii has the same payoff function give the same Fi(x;⋅)F^i(x;\cdot)Fi(x;⋅) at every x∈Xx\in Xx∈X.

A dynamic is Nash-convergent for U\mathcal UU if, for every Γ∈U\Gamma\in\mathcal UΓ∈U with its Nash equilibrium xˉ(Γ)\bar x(\Gamma)xˉ(Γ):

  1. F(⋅ ;Γ)F(\cdot\,;\Gamma)F(⋅;Γ) is C1C^1C1 on XXX;
  2. F(xˉ(Γ);Γ)=0F(\bar x(\Gamma);\Gamma)=0F(xˉ(Γ);Γ)=0;
  3. all eigenvalues of the 4×44\times44×4 Jacobian matrix of F(⋅ ;Γ)F(\cdot\,;\Gamma)F(⋅;Γ) at xˉ(Γ)\bar x(\Gamma)xˉ(Γ) have negative real parts;
  4. every solution x(t)x(t)x(t) converges to xˉ(Γ)\bar x(\Gamma)xˉ(Γ) as t→∞t\to\inftyt→∞, from any initial condition.

The game Γ0\Gamma_0Γ0​ has payoffs u0i(xi,xj)=−∥xi−φ(xj)∥2u_0^i(x^i,x^j)=-\|x^i-\varphi(x^j)\|^2u0i​(xi,xj)=−∥xi−φ(xj)∥2. Here φ:D→D\varphi:D\to Dφ:D→D is continuous, φ(z)=2z\varphi(z)=2zφ(z)=2z for ∥z∥≤13\|z\|\le\frac13∥z∥≤31​, φ\varphiφ rotates the unit circle by π/4\pi/4π/4, and φ\varphiφ is affine on rays in between. The family U0\mathcal U_0U0​ consists of the games ui(xi,xj)=−∥xi−ξi(xj)∥2u^i(x^i,x^j)=-\|x^i-\xi^i(x^j)\|^2ui(xi,xj)=−∥xi−ξi(xj)∥2 with continuous ξi:D→D\xi^i:D\to Dξi:D→D such that ξi(ξj(xi))=xi\xi^i(\xi^j(x^i))=x^iξi(ξj(xi))=xi has a unique solution. Every such game has a unique Nash equilibrium, and Γ0∈U0\Gamma_0\in\mathcal U_0Γ0​∈U0​ has the equilibrium (0,0)(0,0)(0,0).

Formalization targets

Goal: THEOREM 1 for the game Γ0\Gamma_0Γ0​ of §II

Let U\mathcal UU be a family in which each game has a single Nash equilibrium and which contains every game of U0\mathcal U_0U0​ within some η>0\eta>0η>0 of Γ0\Gamma_0Γ0​. Then

F uncoupled for U ⟹ F is not Nash-convergent for U.F\ \text{uncoupled for}\ \mathcal U\ \Longrightarrow\ F\ \text{is not Nash-convergent for}\ \mathcal U.F uncoupled for U ⟹ F is not Nash-convergent for U.

Milestones

  • the explicit φ\varphiφ has the two required properties, and rotates by an angle in [0,π/4][0,\pi/4][0,π/4] (fn. 21);
  • every game of U0\mathcal U_0U0​ has a unique Nash equilibrium, and that of Γ0\Gamma_0Γ0​ is (0,0)(0,0)(0,0);
  • Lemma 2: for an uncoupled Nash-convergent dynamic on U0\mathcal U_0U0​, at a unique best reply Fi=0F^i=0Fi=0 and the own-strategy Jacobian block JiJ^iJi has eigenvalues with negative real parts;
  • the derivative identity, giving the Jacobian at Γ0\Gamma_0Γ0​ the block form
J=[J1−2J1−2J2J2];J=\begin{bmatrix}J^1&-2J^1\\-2J^2&J^2\end{bmatrix};J=[J1−2J2​−2J1J2​];
  • the coefficient a3=3det⁡(J1)tr⁡(J2)+3det⁡(J2)tr⁡(J1)a_3=3\det(J^1)\operatorname{tr}(J^2)+3\det(J^2)\operatorname{tr}(J^1)a3​=3det(J1)tr(J2)+3det(J2)tr(J1) of λ\lambdaλ in det⁡(J−λI)\det(J-\lambda I)det(J−λI), and Lemma 3: if J1,J2J^1,J^2J1,J2 are stable, then JJJ has an eigenvalue with positive real part;
  • the main-text result: no uncoupled dynamic is Nash-convergent for U0\mathcal U_0U0​;
  • the Appendix: the functions ψa\psi_aψa​ satisfy conditions (1)–(4), and the conclusions of Lemma 2 at Γ0\Gamma_0Γ0​ already follow from the games of U0\mathcal U_0U0​ near Γ0\Gamma_0Γ0​.

A companion statement, that the coupled dynamic x˙=xˉ(Γ)−x\dot x=\bar x(\Gamma)-xx˙=xˉ(Γ)−x is Nash-convergent, shows that the notion of Nash-convergence can be met.

Significance

The theorem identifies an informational obstruction rather than a computational one. Convergence to Nash equilibrium is easy if the dynamic may use the whole game, as the coupled dynamic x˙=xˉ(Γ)−x\dot x=\bar x(\Gamma)-xx˙=xˉ(Γ)−x shows. It fails once each player may react only to their own payoff function, and the failure persists on an arbitrarily small neighborhood of a single game. It explains why no natural adaptive procedure has been found that converges to Nash equilibrium in general, and it motivates the stochastic, finite-memory and correlated-equilibrium variants studied afterwards (for example Hart and Mas-Colell, GEB 2006).

The result is proved in the paper. As far as the curators know, it has no machine-checked proof. A formalization fixes the model precisely. That matters here, because the conclusion depends on details the prose treats lightly: which perturbations the family must contain, what the Jacobian is at boundary points, and which solutions count.

Difficulty

The obvious argument fails because an uncoupled dynamic is a different vector field for each game, and nothing forces the fields to fit together except the uncoupledness constraint. The proof extracts information about F(⋅ ;Γ0)F(\cdot\,;\Gamma_0)F(⋅;Γ0​) from auxiliary games that share one player's payoff with Γ0\Gamma_0Γ0​, and in which that player's best reply is constant. Making those auxiliary games lie in the family is the delicate part: in U0\mathcal U_0U0​ they are immediate, but near Γ0\Gamma_0Γ0​ they require the functions ψa\psi_aψa​ of the Appendix, whose fixed-point conditions (3) and (4) rest on an angle argument. The linear-algebra step is exact: the stability of J1J^1J1 and J2J^2J2 must be shown to force instability of the coupled 4×44\times44×4 matrix through the sign of one coefficient of its characteristic polynomial.

Formalization scope

R2\mathbb R^2R2 is modelled as C\mathbb CC, and rotation by θ\thetaθ is multiplication by eiθe^{i\theta}eiθ. Players are Fin 2, 0-based, and the other player is i + 1. A game is a pair of real functions on C2\mathbb C^2C2, but every definition looks only at its values on X=D×DX=D\times DX=D×D. Nash equilibria are pure equilibria in XXX (fn. 9 notes there are no mixed ones). Derivatives are Fréchet derivatives within XXX. Eigenvalue conditions use the published predicate FatkhullinPolyak.Discrete.IsHurwitz, with the 4×44\times44×4 Jacobian indexed in player-major order. The C1C^1C1 and Jacobian conditions, which the paper imposes on every dynamic it considers, are part of NashConvergent. The single-Nash-equilibrium property is a hypothesis of the goal.

Two encodings are deliberate:

  • The neighborhood. "U\mathcal UU contains a neighborhood of Γ0\Gamma_0Γ0​" is read as the Appendix reads it: U\mathcal UU contains every game of U0\mathcal U_0U0​ close to Γ0\Gamma_0Γ0​ in the sense of fn. 7. This is implied by the literal hypothesis, so the formal theorem is at least as strong. A full neighborhood contains games with several equilibria, so together with the single-equilibrium hypothesis it would make the theorem vacuous.
  • Solutions. Solutions are curves that stay in XXX. If curves were allowed to leave XXX, they would follow values of FFF that no game constrains, and Nash-convergence would fail for every FFF, which makes the goal trivial. The goal must also not be met through an empty family: the hypotheses are jointly satisfiable, for instance by {Γ∈U0:Γ within 1 of Γ0}\{\Gamma\in\mathcal U_0:\Gamma\text{ within }1\text{ of }\Gamma_0\}{Γ∈U0​:Γ within 1 of Γ0​}.

The development needs:

  • calculus of C1C^1C1 maps on a product of disks;
  • spectra of real matrices viewed over C\mathbb CC and the characteristic polynomial of a 4×44\times44×4 block matrix;
  • elementary planar geometry of rotations and radial interpolation.

The linear-algebra milestones (block Jacobian, a3a_3a3​, Lemma 3) are independent of game theory and reusable. Contributions are welcome on any milestone, in any order.

Selected references

  • S. Hart and A. Mas-Colell, Uncoupled Dynamics Do Not Lead to Nash Equilibrium, American Economic Review 93(5), 1830–1836, 2003. https://doi.org/10.1257/000282803322655581
  • S. Hart and A. Mas-Colell, A Simple Adaptive Procedure Leading to Correlated Equilibrium, Econometrica 68(5), 1127–1150, 2000. https://doi.org/10.1111/1468-0262.00153
  • J. S. Jordan, Three Problems in Learning Mixed-Strategy Nash Equilibria, Games and Economic Behavior 5(3), 368–386, 1993. https://doi.org/10.1006/game.1993.1022
  • D. P. Foster and H. P. Young, On the Nonconvergence of Fictitious Play in Coordination Games, Games and Economic Behavior 25(1), 79–96, 1998. https://doi.org/10.1006/game.1997.0615
  • S. Hart and A. Mas-Colell, Stochastic Uncoupled Dynamics and Nash Equilibrium, Games and Economic Behavior 57(2), 286–303, 2006. https://doi.org/10.1016/j.geb.2005.09.007
14 thms2 active usersReviewed
Operations ResearchStochastic SystemsTheoretical Computer Science·Captain: mikedeng1

The Power of Two Choices in Randomized Load Balancing I: In the Limiting Supermarket System the Expected Time Converges to T_d(λ) = Σ λ^((d^i−d)/(d−1))Research Paper

Motivation

Randomized load balancing asks how much a dispatcher gains from a little information. In the supermarket model, jobs arrive at nnn servers and each job inspects a few servers chosen at random before joining one. With one random choice every server is an independent M/M/1 queue, and the expected time a job spends in the system is 1/(1−λ)1/(1-\lambda)1/(1−λ) at load λ\lambdaλ. With two choices it is exponentially smaller as λ→1−\lambda \to 1^-λ→1−. This "power of two choices" underlies the design of distributed schedulers, hashing schemes and server farms, where querying every server is too expensive but querying two is cheap.

Timeline:

  • 1994/1999. Azar, Broder, Karlin and Upfal proved the static version, balanced allocations: throwing nnn balls into nnn bins with d≥2d \ge 2d≥2 choices per ball gives a maximum load of log⁡log⁡n/log⁡d+O(1)\log\log n/\log d + O(1)loglogn/logd+O(1) w.h.p., against Θ(log⁡n/log⁡log⁡n)\Theta(\log n/\log\log n)Θ(logn/loglogn) for one choice (SIAM J. Comput. 1999).
  • 1996. Vvedenskaya, Dobrushin and Karpelevich derived the dynamic limiting equations for d=2d = 2d=2 and showed convergence of their trajectories to the fixed point, without a rate (Problems of Information Transmission 32(1), 1996).
  • 1996/2001. Mitzenmacher, independently, introduced the limiting system for general ddd, proved doubly exponential tails along every trajectory and exponential convergence to the fixed point in a weighted L1L_1L1​ potential, and derived the limiting expected time Td(λ)T_d(\lambda)Td​(λ) (IEEE TPDS 2001). This mission formalizes Section 2 of that paper.

Setting

Customers arrive as a Poisson stream of rate λn\lambda nλn, 0<λ<10<\lambda<10<λ<1, at nnn FIFO servers. Each customer chooses ddd servers independently and uniformly at random with replacement and joins the one holding the fewest customers; service times are exponential with mean 111. Let si(t)s_i(t)si​(t) be the fraction of servers holding at least iii customers at time ttt.

A state is a sequence s=(s0,s1,s2,… )s = (s_0, s_1, s_2, \dots)s=(s0​,s1​,s2​,…) of reals with s0=1s_0 = 1s0​=1, si≥0s_i \ge 0si​≥0 and s0≥s1≥s2≥⋯s_0 \ge s_1 \ge s_2 \ge \cdotss0​≥s1​≥s2​≥⋯. The empty state has s0=1s_0 = 1s0​=1 and si=0s_i = 0si​=0 for i≥1i \ge 1i≥1. As n→∞n \to \inftyn→∞ the tails follow the limiting system

dsidt=λ (si−1d−sid)−(si−si+1)(i≥1),s0=1.(1)\frac{ds_i}{dt} = \lambda\,(s_{i-1}^d - s_i^d) - (s_i - s_{i+1}) \quad (i \ge 1), \qquad s_0 = 1. \tag{1}dtdsi​​=λ(si−1d​−sid​)−(si​−si+1​)(i≥1),s0​=1.(1)

A trajectory is a map t↦s(t)t \mapsto s(t)t↦s(t), t≥0t \ge 0t≥0, whose values are states and whose coordinates satisfy (1) (from the right at t=0t = 0t=0). Throughout, d≥2d \ge 2d≥2 is an integer.

The fixed point is πi=λ(di−1)/(d−1)\pi_i = \lambda^{(d^i - 1)/(d - 1)}πi​=λ(di−1)/(d−1), so π0=1\pi_0 = 1π0​=1, π1=λ\pi_1 = \lambdaπ1​=λ, π2=λ1+d\pi_2 = \lambda^{1+d}π2​=λ1+d. A customer arriving in state sss becomes the iii-th customer of its queue with probability si−1d−sids_{i-1}^d - s_i^dsi−1d​−sid​ and then waits for iii services, so the expected time it spends in the system is

E(s)=∑i=1∞i (si−1d−sid).E(s) = \sum_{i=1}^{\infty} i\,(s_{i-1}^d - s_i^d).E(s)=i=1∑∞​i(si−1d​−sid​).

The target constant is

Td(λ)=∑i=1∞λdi−dd−1.T_d(\lambda) = \sum_{i=1}^{\infty} \lambda^{\frac{d^i - d}{d-1}}.Td​(λ)=i=1∑∞​λd−1di−d​.

Formalization targets

Goal: Corollary 2

For d≥2d \ge 2d≥2 and 0<λ<10 < \lambda < 10<λ<1, Td(λ)<∞T_d(\lambda) < \inftyTd​(λ)<∞, and:

if sj(0)=0 for some j, then E(s(t))→t→∞Td(λ);if s(0) is empty, then E(s(t))≤Td(λ)  ∀t≥0.\text{if } s_j(0) = 0 \text{ for some } j, \text{ then } E(s(t)) \xrightarrow[t\to\infty]{} T_d(\lambda);\qquad \text{if } s(0) \text{ is empty, then } E(s(t)) \le T_d(\lambda) \ \ \forall t \ge 0.if sj​(0)=0 for some j, then E(s(t))t→∞​Td​(λ);if s(0) is empty, then E(s(t))≤Td​(λ)  ∀t≥0.

The hypothesis sj(0)=0s_j(0) = 0sj​(0)=0 holds for every initial state that comes from a finite system.

Milestones, in the order the proof uses them

  • Lemma 2. π\piπ is the unique fixed point of (1) with ∑i≥1si<∞\sum_{i\ge1} s_i < \infty∑i≥1​si​<∞.
  • Theorem 2. If sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj, there are constants N≥1N \ge 1N≥1, 0<α<10<\alpha<10<α<1, β>1\beta>1β>1, γ>0\gamma>0γ>0, independent of ttt, with si(t)≤γ αβis_i(t) \le \gamma\,\alpha^{\beta^i}si​(t)≤γαβi for all i≥Ni \ge Ni≥N, t≥0t \ge 0t≥0. From the empty state, si(t)≤πis_i(t) \le \pi_isi​(t)≤πi​ for all iii and t≥0t \ge 0t≥0.
  • Theorem 3. There are weights wi≥1w_i \ge 1wi​≥1 such that Φ(t)=∑i≥1wi∣si(t)−πi∣\Phi(t) = \sum_{i\ge1} w_i |s_i(t) - \pi_i|Φ(t)=∑i≥1​wi​∣si​(t)−πi​∣ satisfies Φ(t)≤c0e−δt\Phi(t) \le c_0 e^{-\delta t}Φ(t)≤c0​e−δt (δ>0\delta > 0δ>0) whenever Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞, and in particular whenever sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj.
  • Corollary 1. Under the conditions of Theorem 3 (weights wi≥1w_i \ge 1wi​≥1 fixed before the trajectory, with Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞, or sj(0)=0s_j(0) = 0sj​(0)=0 for some jjj), ∑i≥1∣si(t)−πi∣≤c0e−δt\sum_{i\ge1} |s_i(t) - \pi_i| \le c_0 e^{-\delta t}∑i≥1​∣si​(t)−πi​∣≤c0​e−δt.
  • Proof of Corollary 2, display. ∑i≥1i(si−1d−sid)=∑i≥0sid\sum_{i\ge1} i(s_{i-1}^d - s_i^d) = \sum_{i\ge0} s_i^d∑i≥1​i(si−1d​−sid​)=∑i≥0​sid​ for a state with si→0s_i \to 0si​→0.
  • Lemma 4. The drift of (1) is Lipschitz in ℓ1\ell^1ℓ1 on states, with constant 2+2dλ2 + 2d\lambda2+2dλ.

Significance

The comparison T1(λ)=1/(1−λ)T_1(\lambda) = 1/(1-\lambda)T1​(λ)=1/(1−λ) against Td(λ)T_d(\lambda)Td​(λ) is the quantitative content of the power of two choices: the companion mission shows Td(λ)/log⁡T1(λ)→1/log⁡dT_d(\lambda)/\log T_1(\lambda) \to 1/\log dTd​(λ)/logT1​(λ)→1/logd as λ→1−\lambda \to 1^-λ→1−, an exponential improvement. Corollary 2 is what connects that number to the dynamics: it says the fixed point's expected time is actually reached from realistic initial states, and is an upper bound from an empty start. Theorem 2's comparison argument and Theorem 3's weighted potential are reused across the mean-field analysis of load-balancing variants (threshold policies, heterogeneous servers, work stealing), so the formal statements here are templates for that literature.

All results are proved in the paper (Theorem 3's proof is written out for d=2d = 2d=2 with a remark that it extends). None has a machine-checked proof that we know of. The work is formalizing the known arguments for all d≥2d \ge 2d≥2, including the parts the paper delegates to a citation: quasimonotone comparison for countable ODE systems in Theorem 2, and the upper right Dini derivative handling of ∣ϵi∣|\epsilon_i|∣ϵi​∣ in Theorem 3.

Difficulty

The system is infinite-dimensional, so standard finite-dimensional ODE comparison and Lyapunov theorems do not apply as stated. Theorem 2 rests on a monotonicity property (raising the initial tails raises them for all time) that the paper justifies by a coupling intuition and a citation to a comparison theorem for quasimonotone systems; that theorem must be supplied for ℓ∞\ell^\inftyℓ∞-bounded countable systems. The plain L1L_1L1​ distance is nonincreasing along trajectories but does not decay exponentially by a direct estimate; the weights wiw_iwi​ must be built so that every coordinate's contribution to dΦ/dtd\Phi/dtdΦ/dt is dominated by −δwi∣ϵi∣-\delta w_i |\epsilon_i|−δwi​∣ϵi​∣, while staying geometrically bounded so that Φ(0)<∞\Phi(0) < \inftyΦ(0)<∞ under the doubly exponential tails of Theorem 2. Exchanging t→∞t \to \inftyt→∞ with the infinite sum defining EEE needs uniform tail control, which is again Theorem 2.

Formalization scope

  • Namespace PowerTwoChoices.Limit; λ is lam : ℝ, d:Nd : ℕd:N with 2≤d2 \le d2≤d, 0<λ<10 < \lambda < 10<λ<1 in every theorem.
  • A state is x : ℕ → ℝ with x 0 = 1, nonnegative and antitone. A trajectory is s : ℝ → ℕ → ℝ, a state for every t≥0t \ge 0t≥0, with HasDerivWithinAt on Set.Ici 0 for each coordinate i≥1i \ge 1i≥1: right derivative at t=0t = 0t=0, two-sided for t>0t > 0t>0.
  • Exponents are natural numbers: πi=λ∑k<idk\pi_i = \lambda^{\sum_{k<i} d^k}πi​=λ∑k<i​dk, and TdT_dTd​'s iii-th term is λ∑1≤k<idk\lambda^{\sum_{1\le k<i} d^k}λ∑1≤k<i​dk.
  • Φ\PhiΦ, the L1L_1L1​ distance, EEE and TdT_dTd​ are sums in [0,∞][0,\infty][0,∞], so a divergent series is ∞\infty∞, never a default 000. "Converges exponentially" (Definition 2) means Φ(t)≤c0e−δt\Phi(t) \le c_0 e^{-\delta t}Φ(t)≤c0​e−δt for all t≥0t \ge 0t≥0 with real c0c_0c0​ and δ>0\delta > 0δ>0; δ\deltaδ may depend on the trajectory. The paper's d(t)d(t)d(t) is renamed l1Dist.
  • Time is real and t→∞t \to \inftyt→∞ is Filter.atTop.
  • Every theorem quantifies over trajectories; existence of a trajectory from a given state (Picard iteration, cited by the paper) is not part of the mission. The class is nonempty: the constant trajectory at π\piπ is one.
  • Ruled out: summing EEE or TdT_dTd​ as a real tsum (a divergent series would make the upper bound free and the limit attainable by a junk 000), dropping the summability condition in Lemma 2 ((1,1,… )(1,1,\dots)(1,1,…) is also a fixed point), choosing Theorem 3's weights after the trajectory, and stating anything for d=2d = 2d=2 only.
  • Needed infrastructure: comparison principles for quasimonotone countable ODE systems, Dini-derivative Grönwall estimates, and interchange of limits and ℓ1\ell^1ℓ1 sums. All of these are reusable beyond this mission, and contributions of such lemmas as separate theorems are welcome.

Selected references

  • M. Mitzenmacher, The Power of Two Choices in Randomized Load Balancing, IEEE Transactions on Parallel and Distributed Systems 12(10), 2001, pp. 1094–1104. https://doi.org/10.1109/71.963420
  • Y. Azar, A. Z. Broder, A. R. Karlin, E. Upfal, Balanced Allocations, SIAM Journal on Computing 29(1), 1999, pp. 180–200. https://doi.org/10.1137/S0097539795288490
  • N. D. Vvedenskaya, R. L. Dobrushin, F. I. Karpelevich, Queueing System with Selection of the Shortest of Two Queues: An Asymptotic Approach, Problems of Information Transmission 32(1), 1996, pp. 15–27.
  • T. G. Kurtz, Approximation of Population Processes, SIAM, 1981. https://doi.org/10.1137/1.9781611970333
8 thms2 active usersReviewed
Control TheoryOperations Research·Captain: mikedeng1

Dynamic Instabilities and Stabilization Methods in Distributed Real-Time Scheduling of Manufacturing Systems 3: Clear-a-Fraction Policies Are Stable From Every Initial State When ρ′ₘ < 1Research Paper

Motivation

A flexible manufacturing system processes several part types on shared machines, and a machine that switches from one part type to another pays a set-up time. Real-time, distributed scheduling rules for such systems decide locally, at each machine, when to switch and to which buffer. The simplest such rules are clearing policies: a machine keeps working on its current buffer until that buffer is empty, then switches. Perkins and Kumar (IEEE TAC 34, 1989; reference [18] of Kumar–Seidman 1990) showed that every clear-a-fraction (CAF) policy, a clearing policy that always switches to a buffer holding at least a fixed fraction of the machine's work, keeps all buffers bounded in every acyclic system whenever each machine's load is below one.

Kumar and Seidman (IEEE TAC 1990) showed that acyclicity cannot simply be dropped. In §III of the paper, a two-machine re-entrant line and a two-part-type system, both with every machine loaded below capacity, have clearing trajectories whose buffer levels grow without bound. This mission formalizes the paper's positive result for non-acyclic systems: Theorem 1, a stronger capacity condition under which every CAF policy is stable from every initial state.

Setting

There are PPP part types and MMM machines. Part type ppp enters at rate dp>0d_p>0dp​>0 and visits the machines μp,1,…,μp,np\mu_{p,1},\dots,\mu_{p,n_p}μp,1​,…,μp,np​​ in turn; revisits are allowed. At its iii-th stage a part waits in buffer bp,ib_{p,i}bp,i​ and needs processing time τp,i>0\tau_{p,i}>0τp,i​>0. Machine mmm serves Bm={bp,i:μp,i=m}B_m=\{b_{p,i}:\mu_{p,i}=m\}Bm​={bp,i​:μp,i​=m}, and switching from bbb to b′∈Bmb'\in B_mb′∈Bm​ costs δb,b′≥0\delta_{b,b'}\ge0δb,b′​≥0. Flows are fluid. The level xb(t)≥0x_b(t)\ge0xb​(t)≥0 satisfies xb(t)=xb(0)+ub(t)−yb(t)x_b(t)=x_b(0)+u_b(t)-y_b(t)xb​(t)=xb​(0)+ub​(t)−yb​(t), where yby_byb​ is the cumulative output and ubu_bub​ the cumulative input: dptd_p tdp​t for the first buffer of a route, the output of the previous buffer otherwise. Each machine works through runs. A run is a set-up for a buffer, during which nothing is processed, followed by processing of that buffer at rate at most 1/τb1/\tau_b1/τb​, and at exactly that rate while the buffer is nonempty.

A trajectory is clearing (Definition 1) if each machine leaves its buffer exactly at the first time the buffer is empty while another of its buffers is nonempty, and then sets up for such a buffer. It is CAF with constants εm>0\varepsilon_m>0εm​>0, KmK_mKm​ (Definition 2) if every set-up commenced at time ttt is for a buffer with

xp,i(t) ≥ εm∑(q,j): μq,j=mxq,j(t)−Km.x_{p,i}(t)\ \ge\ \varepsilon_m\sum_{(q,j):\,\mu_{q,j}=m}x_{q,j}(t)-K_m .xp,i​(t) ≥ εm​(q,j):μq,j​=m∑​xq,j​(t)−Km​.

A trajectory is stable if sup⁡t≥0xp,i(t)<∞\sup_{t\ge0}x_{p,i}(t)<\inftysupt≥0​xp,i​(t)<∞ for every buffer.

The graph on machines has an arc m→m′m\to m'm→m′ when m≠m′m\ne m'm=m′ and some part type visits m′m'm′ right after mmm. Machines are diconnected, m↔m′m\leftrightarrow m'm↔m′, when each is reachable from the other. For each buffer, λp,i\lambda_{p,i}λp,i​ is the last earlier stage at a different machine, if any, and πp,i\pi_{p,i}πp,i​ is that stage's machine, the prior machine. The modified input rate is dp,i′=1/τp,λp,id'_{p,i}=1/\tau_{p,\lambda_{p,i}}dp,i′​=1/τp,λp,i​​ if πp,i↔μp,i\pi_{p,i}\leftrightarrow\mu_{p,i}πp,i​↔μp,i​, and dp,i′=dpd'_{p,i}=d_pdp,i′​=dp​ otherwise (11)–(13).

Formalization targets

Goal: Theorem 1 (p. 294)

If

ρm′:=∑(p,i): μp,i=mdp,i′ τp,i<1for all m,(14)\rho'_m:=\sum_{(p,i):\,\mu_{p,i}=m}d'_{p,i}\,\tau_{p,i}<1\qquad\text{for all } m, \tag{14}ρm′​:=(p,i):μp,i​=m∑​dp,i′​τp,i​<1for all m,(14)

then for all ε>0\varepsilon>0ε>0, all KKK, every CAF trajectory from every initial state is stable. The bound on each buffer may depend on the trajectory.

Milestones (the proof's own steps, p. 295)

For a machine mmm in a minimal class, Vm(t)=∑μp,i=mxp,i(t)[τp,i+⋯+τp,i+ηp,i−1]V_m(t)=\sum_{\mu_{p,i}=m}x_{p,i}(t)[\tau_{p,i}+\dots+\tau_{p,i+\eta_{p,i}-1}]Vm​(t)=∑μp,i​=m​xp,i​(t)[τp,i​+⋯+τp,i+ηp,i​−1​] is the work at mmm (15), and Tn,Tn+1T_n, T_{n+1}Tn​,Tn+1​ are consecutive set-up commencements:

  1. (18): Vm(Tn+1)≤max⁡[0,Vm(Tn)−(1−ρm′)(Tn+1−Tn)+δˉ]V_m(T_{n+1})\le\max[0,V_m(T_n)-(1-\rho'_m)(T_{n+1}-T_n)+\bar\delta]Vm​(Tn+1​)≤max[0,Vm​(Tn​)−(1−ρm′​)(Tn+1​−Tn​)+δˉ].
  2. (20): xpn∗,in∗(Tn)≥2δˉ/((1−ρm′)τpn∗,in∗)⇒Tn+1−Tn≥2δˉ/(1−ρm′)x_{p^*_n,i^*_n}(T_n)\ge 2\bar\delta/((1-\rho'_m)\tau_{p^*_n,i^*_n})\Rightarrow T_{n+1}-T_n\ge2\bar\delta/(1-\rho'_m)xpn∗​,in∗​​(Tn​)≥2δˉ/((1−ρm′​)τpn∗​,in∗​​)⇒Tn+1​−Tn​≥2δˉ/(1−ρm′​).
  3. Vm(Tn)≥Γm⇒Vm(Tn+1)≤Vm(Tn)−δˉV_m(T_n)\ge\Gamma_m\Rightarrow V_m(T_{n+1})\le V_m(T_n)-\bar\deltaVm​(Tn​)≥Γm​⇒Vm​(Tn+1​)≤Vm​(Tn​)−δˉ, with the explicit Γm\Gamma_mΓm​ of p. 295.
  4. Every buffer of every machine in a minimal class is bounded.
  5. The induction step: with upstream classes bounded, Vm(Tn+1)≤max⁡{Γˉ,Vm(Tn)−(1−ρm′)(Tn+1−Tn)+δˉ+Γˉ}V_m(T_{n+1})\le\max\{\bar\Gamma,V_m(T_n)-(1-\rho'_m)(T_{n+1}-T_n)+\bar\delta+\bar\Gamma\}Vm​(Tn+1​)≤max{Γˉ,Vm​(Tn​)−(1−ρm′​)(Tn+1​−Tn​)+δˉ+Γˉ}.

Significance

The result. Theorem 1 is a sufficient condition for stability that holds for every system topology and every CAF policy, with no restriction to acyclic flows. It separates two kinds of upstream supply. A machine that is not in a common cycle with its supplier needs capacity only for the average rate dpd_pdp​. A machine that is in such a cycle must budget for the supplier's peak rate. The paper's examples show that some strengthening of ρm<1\rho_m<1ρm​<1 is needed for clearing policies on cyclic systems: they are unstable under ρm<1\rho_m<1ρm​<1 alone. Section V of the paper builds on this gap, with a supervisory mechanism that restores stability under ρm<1\rho_m<1ρm​<1 alone.

Formalizing it. The theorem is proved in the paper; no machine-checked proof exists. A formalization must turn a two-page argument with a set-up/processing run structure, a starvation case analysis and an induction over the condensation of a directed graph into rigorous statements. The result is a reusable fluid model of scheduling with set-up times. It also makes explicit the conventions of the clearing rule, which the paper leaves informal.

Difficulty

A natural first attempt bounds the total work VmV_mVm​ at each machine separately, using only the average arrival rates. This fails on cyclic systems. A machine downstream in a cycle can receive parts in bursts at the upstream machine's full processing rate 1/τ1/\tau1/τ, far above dpd_pdp​; Example 1 of the paper builds exactly such a positive feedback. The proof therefore has to (a) bound the inflow into a machine of a minimal class by the peak rates in (14); (b) handle starvation inside a run, where the machine works below its maximal rate; (c) control the set-up overhead, which the CAF rule amortizes by forcing long runs once VmV_mVm​ is large; and (d) push boundedness down the partial order of classes, where the bounded upstream buffers enter as an additive constant Γˉ\bar\GammaΓˉ. Step (d) needs a bound on the total content upstream, not one per buffer.

Formalization scope

  • Model. System P M holds the data. Part types, machines and stages are 0-based (paper stage iii is Lean stage i−1i-1i−1). Trajectory S holds levels, cumulative outputs and runs, with N m : ℕ∞ runs per machine. Time is real, with explicit t≥0t\ge0t≥0. Run starts are nondecreasing and, if infinitely many, tend to infinity. Machines never idle outside runs: idling on an empty buffer is processing at the inflow rate.
  • Processing law. The output is bounded by 1/τb1/\tau_b1/τb​ times the Lebesgue measure of the time spent processing bbb, with equality on intervals of processing of a nonempty buffer.
  • Clearing. "Nonempty" in Definition 1 for the buffer switched to is read as nonempty or with inflow starting now. Under this reading the paper's example trajectories are clearing trajectories; read literally, "the first time" would not exist. The emptiness test on the current buffer is literal. The no-early-exit condition holds on the open processing interval.
  • Set-ups. Set-ups occur only between distinct buffers. δˉ\bar\deltaδˉ is the largest set-up time between distinct buffers of mmm, or 000 if there are none. Zero set-up times are allowed; δˉ>0\bar\delta>0δˉ>0 is not assumed.
  • Constants. Γm\Gamma_mΓm​, τˉ\bar\tauτˉ, τ‾\underline\tauτ​, Γˉ\bar\GammaΓˉ are explicit definitions, never existentials. Every denominator is positive under the hypotheses.
  • Trivializations ruled out. The trajectory class is not empty: a sorry-free witness (one machine, one buffer, dτ<1d\tau<1dτ<1, any initial level) satisfies every predicate, together with (14). The goal quantifies over every system, every ε>0\varepsilon>0ε>0 and KKK, and every CAF trajectory. It does not fix a selection rule, an acyclic topology, routes without revisits or positive set-ups.
  • Infrastructure. Continuity of the levels (from the rate cap), restarting a trajectory at a run start, inflow bounds via conservation along routes, and the condensation of the machine graph. These are reusable for the related Kumar–Seidman missions on instability and supervisory stabilization. Proofs of the milestones in any order are welcome.

Selected references

  • P. R. Kumar and T. I. Seidman, Dynamic instabilities and stabilization methods in distributed real-time scheduling of manufacturing systems, IEEE Transactions on Automatic Control 35(3), 289–298, 1990. https://doi.org/10.1109/9.50339
  • J. R. Perkins and P. R. Kumar, Stable, distributed, real-time scheduling of flexible manufacturing/assembly/disassembly systems, IEEE Transactions on Automatic Control 34, 139–148, February 1989 (cited as [18] in Kumar–Seidman 1990; the CAF stability result for acyclic systems).
10 thms2 active usersReviewed
Operations ResearchProbabilityRandom Matrix Theory·Captain: mikedeng1

Subadditive Ergodic Theory 5: For a Stationary Sequence in a Banach Algebra with E(log‖Y₁‖)⁺ < ∞, n⁻¹ log‖Y₁⋯Y_n‖ Converges in [−∞, ∞)Research Paper

Motivation

Products of random linear operators appear wherever a system evolves by repeated application of randomly chosen linear maps: linear recursions with random coefficients, products of random matrices in statistical physics, the growth of random dynamical systems, and population models in random environments. The basic question is the exponential growth rate of the product Y1Y2⋯YnY_1Y_2\cdots Y_nY1​Y2​⋯Yn​. For square matrices, Furstenberg and Kesten (Ann. Math. Statist. 31, 1960) proved that n−1log⁡∥Y1⋯Yn∥n^{-1}\log\|Y_1\cdots Y_n\|n−1log∥Y1​⋯Yn​∥ converges for stationary sequences with a logarithmic moment condition.

Kingman (Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973) showed that this limit theorem is an instance of the subadditive ergodic theorem, and that the instance needs nothing of matrices beyond the norm inequality ∥AB∥≤∥A∥ ∥B∥\|AB\|\le\|A\|\,\|B\|∥AB∥≤∥A∥∥B∥. His Theorem 6 therefore holds in an arbitrary real or complex Banach algebra, including infinite-dimensional ones such as infinite matrices with finite ℓ1\ell_1ℓ1​ norm. It is the source of what later became known as the top Lyapunov exponent of a stationary random operator product.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space. A two-parameter family is a collection x=(xst)x=(x_{st})x=(xst​) of random variables indexed by nonnegative integers s<ts<ts<t. Kingman's conditions (§1.1–1.2) are:

  • S₁: xsu≤xst+xtux_{su}\le x_{st}+x_{tu}xsu​≤xst​+xtu​ whenever s<t<us<t<us<t<u;
  • S₂: the joint distributions of (xs+1,t+1)(x_{s+1,t+1})(xs+1,t+1​) are the same as those of (xst)(x_{st})(xst​);
  • S₃: gt=E(x0t)g_t=E(x_{0t})gt​=E(x0t​) is finite for every t≥1t\ge1t≥1 and gt≥−Atg_t\ge -Atgt​≥−At for some constant AAA;
  • S₃′: E(x01+)<∞E(x_{01}^+)<\inftyE(x01+​)<∞, where x+=max⁡(x,0)x^+=\max(x,0)x+=max(x,0).

A family of real random variables satisfying S₁, S₂ and S₃ is a subadditive process. Kingman's Theorem 1 (the goal of the first mission of this series) says that for a subadditive process x0t/tx_{0t}/tx0t​/t converges almost surely and in mean to a finite random variable ξ\xiξ with E(ξ)=γ=inf⁡t≥1gt/tE(\xi)=\gamma=\inf_{t\ge1}g_t/tE(ξ)=γ=inft≥1​gt​/t.

A Banach algebra B\mathfrak BB is a complete normed algebra over R\mathbb RR or C\mathbb CC whose norm satisfies ∥AB∥≤∥A∥ ∥B∥\|AB\|\le\|A\|\,\|B\|∥AB∥≤∥A∥∥B∥. A sequence (Yn)n≥1(Y_n)_{n\ge1}(Yn​)n≥1​ of B\mathfrak BB-valued random elements is stationary if (Yn+1)n≥1(Y_{n+1})_{n\ge1}(Yn+1​)n≥1​ and (Yn)n≥1(Y_n)_{n\ge1}(Yn​)n≥1​ have the same joint law. The log-norm process is

xst=log⁡∥Ys+1Ys+2⋯Yt∥∈[−∞,∞),s<t,x_{st}=\log\|Y_{s+1}Y_{s+2}\cdots Y_t\|\in[-\infty,\infty),\qquad s<t,xst​=log∥Ys+1​Ys+2​⋯Yt​∥∈[−∞,∞),s<t,

with log⁡0=−∞\log 0=-\inftylog0=−∞. Expectations of [−∞,∞)[-\infty,\infty)[−∞,∞)-valued variables are extended expectations E(f)=∫f+ dP−∫f− dPE(f)=\int f^+\,dP-\int f^-\,dPE(f)=∫f+dP−∫f−dP, defined when ∫f+ dP<∞\int f^+\,dP<\infty∫f+dP<∞ and possibly equal to −∞-\infty−∞.

Formalization targets

Goal: Theorem 6 (p. 893)

If (Yn)(Y_n)(Yn​) is a stationary sequence in a real or complex Banach algebra and E{(log⁡∥Y1∥)+}<∞E\{(\log\|Y_1\|)^+\}<\inftyE{(log∥Y1​∥)+}<∞, then

ξ=lim⁡n→∞n−1log⁡∥Y1Y2⋯Yn∥\xi=\lim_{n\to\infty}n^{-1}\log\|Y_1Y_2\cdots Y_n\|ξ=n→∞lim​n−1log∥Y1​Y2​⋯Yn​∥

exists in −∞≤ξ<∞-\infty\le\xi<\infty−∞≤ξ<∞ with probability one, and

E(ξ)=lim⁡n→∞n−1E{log⁡∥Y1Y2⋯Yn∥}.E(\xi)=\lim_{n\to\infty}n^{-1}E\{\log\|Y_1Y_2\cdots Y_n\|\}.E(ξ)=n→∞lim​n−1E{log∥Y1​Y2​⋯Yn​∥}.

The goal fixes no constant and no ergodicity assumption: ξ\xiξ is in general a non-degenerate random variable.

Milestones

  1. (1.2.7), p. 885: under S₁, S₂ and S₃′, E(xst+)<∞E(x_{st}^+)<\inftyE(xst+​)<∞ for all s<ts<ts<t.
  2. Proof of Theorem 2, p. 886: the truncation xst(N)=max⁡(xst,−N(t−s))x^{(N)}_{st}=\max(x_{st},-N(t-s))xst(N)​=max(xst​,−N(t−s)) is a subadditive process for every positive integer NNN.
  3. Theorem 2, p. 885: if xxx satisfies S₁, S₂ and S₃′ but not S₃, then ξ=lim⁡x0t/t\xi=\lim x_{0t}/tξ=limx0t​/t exists with probability one in [−∞,∞)[-\infty,\infty)[−∞,∞) and E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞.
  4. Proof of Theorem 6, p. 893: the log-norm process satisfies S₁, S₂ and S₃′.

Significance

Theorem 6 defines a stochastic spectral radius: if every YnY_nYn​ equals a fixed element yyy, then eξe^\xieξ is the spectral radius of yyy by Gelfand's formula, and for independent YnY_nYn​ with common law π\piπ the limit is a constant ρ(π)\rho(\pi)ρ(π) depending only on π\piπ. For k×kk\times kk×k matrices the theorem reduces to the Furstenberg–Kesten theorem. Theorem 2, the extension of the subadditive ergodic theorem from S₃ to S₃′, is the form needed whenever a process can have mean growth rate −∞-\infty−∞, as happens for products that can vanish or contract superlinearly; it is used well beyond random products.

All results here are proved on paper (Kingman 1973, building on his 1968 paper). None of them is machine-checked: Mathlib has no subadditive ergodic theorem, no Furstenberg–Kesten theorem and no random-product limit in normed algebras. The platform poses an ergodic, constant-limit form of Kingman's theorem (PalmQueueing.Ergodic.kingman_subadditive, open); this mission's Theorem 2 is a different statement (non-ergodic, conclusion E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞ under failure of S₃). A complete development would give the first formal proof of the Furstenberg–Kesten limit, in the generality of Banach algebras.

Difficulty

Theorem 6 is short given Theorems 1 and 2, but the obvious one-line reduction to Theorem 1 fails in two places. First, the log-norm process can take the value −∞-\infty−∞ and its means gtg_tgt​ can be −∞-\infty−∞ or decrease superlinearly, so condition S₃ fails and Theorem 1 does not apply; the case E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞ is a separate theorem (Theorem 2), whose proof must exchange a limit in ttt with a limit in an auxiliary parameter. Second, stationarity of the log-norm process (S₂) is a statement about joint laws on a path space; in a non-separable Banach algebra, multiplication need not be measurable for the product σ\sigmaσ-algebra on B×B\mathfrak B\times\mathfrak BB×B, so it is not automatic that the law of (Yn)(Y_n)(Yn​) determines the joint law of the products Ys+1⋯YtY_{s+1}\cdots Y_tYs+1​⋯Yt​. The main dependency, Theorem 1 itself, is the subject of a separate mission and is not restated here.

Formalization scope

The Lean development fixes these conventions:

  • Families are functions x : ℕ → ℕ → Ω → β; only pairs s<ts<ts<t enter any condition. S₁ is required almost surely for each triple (the weaker hypothesis); the log-norm milestone proves it at every sample point.
  • S₂ and stationarity are equalities of laws of the whole path (Measure.map) on the product σ\sigmaσ-algebra, not equality of one-dimensional marginals.
  • S₃′ and all positive parts are lower Lebesgue integrals; expectations that may be −∞-\infty−∞ are computed as ∫f+−∫f−\int f^+ - \int f^-∫f+−∫f− in EReal, never as Bochner integrals (which return 000 for non-integrable functions).
  • log⁡∥⋅∥\log\|\cdot\|log∥⋅∥ is ENNReal.log of the norm, so log⁡∥0∥=−∞\log\|0\|=-\inftylog∥0∥=−∞; Real.log 0 = 0 would replace a vanishing product's growth rate −∞-\infty−∞ by 000, and is ruled out.
  • B\mathfrak BB is a complete unital NormedRing with NormedAlgebra 𝕜 𝔅, RCLike 𝕜. Each YnY_nYn​ is strongly measurable; B\mathfrak BB is not assumed separable.
  • Limits are Filter.atTop on ℕ in the topology of EReal; the conclusions assert ξ<∞\xi<\inftyξ<∞ almost surely, E(ξ+)<∞E(\xi^+)<\inftyE(ξ+)<∞, and, for (2.3.5), both the existence of the limit of means and its value.

A formalization that replaces the extended logarithm by Real.log, or the extended expectation by a Bochner integral, makes the statement false or trivially different, and is excluded.

Reusable infrastructure: extended expectations of EReal-valued random variables, joint-law stationarity of sequences and two-parameter families, and the truncation lemma for S₃′ processes. Contributions toward Theorem 1 (mission 1 of this series), toward measurability of products of strongly measurable random elements, and toward the milestones in any order are welcome.

Selected references

  • J. F. C. Kingman, Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973. https://doi.org/10.1214/aop/1176996798
  • J. F. C. Kingman, The ergodic theory of subadditive stochastic processes, J. Roy. Statist. Soc. Ser. B 30:499–510, 1968. https://doi.org/10.1111/j.2517-6161.1968.tb00749.x
  • H. Furstenberg and H. Kesten, Products of random matrices, Ann. Math. Statist. 31:457–469, 1960. https://doi.org/10.1214/aoms/1177705909
8 thms2 active usersReviewed
Operations ResearchProbabilityRandom Matrix Theory·Captain: mikedeng1

Subadditive Ergodic Theory 4: Furstenberg–Kesten — for Stationary Positive Random Matrices, n⁻¹ log [Y₁⋯Y_n]_ij Converges, Independently of i and jResearch Paper

Products of random matrices

Many systems evolve by repeated multiplication by a random linear map: the state of a linear system with randomly varying coefficients, population vectors in a random environment (Leslie models whose rates change from year to year), the transfer matrices of a disordered one-dimensional medium, and the transition operators of a Markov chain in a random environment. In each case the object of interest is the product Xn=Y1Y2⋯YnX_n = Y_1 Y_2 \cdots Y_nXn​=Y1​Y2​⋯Yn​ of random matrices and its growth as n→∞n\to\inftyn→∞.

The basic answer is due to Furstenberg and Kesten (Products of random matrices, Ann. Math. Statist. 31 (1960)): under a logarithmic moment condition and stationarity, n−1log⁡n^{-1}\logn−1log of the size of XnX_nXn​ converges. Their proof was a substantial piece of analysis. In his 1973 IMS Special Invited Paper (Kingman, Subadditive ergodic theory, Ann. Probab. 1 (1973)), J. F. C. Kingman showed that for matrices with strictly positive entries the result is a short corollary of his subadditive ergodic theorem (Theorem 1 of that paper, 1968). This mission formalizes that application: Theorem 5 of the 1973 paper, §2.2, pp. 891–892.

Timeline:

  • 1960: Furstenberg and Kesten prove convergence of n−1log⁡∥Xn∥n^{-1}\log\|X_n\|n−1log∥Xn​∥ and, for positive matrices, of n−1log⁡[Xn]ijn^{-1}\log[X_n]_{ij}n−1log[Xn​]ij​.
  • 1968: Kingman proves the subadditive ergodic theorem (J. Roy. Statist. Soc. B 30).
  • 1973: Kingman's survey deduces the positive-matrix theorem (Theorem 5) and the general Banach-algebra version (Theorem 6) from it.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space, k≥1k\ge1k≥1, and let Y1,Y2,…Y_1, Y_2,\dotsY1​,Y2​,… be random k×kk\times kk×k real matrices. Write [A]ij[A]_{ij}[A]ij​ for the (i,j)(i,j)(i,j)th entry of a matrix AAA, and

Xn=Y1Y2⋯Yn(2.2.1),X_n = Y_1 Y_2\cdots Y_n \qquad (2.2.1),Xn​=Y1​Y2​⋯Yn​(2.2.1),

the product taken left to right. The sequence (Yn)(Y_n)(Yn​) is stationary if the joint law of (Y2,Y3,… )(Y_2, Y_3, \dots)(Y2​,Y3​,…) equals the joint law of (Y1,Y2,… )(Y_1, Y_2, \dots)(Y1​,Y2​,…); this is a statement about all finite-dimensional distributions at once, and it includes the case of independent identically distributed matrices.

The proof works with the diagonal process

zst=[Ys+1Ys+2⋯Yt]11,xst=−log⁡zst(s<t),z_{st} = [Y_{s+1}Y_{s+2}\cdots Y_t]_{11},\qquad x_{st} = -\log z_{st}\qquad (s<t),zst​=[Ys+1​Ys+2​⋯Yt​]11​,xst​=−logzst​(s<t),

and with the ℓ1\ell_1ℓ1​-norm ∥A∥=max⁡i∑j∣[A]ij∣\|A\| = \max_i \sum_j |[A]_{ij}|∥A∥=maxi​∑j​∣[A]ij​∣. A family (xst)s<t(x_{st})_{s<t}(xst​)s<t​ is a subadditive process (§1.1) if S₁: xsu≤xst+xtux_{su}\le x_{st}+x_{tu}xsu​≤xst​+xtu​ for s<t<us<t<us<t<u; S₂: the joint distributions of (xs+1,t+1)(x_{s+1,t+1})(xs+1,t+1​) equal those of (xst)(x_{st})(xst​); S₃: gt=E(x0t)g_t=E(x_{0t})gt​=E(x0t​) exists and gt≥−Atg_t\ge -Atgt​≥−At for some constant AAA.

Formalization targets

Goal: Theorem 5

Suppose the elements of the matrices YnY_nYn​ are strictly positive, E∣log⁡[Yn]ij∣<∞E|\log[Y_n]_{ij}|<\inftyE∣log[Yn​]ij​∣<∞ for every nnn and every i,ji,ji,j, and (Yn)(Y_n)(Yn​) is stationary. Then there is one finite random variable λ\lambdaλ such that for every (i,j)(i,j)(i,j)

λ=lim⁡n→∞n−1log⁡[Xn]ij(2.2.2)\lambda = \lim_{n\to\infty} n^{-1}\log [X_n]_{ij} \qquad (2.2.2)λ=n→∞lim​n−1log[Xn​]ij​(2.2.2)

with probability one and in mean. The limit is random in general (it is constant when (Yn)(Y_n)(Yn​) is ergodic); the theorem asserts its existence, its finiteness and its independence of (i,j)(i,j)(i,j), and nothing about its value.

Milestones, in the order of the paper's proof

  1. (2.3.1): [AB]11≥[A]11[B]11[AB]_{11}\ge[A]_{11}[B]_{11}[AB]11​≥[A]11​[B]11​ for matrices with strictly positive entries.
  2. xst=−log⁡zstx_{st}=-\log z_{st}xst​=−logzst​ satisfies S₁ and S₂, and each xstx_{st}xst​ has finite expectation gt−sg_{t-s}gt−s​.
  3. E{log⁡∥Y1∥}<∞E\{\log\|Y_1\|\}<\inftyE{log∥Y1​∥}<∞ and gn/n≥−E{log⁡∥Y1∥}g_n/n\ge -E\{\log\|Y_1\|\}gn​/n≥−E{log∥Y1​∥} for all n≥1n\ge1n≥1, so S₃ holds.
  4. The limit (2.2.2) exists, with probability one and in mean, for i=j=1i=j=1i=j=1.
  5. (2.2.3): for every (i,j)(i,j)(i,j), P{lim inf⁡n−1log⁡[Xn]ij≥λ}=1P\{\liminf n^{-1}\log[X_n]_{ij}\ge\lambda\}=1P{liminfn−1log[Xn​]ij​≥λ}=1.
  6. For every (i,j)(i,j)(i,j), P{lim sup⁡n−1log⁡[Xn]ij≤λ}=1P\{\limsup n^{-1}\log[X_n]_{ij}\le\lambda\}=1P{limsupn−1log[Xn​]ij​≤λ}=1.

Significance

The limit λ\lambdaλ is the top Lyapunov exponent of the random product: it is the almost-sure exponential growth rate of every entry, and hence of every norm, of XnX_nXn​. It governs the stability of random linear recursions vn=vn−1Ynv_{n}=v_{n-1}Y_nvn​=vn−1​Yn​, the long-run growth rate of populations in random environments, and localization in one-dimensional disordered systems. Theorem 5 is the existence statement on which all of these quantitative questions rest.

The theorem has been proved since 1960, and Kingman's derivation is a classical model application of subadditive ergodic theory. To our knowledge it has no machine-checked proof: Mathlib has neither Kingman's subadditive ergodic theorem nor any limit theorem for random matrix products. This mission produces a formal statement of the result together with the formal decomposition of the proof into the steps Kingman writes down; its milestone 4 is exactly where the subadditive ergodic theorem (the goal of the companion mission Subadditive Ergodic Theory 1) is applied.

Difficulty

Milestones 1–3 are deterministic matrix inequalities plus integrability bookkeeping; the substance is elsewhere. First, milestone 4 needs the full subadditive ergodic theorem, almost-sure and in mean, for a non-ergodic stationary process: the classical Birkhoff theorem does not apply, because log⁡[Xn]11\log[X_n]_{11}log[Xn​]11​ is not a sum of stationary increments. Second, passing from the diagonal entry to all entries requires controlling n−1log⁡[Yn]1jn^{-1}\log[Y_n]_{1j}n−1log[Yn​]1j​ along a stationary sequence with only a first-moment hypothesis, and transporting an almost-sure statement about Xn′=Y2⋯Yn+1X_n'=Y_2\cdots Y_{n+1}Xn′​=Y2​⋯Yn+1​ back to XnX_nXn​ by stationarity, where the limit λ\lambdaλ is itself random. The natural shortcut — treating λ\lambdaλ as a constant — is only valid under ergodicity, which is not assumed.

Formalization scope

  • Matrices are Matrix (Fin k) (Fin k) ℝ with NeZero k; the paper's index 111 is 0 : Fin k. The sequence is Y : ℕ → Ω → Matrix …, read only for n≥1n\ge1n≥1; Y 0 plays no role.
  • Products are ordered: Ys+1⋯YtY_{s+1}\cdots Y_tYs+1​⋯Yt​ is the List.prod of [Y (s+1), …, Y t]; X0X_0X0​ is the identity.
  • Stationarity is equality of the laws of (Yn+2)n≥0(Y_{n+2})_{n\ge0}(Yn+2​)n≥0​ and (Yn+1)n≥0(Y_{n+1})_{n\ge0}(Yn+1​)n≥0​ on ℕ → Fin k → Fin k → ℝ with the product σ-algebra. Independence is not assumed.
  • Positivity holds for every outcome; "their logarithms have finite expectations" is integrability of every log⁡[Yn]ij\log[Y_n]_{ij}log[Yn​]ij​, n≥1n\ge1n≥1.
  • "Finite limit" is a real-valued lam : Ω → ℝ; "in mean" is E∣n−1log⁡[Xn]ij−λ∣→0E|n^{-1}\log[X_n]_{ij}-\lambda|\to0E∣n−1log[Xn​]ij​−λ∣→0 with λ\lambdaλ integrable; time is n∈Nn\in\mathbb Nn∈N with Filter.atTop. One lam serves all (i,j)(i,j)(i,j).
  • Lim inf and lim sup inequalities are stated with ε\varepsilonε: almost surely, for every ε>0\varepsilon>0ε>0, eventually n−1log⁡[Xn]ij≥λ−εn^{-1}\log[X_n]_{ij}\ge\lambda-\varepsilonn−1log[Xn​]ij​≥λ−ε (respectively ≤λ+ε\le\lambda+\varepsilon≤λ+ε), which avoids the junk value of a real liminf on unbounded sequences.
  • Real.log 0 = 0 in Lean; the statements apply log only to entries that are strictly positive under the hypotheses, so no junk value enters. Dropping the positivity hypothesis would change the theorem, and is not an acceptable shortcut.
  • The S₁/S₂ vocabulary of §1.1 comes from the group's shared process module; this mission defines gtg_tgt​ locally. The general subadditive ergodic theorem is not restated here, and milestone 4 is the object-specific statement the paper writes.

Welcome contributions: proofs of the matrix inequalities, the integrability and stationarity transfer lemmas, a formal subadditive ergodic theorem (shared with the companion mission).

Selected references

  • J. F. C. Kingman, Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973. https://doi.org/10.1214/aop/1176996798
  • H. Furstenberg and H. Kesten, Products of random matrices, Ann. Math. Statist. 31(2):457–469, 1960. https://doi.org/10.1214/aoms/1177705909
  • J. F. C. Kingman, The ergodic theory of subadditive stochastic processes, J. Roy. Statist. Soc. Ser. B 30(3):499–510, 1968. https://doi.org/10.1111/j.2517-6161.1968.tb00749.x
9 thms2 active usersReviewed
Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Subadditive Ergodic Theory 3: A Separable Continuous-Parameter Subadditive Process with E(Ω_I) < ∞ Has x₀ₜ/t → ξ with Probability One and in Mean, E(ξ) = γResearch Paper

Motivation

Many random growth models attach a cost, distance, or accumulated quantity to each time interval. If the quantity over a long interval is at most the sum over two adjacent intervals, it is subadditive. A stable rate over long intervals is useful even when the underlying random system does not have a simple independent-increment description. Kingman's 1973 account places percolation and products of random matrices among the applications of this framework. Its basic theorem treats integer time; the present mission concerns the change to every nonnegative real time. Kingman, §1.1 and §1.4.

The change matters because observing a process at integer times can miss arbitrarily large behavior between observations. Kingman gives a smooth stationary-increment example in Theorem 3 where no prescribed increasing bound eventually controls the values at all real times. Theorem 4 gives a condition that does control this local behavior. These two results together explain why the continuous-time statement needs more than a formal change of index type. Kingman, Theorems 3–4.

Setting

Work on a probability space (S,F,P)(S,\mathcal F,P)(S,F,P). A continuous-parameter subadditive process is a family of real random variables xstx_{st}xst​ indexed by 0≤s<t0\le s<t0≤s<t. It satisfies xsu≤xst+xtux_{su}\le x_{st}+x_{tu}xsu​≤xst​+xtu​ whenever 0≤s<t<u0\le s<t<u0≤s<t<u. Its stationarity says that, for every real shift τ≥0\tau\ge0τ≥0, the complete shifted family (xs+τ,t+τ)s<t(x_{s+\tau,t+\tau})_{s<t}(xs+τ,t+τ​)s<t​ has the same joint distribution as (xst)s<t(x_{st})_{s<t}(xst​)s<t​. Finally, the mean gt=E(x0t)g_t=E(x_{0t})gt​=E(x0t​) exists as a finite real number for each t>0t>0t>0 and obeys gt≥−Atg_t\ge-Atgt​≥−At for one constant AAA. These are the continuous-time versions of Kingman's conditions S₁, S₂, and S₃. Equality of the law of each individual coordinate would be too weak for S₂. Kingman, pp. 883–884, 887.

For an interval I⊆[0,∞)I\subseteq[0,\infty)I⊆[0,∞), the oscillation is ΩI=sup⁡s<t, s,t∈I∣xst∣\Omega_I=\sup_{s<t,\,s,t\in I}|x_{st}|ΩI​=sups<t,s,t∈I​∣xst​∣. A process has the local oscillation condition when E(ΩI)<∞E(\Omega_I)<\inftyE(ΩI​)<∞ for one nondegenerate interval III. In §1.4 the paper states that this condition then holds on every bounded interval. The quantity γ=inf⁡t>0gt/t\gamma=\inf_{t>0}g_t/tγ=inft>0​gt​/t is the mean growth rate. Kingman, (1.4.1), (1.4.6)–(1.4.7).

The paper also requires separability. Here this means that, outside one probability-zero set, the value at every admissible pair of times can be approached along a sequence from a fixed countable dense set of pairs. It is a condition on how the uncountable family is observed, and it permits discontinuous sample paths. Kingman cites the standard separability convention without defining it in §1.4; the mission makes the convention explicit. Kingman, Theorem 4 and following discussion.

Formalization targets

Theorem 4: convergence at all real times

For a separable process satisfying S₁–S₃ and the local oscillation condition, the target is an integrable real random variable ξ\xiξ such that

x0tt⟶ξalmost surely and in L1(P)(t→∞, t∈R),E(ξ)=γ=inf⁡u>0guu.\frac{x_{0t}}{t}\longrightarrow\xi\quad\text{almost surely and in }L^1(P) \quad(t\to\infty,\ t\in\mathbb R), \qquad E(\xi)=\gamma=\inf_{u>0}\frac{g_u}{u}.tx0t​​⟶ξalmost surely and in L1(P)(t→∞, t∈R),E(ξ)=γ=u>0inf​ugu​​.

The time variable ranges over all real values tending to infinity. The integer-time assertion (1.4.8) is a separate milestone, not the goal. Other milestones identify the deterministic mean rate, extend the oscillation condition to bounded intervals, record the bounds at times between consecutive integers, and state the vanishing of normalized unit-interval oscillation. Each comes from a sentence or display in §1.4. Kingman, Theorem 4 and proof.

Significance

Theorem 4 gives a long-run rate for a broad stationary subadditive family without assuming that its trajectories are continuous or differentiable. Its mean statement identifies the expectation of the random limit with a deterministic infimum of normalized expectations. The paper notes that the usual continuous-time ergodic theorem for additive integral processes is a corollary, because such processes satisfy its oscillation condition. The condition is therefore compatible with familiar additive models while also covering discontinuous subadditive ones. Kingman, p. 890.

The theorem and its argument are known from the paper; this mission asks for a machine-checked development of the stated result. A completed development would provide reusable formal interfaces for joint-law stationarity of an uncountable family, separability, extended-valued oscillations, and almost-sure plus L1L^1L1 limits. The proposed theorem statements compile as open goals; compiling them does not prove them. Kingman, §1.4.

Difficulty

An integer-time subadditive theorem controls x0n/nx_{0n}/nx0n​/n only on its discrete skeleton. It cannot by itself rule out large values of x0t/tx_{0t}/tx0t​/t for times between consecutive integers; Theorem 3 shows that such behavior can occur even with smooth stationary sample paths and finite expectations. A continuous-time result must control local variation as the observation window moves to large times. The uncountable supremum in ΩI\Omega_IΩI​ also needs a genuine extended value and a measurability convention. Kingman, Theorems 3–4.

The paper's displayed assertion (1.4.1), that gt/tg_t/tgt​/t converges as real t→∞t\to\inftyt→∞ under S₁–S₃ alone, needs qualification: a discontinuous additive function can make a deterministic subadditive mean with no such limit. The corresponding milestone includes the finite-oscillation condition assumed by Theorem 4. This correction is disclosed in the theorem's formalization note. Kingman, (1.4.1), (1.4.7).

Formalization scope

Lean indexes the family by R→R→S→R\mathbb R\to\mathbb R\to S\to\mathbb RR→R→S→R and uses only 0≤s<t0\le s<t0≤s<t; values at other pairs carry no meaning. Each valid coordinate is measurable. S₁ is pointwise in the sample point, while S₂ is equality of the probability laws of the complete path before and after every nonnegative real shift. S₃ states integrability of x0tx_{0t}x0t​ for every t>0t>0t>0 and one linear lower bound on its mean. The sample-space type is called SSS so that ΩI\Omega_IΩI​ denotes oscillation without ambiguity.

Oscillation is valued in the extended nonnegative reals. Thus an unbounded supremum is infinite, and the expected-oscillation condition cannot hold because of a default real-supremum value. Separability is the countable graph-approximation condition outside one measurable null set. The premise is finiteness on one closed interval [a,b][a,b][a,b] with 0≤a<b0\le a<b0≤a<b; the propagation milestone covers bounded intervals with either choice of endpoints. The limit in Theorem 4 uses the filter at infinity on real time. Its almost-sure convergence and convergence in mean are separate clauses, and ξ\xiξ is integrable. No continuity of paths, ergodicity, or independence is assumed.

A complete proof may build on Mathlib's measure theory, filters, Borel–Cantelli lemmas, and real analysis. The process and oscillation definitions, along with the finite-oscillation and skeleton statements, are reusable beyond this particular theorem. Contributions that establish these interfaces and the named intermediate statements are within scope. A statement limited to integer times, a marginal-only version of stationarity, or a real supremum that returns a default value on an unbounded set would not express this target.

Selected references

  • J. F. C. Kingman, Subadditive ergodic theory, The Annals of Probability 1(6):883–899, 1973. DOI: 10.1214/aop/1176996798.
7 thms2 active usersReviewed
Operations ResearchStochastic Systems·Captain: mikedeng1

Stability and Instability of Fluid Models for Reentrant Lines 3: In Every Reentrant Line the Last-Buffer-First-Served Fluid Model Is StableResearch Paper

Motivation

A manufacturing line can send the same job through several stations and return it to a station it visited earlier. Semiconductor fabrication is one example. Such a reentrant line has several customer classes at one server, and the server must choose which class to work on. A station may have enough capacity on average yet the line can still accumulate an unbounded queue under an unfortunate service rule. Dai and Weiss use deterministic fluid models to study this question: fluid represents large queues, and its motion exposes the long-run effect of the service rule. Their paper proves that two simple buffer priority disciplines have stable fluid models for every reentrant line satisfying the usual station load condition. This mission concerns Last-Buffer-First-Served, abbreviated LBFS. Dai and Weiss (1996).

The distinction between fluid and stochastic queue stability matters. Dai and Weiss cite an earlier theorem connecting stable fluid models to stable queueing disciplines under the stochastic assumptions of their introduction. The target here is their fluid theorem, Theorem 4.4, rather than a separate formalization of that stochastic implication. Dai and Weiss (1996), pp. 115, 119, 124.

Setting

There are KKK classes, numbered in route order, and III stations. Every unit of fluid enters class 111 at rate one. On completing service in class kkk, it becomes class k+1k+1k+1; after class KKK, it leaves. The station serving class kkk is σ(k)\sigma(k)σ(k). Different classes may share a station. The constituency of station iii is Ci={k:σ(k)=i}C_i=\{k:\sigma(k)=i\}Ci​={k:σ(k)=i}, and class kkk has positive mean service requirement mkm_kmk​, so its service rate is μk=1/mk\mu_k=1/m_kμk​=1/mk​. The nominal workload at station iii is ρi=∑k∈Cimk\rho_i=\sum_{k\in C_i}m_kρi​=∑k∈Ci​​mk​. The paper assumes ρi<1\rho_i<1ρi​<1 at every station. Dai and Weiss (1996), pp. 115–117.

For time t≥0t\ge0t≥0, Qk(t)Q_k(t)Qk​(t) is the amount of fluid in class kkk, and Tk(t)T_k(t)Tk​(t) is the cumulative server time spent on that class. The flow equations say that class content equals its initial content plus completed service from the preceding class minus its own completed service. The first class receives the external unit-rate flow. Each QkQ_kQk​ remains nonnegative, each TkT_kTk​ starts at zero and is nondecreasing, and the cumulative idle time of every station is nondecreasing. A priority rule adds a condition on when a server may reserve capacity for lower-ranked classes. These are the fluid equations of Definition 1.2 and §4. Dai and Weiss (1996), pp. 118, 122–123.

A priority ranking π\piπ assigns a distinct rank to every class, with smaller rank meaning higher priority. For class kkk, let HkH_kHk​ contain the classes at the same station whose rank is at least as high as kkk's. In a preemptive-resume priority fluid model, capacity unused by HkH_kHk​ may increase only when the fluid workload in HkH_kHk​ is zero. Under LBFS, π(k)=K+1−k\pi(k)=K+1-kπ(k)=K+1−k: a class later in the route has higher priority. Priority is compared within each station, even though the ranking is written globally. Dai and Weiss (1996), pp. 122–123, Definition 4.1.

Formalization targets

Theorem 4.4 asks for stability of the LBFS fluid model for every reentrant line with positive service requirements and ρi<1\rho_i<1ρi​<1:

∃δ>0  ∀(Q,T),[(Q,T) is an LBFS fluid solution and ∣Q(0)∣=1]⟹∀t≥δ,  Q(t)=0,\exists\delta>0\;\forall (Q,T),\quad \bigl[(Q,T)\text{ is an LBFS fluid solution and }|Q(0)|=1\bigr] \Longrightarrow \forall t\ge\delta,\;Q(t)=0,∃δ>0∀(Q,T),[(Q,T) is an LBFS fluid solution and ∣Q(0)∣=1]⟹∀t≥δ,Q(t)=0,

where ∣Q(0)∣=∑k=1KQk(0)|Q(0)|=\sum_{k=1}^K Q_k(0)∣Q(0)∣=∑k=1K​Qk​(0). The same δ\deltaδ must work for every solution and every normalized initial configuration. This is exactly the fluid stability definition used by the paper. Dai and Weiss (1996), pp. 118–119, 124.

The milestones follow the paper's own intermediate statements. Lemma 2.2 treats a nonnegative absolutely continuous function whose derivative is negative whenever the function is positive. Proposition 4.2 identifies flow-rate relations at a regular point under a buffer priority rule. The proof of Theorem 4.4 records a uniform negative drift for total content and the explicit emptying time

δ=∣Q(0)∣λ^−1,λ^=1max⁡1≤i≤Iρi>1.\delta=\frac{|Q(0)|}{\widehat\lambda-1},\qquad \widehat\lambda=\frac{1}{\max_{1\le i\le I}\rho_i}>1.δ=λ−1∣Q(0)∣​,λ=max1≤i≤I​ρi​1​>1.

The explicit time is stated for every initial fluid amount; normalization to one belongs only to the final stability theorem. Dai and Weiss (1996), pp. 120, 123–125.

Significance

The theorem gives a uniform finite clearing time for the LBFS fluid model whenever each station's nominal workload is below its capacity. It applies to any number of stations, any finite route, and any assignment of route stages to stations. This is stronger than checking a particular factory layout. The conclusion concerns every fluid solution, which matters because the defining equations need not determine a unique path. Dai and Weiss (1996), pp. 118–119, 124–125.

Formalizing the result requires a reusable interface for reentrant lines, service allocation, station workloads, and the priority complementarity condition, plus separate statements for the extinction criterion and priority flow rates. The theorem is proved in the 1996 paper; the remaining work in this mission is a machine-checked Lean proof of its fluid-model statement and of the listed milestones. The stochastic queueing theorem cited by Dai and Weiss is outside this mission's scope.

Difficulty

The load inequalities ρi<1\rho_i<1ρi​<1 compare average work with available server time, but by themselves they do not specify which class receives service at an instant. Under other service rules, reentrant lines can amplify queued fluid despite every station being nominally underloaded; the same paper gives such an example. A formal proof therefore has to use the precise LBFS priority condition, not only the flow equations and the load inequalities. The regular-time argument must then yield a single bound valid across every possible fluid path. Dai and Weiss (1996), §§4–5.

Formalization scope

Lean represents classes and stations by finite index types. Their indices start at zero: Lean class k−1k-1k−1 corresponds to paper class kkk, and LBFS is Fin.revPerm. The paths QQQ and TTT are functions on all real times, while the fluid equations and conclusions are imposed only for t≥0t\ge0t≥0. The external arrival rate is one, as in the paper's normalization. The conditions that station idle capacity and priority-set unused capacity increase only when their relevant content is zero are expressed by constancy on each interval where that content stays positive. Service and fluid paths are not given extra continuity hypotheses; the fluid equations and monotonicity conditions provide the regularity used in the paper. Dai and Weiss (1996), pp. 116–119, 122–123.

The service requirements mk>0m_k>0mk​>0 are explicit so μk=1/mk\mu_k=1/m_kμk​=1/mk​ has its intended value. The drift and emptying-time milestones explicitly assume K>0K>0K>0, since their formula divides by the maximum station workload. The main theorem retains the universal quantification over lines; when K=0K=0K=0, its normalization ∣Q(0)∣=1|Q(0)|=1∣Q(0)∣=1 is impossible. A faithful solution predicate must include the priority condition (4.4), whose omission would change Theorem 4.4 into a false claim about all work-conserving policies. The definition layer, elementary real-analysis extinction lemma, and priority flow-rate relations are useful beyond this single stability theorem. Dai and Weiss (1996), pp. 117–125.

Selected references

  • J. G. Dai and G. Weiss, Stability and instability of fluid models for reentrant lines, Mathematics of Operations Research 21(1), 115–134, 1996. DOI: 10.1287/moor.21.1.115.
8 thms2 active usersReviewed
Operations ResearchStochastic Systems·Captain: mikedeng1

Stability and Instability of Fluid Models for Reentrant Lines 2: In Every Reentrant Line the First-Buffer-First-Served Fluid Model Is StableResearch Paper

Why priority rules in reentrant lines matter

Semiconductor wafer fabrication is the standard example of a reentrant line: every wafer follows the same long route through a set of machines, and visits several machines many times. Each visit is a separate processing step, and a machine with work waiting from several steps must choose which step to serve. Kumar (1993) proposed studying such lines through their buffer priority rules, and Lu and Kumar (1991) showed that a priority rule can make a line unstable even though every machine has spare capacity. The question is therefore not academic: a scheduling rule that looks reasonable can let queues grow without bound.

Dai (1995) reduced the positive Harris recurrence of a multiclass queueing network to the stability of a deterministic fluid model, and Dai and Weiss (1996) used this reduction to prove stability results for several reentrant lines. This mission formalizes their Theorem 4.3: under the First-Buffer-First-Served (FBFS) discipline, the fluid model of every reentrant line is stable whenever each station's nominal workload is below one. Kumar (1993) had proved the analogous statement for discrete deterministic systems.

Timeline:

  • 1991. Lu and Kumar exhibit a two-station reentrant line that is unstable under a static priority rule with every workload below one.
  • 1993. Kumar proves stability of FBFS and LBFS for discrete deterministic reentrant lines.
  • 1995. Dai shows that stability of the fluid model implies positive Harris recurrence of the stochastic network.
  • 1996. Dai and Weiss prove that the FBFS and LBFS fluid models of every reentrant line are stable (Theorems 4.3 and 4.4), and with Dai's theorem obtain stability of the stochastic networks.

Setting

A reentrant line has III stations and KKK classes. All fluid follows one route: it enters as class 111, becomes class k+1k+1k+1 when class kkk is completed, and leaves after class KKK. Class kkk is served at station σ(k)\sigma(k)σ(k) with mean service time mk>0m_k > 0mk​>0, and μk=1/mk\mu_k = 1/m_kμk​=1/mk​. The constituency of station iii is Ci={k:σ(k)=i}C_i = \{k : \sigma(k) = i\}Ci​={k:σ(k)=i}, and its nominal workload is ρi=∑k∈Cimk\rho_i = \sum_{k\in C_i} m_kρi​=∑k∈Ci​​mk​. The exogenous arrival rate is 111. The standing assumption of the paper is

ρi<1(i=1,…,I).(1.7)\rho_i < 1 \qquad (i = 1,\dots,I). \tag{1.7}ρi​<1(i=1,…,I).(1.7)

A fluid model solution is a pair of paths Q(t)=(Qk(t))kQ(t) = (Q_k(t))_kQ(t)=(Qk​(t))k​, the fluid levels, and T(t)=(Tk(t))kT(t) = (T_k(t))_kT(t)=(Tk​(t))k​, the cumulative service time given to each class, such that for t≥0t \ge 0t≥0:

Qk(t)=Qk(0)+μk−1Tk−1(t)−μkTk(t),Qk(t)≥0,Q_k(t) = Q_k(0) + \mu_{k-1}T_{k-1}(t) - \mu_k T_k(t), \qquad Q_k(t) \ge 0,Qk​(t)=Qk​(0)+μk−1​Tk−1​(t)−μk​Tk​(t),Qk​(t)≥0,

with μ0T0(t)=t\mu_0T_0(t) = tμ0​T0​(t)=t; each TkT_kTk​ starts at 000 and is nondecreasing; and the idle time Ui(t)=t−∑k∈CiTk(t)U_i(t) = t - \sum_{k\in C_i}T_k(t)Ui​(t)=t−∑k∈Ci​​Tk​(t) of each station is nondecreasing.

A buffer priority discipline is a permutation π\piπ of the classes; a class kkk has priority over a class lll at the same station when π(k)<π(l)\pi(k) < \pi(l)π(k)<π(l). Write Hk={l∈Cσ(k):π(l)≤π(k)}H_k = \{l \in C_{\sigma(k)} : \pi(l) \le \pi(k)\}Hk​={l∈Cσ(k)​:π(l)≤π(k)}, Tk+=∑l∈HkTlT_k^+ = \sum_{l\in H_k}T_lTk+​=∑l∈Hk​​Tl​, Uk+(t)=t−Tk+(t)U_k^+(t) = t - T_k^+(t)Uk+​(t)=t−Tk+​(t) and Wk+=∑l∈HkmlQlW_k^+ = \sum_{l\in H_k} m_l Q_lWk+​=∑l∈Hk​​ml​Ql​. Under preemptive resume, Uk+U_k^+Uk+​ may increase only at times when Wk+=0W_k^+ = 0Wk+​=0 (condition (4.4)): a station never idles toward the classes of priority at least that of kkk while any of them holds fluid. FBFS is π(k)=k\pi(k) = kπ(k)=k, so earlier steps of the route have priority.

The fluid model is stable (Definition 1.3) if there is a time δ>0\delta > 0δ>0 such that every solution with ∣Q(0)∣=∑kQk(0)=1|Q(0)| = \sum_k Q_k(0) = 1∣Q(0)∣=∑k​Qk​(0)=1 has Q(t)=0Q(t) = 0Q(t)=0 for all t≥δt \ge \deltat≥δ.

Formalization targets

Goal: Theorem 4.3

For every reentrant line with mk>0m_k > 0mk​>0 and (1.7),

the fluid model (1.8)–(1.12), (4.4) with π(k)=k is stable.\text{the fluid model (1.8)–(1.12), (4.4) with } \pi(k) = k \text{ is stable.}the fluid model (1.8)–(1.12), (4.4) with π(k)=k is stable.

The goal asserts existence of an emptying time; it does not fix the value.

Milestones

  1. Lemma 2.2 (i): a nonnegative function has zero derivative wherever it vanishes and is differentiable.
  2. Lemma 2.2 (ii): an absolutely continuous nonnegative ggg whose derivative is at most −ε-\varepsilon−ε wherever g>0g > 0g>0 vanishes from g(0)/εg(0)/\varepsilong(0)/ε on, and is nonincreasing.
  3. Proposition 4.2: at a regular time of a priority fluid model, an empty buffer has equal in- and out-flow rates, and at each station the highest-priority nonempty class satisfies ∑k∈Hk0mkdk=1\sum_{k\in H_{k_0}} m_kd_k = 1∑k∈Hk0​​​mk​dk​=1 while lower-priority classes have zero out-flow.
  4. Inductive step (proof of Theorem 4.3): once buffers 1,…,k−11,\dots,k-11,…,k−1 stay empty from tk−1t_{k-1}tk−1​ on, buffer kkk is empty from tk=tk−1+Qk(tk−1)mk/(1−∑l∈Hkml)t_k = t_{k-1} + Q_k(t_{k-1})m_k/(1 - \sum_{l\in H_k} m_l)tk​=tk−1​+Qk​(tk−1​)mk​/(1−∑l∈Hk​​ml​) on.
  5. Emptying time (proof of Theorem 4.3): every solution with ∣Q(0)∣=1|Q(0)| = 1∣Q(0)∣=1 is empty from
δ=∑k=1Kmk∏l=1k−1(1−∑j∈Hl∖{l}mj)∏l=1k(1−∑j∈Hlmj)\delta = \sum_{k=1}^K m_k\frac{\prod_{l=1}^{k-1}(1-\sum_{j\in H_l\setminus\{l\}}m_j)}{\prod_{l=1}^{k}(1-\sum_{j\in H_l}m_j)}δ=k=1∑K​mk​∏l=1k​(1−∑j∈Hl​​mj​)∏l=1k−1​(1−∑j∈Hl​∖{l}​mj​)​

on, which gives the goal with an explicit constant.

Significance

Combined with Dai's theorem (Theorem 1.1 of the paper), Theorem 4.3 gives positive Harris recurrence of every multiclass reentrant line operated under FBFS, under the distributional assumptions of that theorem, whenever (1.7) holds. Since Lu–Kumar-type examples show that priority rules can destabilize a network with spare capacity, a rule that is provably stable on every reentrant line is a meaningful guarantee. FBFS, together with LBFS, is the basic positive case against which the instability examples in the same paper (Theorem 5.1) are compared.

Formalizing the result adds a machine-checked version of the fluid model with priority constraints, stated for an arbitrary line rather than a fixed network, and a checked explicit emptying time. The result is proved in the paper; no machine-checked proof is known. The rate identities of Proposition 4.2 and the extinction lemma are reused by the LBFS mission of this series.

Difficulty

The fluid model gives the paths only as nondecreasing functions subject to equations; nothing says they are differentiable. Every argument about rates holds only at regular times, and the conclusion must be integrated back through absolute continuity, which itself must be derived from the monotonicity conditions. The priority condition (4.4) is an "increases only when empty" condition; turning it into the rate identity (4.6) at a regular point requires continuity of the fluid levels and a careful local argument. The induction over classes needs uniform control of every earlier buffer for all later times, not only at one instant, so a pointwise reading of "buffer k−1k-1k−1 is empty" is not enough. Finally, the explicit constant δ\deltaδ requires bounding the content of buffer kkk at time tk−1t_{k-1}tk−1​ by the total content, which may have grown since time 000.

Formalization scope

  • Classes and stations are Fin K and Fin I, 0-based: the paper's class kkk is Lean index k−1k-1k−1.
  • Paths are total functions ℝ → Fin K → ℝ; every equation is imposed on t≥0t \ge 0t≥0 only, and derivatives are taken at t>0t > 0t>0.
  • Conditions (1.13) and (4.4) are in interval form (ConstantWhile): the idle process is constant on every interval of [0,∞)[0,\infty)[0,∞) on which the content stays positive. This is equivalent to the paper's Stieltjes integral form for continuous paths.
  • Lipschitz continuity of the paths is not assumed; it follows from the monotonicity conditions.
  • mk>0m_k > 0mk​>0 is an explicit hypothesis; the paper takes it for granted.
  • Priorities are Equiv.Perm (Fin K), FBFS is the identity; ∣Q(0)∣|Q(0)|∣Q(0)∣ is ∑kQk(0)\sum_k Q_k(0)∑k​Qk​(0).
  • In Lemma 2.2 (ii) the printed strict "g˙(t)<−ε\dot g(t) < -\varepsilong˙​(t)<−ε" is relaxed to "≤−ε\le -\varepsilon≤−ε", as every application requires; absolute continuity is dropped from Lemma 2.2 (i), where it is not needed. Both changes strengthen the lemma.
  • In the inductive step, "stay empty for t>tk−1t > t_{k-1}t>tk−1​" is read as t≥tk−1t \ge t_{k-1}t≥tk−1​, and the case Qk(tk−1)=0Q_k(t_{k-1}) = 0Qk​(tk−1​)=0 is included.
  • The stochastic network is not formalized; only the fluid model is.

A trivializing formalization is ruled out: the goal uses the priority fluid model, not the work-conserving one alone (which would claim that every work-conserving fluid model is stable, false by Theorem 5.1), and a sorry-free witness shows that the FBFS solution predicate has solutions with ∣Q(0)∣=1|Q(0)| = 1∣Q(0)∣=1, so stability is not vacuous.

Contributions welcome: the extinction lemma for absolutely continuous functions, the derivation of Lipschitz continuity from (1.10)–(1.12), and the rate identities of Proposition 4.2 are reusable beyond this mission.

Selected references

  • J. G. Dai and G. Weiss, Stability and instability of fluid models for reentrant lines, Mathematics of Operations Research 21(1) (1996) 115–134. https://doi.org/10.1287/moor.21.1.115
  • J. G. Dai, On positive Harris recurrence of multiclass queueing networks: a unified approach via fluid limit models, Annals of Applied Probability 5(1) (1995) 49–77. https://doi.org/10.1214/aoap/1177004828
  • P. R. Kumar, Re-entrant lines, Queueing Systems 13 (1993) 87–110. https://doi.org/10.1007/BF01149327
  • S. H. Lu and P. R. Kumar, Distributed scheduling based on due dates and buffer priorities, IEEE Transactions on Automatic Control 36(12) (1991) 1406–1416. https://doi.org/10.1109/9.106159
8 thms2 active usersReviewed
Geometry & Topology·Captain: Lucas

Building Anosov flows on 3-manifolds (Béguin–Bonatti–Yu)Research Paper

Motivation

Anosov flows are the model of uniformly hyperbolic, chaotic continuous-time dynamics: a nonsingular vector field XXX on a closed manifold MMM is Anosov when the tangent bundle splits as TM=Es⊕RX⊕EuTM=E^s\oplus\mathbb RX\oplus E^uTM=Es⊕RX⊕Eu, with EsE^sEs uniformly contracted and EuE^uEu uniformly expanded by the derivative of the flow. They are structurally stable, so one can hope to classify them up to topological equivalence. In dimension three this classification is far from complete: it is not known which closed 3-manifolds carry Anosov flows, nor how many inequivalent Anosov flows a given manifold can carry.

The classical examples — suspensions of hyperbolic toral automorphisms and geodesic flows of hyperbolic surfaces — are rigid (Plante; Ghys). Non-algebraic examples were built by Franks–Williams (a nontransitive Anosov flow, 1980), Handel–Thurston, Goodman, Fried, Bonatti–Langevin, Fenley, Barbot and others. Several of these examples glue together neighbourhoods of hyperbolic sets along their boundaries. Béguin, Bonatti and Yu (Geom. Topol. 21 (2017)) turned this into a general theory, and used it to answer questions of Katok and of Barbot–Fenley.

Setting

A plug (U,X)(U,X)(U,X) is a compact 3-manifold UUU with boundary and a nonsingular C¹ vector field XXX transverse to ∂U\partial U∂U. The boundary splits into the entrance boundary ∂inU\partial^{in}U∂inU (where XXX points inwards) and the exit boundary ∂outU\partial^{out}U∂outU. The maximal invariant set Λ\LambdaΛ consists of the points whose orbit stays in UUU for all times. The plug is hyperbolic if Λ\LambdaΛ is a hyperbolic set with one-dimensional strong stable and strong unstable bundles. The entrance lamination LXs=Ws(Λ)∩∂inUL^s_X=W^s(\Lambda)\cap\partial^{in}ULXs​=Ws(Λ)∩∂inU and the exit lamination LXu=Wu(Λ)∩∂outUL^u_X=W^u(\Lambda)\cap\partial^{out}ULXu​=Wu(Λ)∩∂outU are one-dimensional laminations of the boundary surfaces. The plug has filling MS laminations when every component of ∂inU∖LXs\partial^{in}U\setminus L^s_X∂inU∖LXs​ (and of ∂outU∖LXu\partial^{out}U\setminus L^u_X∂outU∖LXu​) is a strip: a disc whose accessible boundary consists of two leaves asymptotic to each other at both ends.

A diffeomorphism φ:∂outU→∂inU\varphi:\partial^{out}U\to\partial^{in}Uφ:∂outU→∂inU is a strongly transverse gluing map if φ∗(LXu)\varphi_*(L^u_X)φ∗​(LXu​) and LXsL^s_XLXs​ are transverse and cut ∂inU\partial^{in}U∂inU into squares with sides alternately on leaves of the two laminations. Gluing then gives a closed manifold U/φU/\varphiU/φ with an induced vector field ZZZ. Two triples (U,X,φ)(U,X,\varphi)(U,X,φ) and (U,Y,ψ)(U,Y,\psi)(U,Y,ψ) are strongly isotopic if they are joined by a continuous path of such data.

Formalization targets

Goal: the gluing theorem (Theorem 1.5)

(U,X) hyperbolic plug with filling MS laminations, Λ without attractors or repellers, φ strongly transverse⟹ ∃ (Y,ψ) strongly isotopic to (X,φ) with the field induced by Y on U/ψ Anosov.\begin{gathered}(U,X)\ \text{hyperbolic plug with filling MS laminations},\ \Lambda\ \text{without attractors or repellers},\ \varphi\ \text{strongly transverse}\\ \Longrightarrow\ \exists\,(Y,\psi)\ \text{strongly isotopic to}\ (X,\varphi)\ \text{with the field induced by } Y \text{ on } U/\psi\ \text{Anosov}.\end{gathered}(U,X) hyperbolic plug with filling MS laminations, Λ without attractors or repellers, φ strongly transverse⟹ ∃(Y,ψ) strongly isotopic to (X,φ) with the field induced by Y on U/ψ Anosov.​

Milestones

  • Proposition 1.1: gluing two hyperbolic plugs along transverse laminations gives a hyperbolic plug. Proposition 1.3: strongly transverse gluing preserves filling MS laminations.
  • Lemma 3.27 (self-gluing case): the glued manifold U/φU/\varphiU/φ exists as a closed smooth manifold with an induced vector field.
  • Proposition 1.6: if the graph of basic pieces is strongly connected, the Anosov flow of Theorem 1.5 is transitive.
  • Theorem 1.8: every transitive Anosov flow on a closed 3-manifold is a factor of a transitive Anosov flow on another closed 3-manifold, restricted to a compact invariant set.
  • Theorem 1.9: some closed orientable 3-manifold carries both a transitive and a nontransitive Anosov flow.
  • Theorem 1.10 and Corollary 1.11: every MS foliation of a closed orientable surface is the entrance foliation of a transitive attracting hyperbolic plug; in particular incoherent transitive hyperbolic attractors exist.
  • Theorem 1.12: every hyperbolic plug with filling MS laminations embeds, up to topological equivalence, in an Anosov flow on a closed orientable 3-manifold, which can be taken transitive when Λ\LambdaΛ has no attractors or repellers.
  • Theorem 1.13: for every n≥1n\ge1n≥1 some closed orientable 3-manifold carries nnn pairwise inequivalent transitive Anosov flows.
  • Theorem 1.15: some transitive Anosov flow admits infinitely many pairwise nonisotopic transverse tori.

Significance

Theorem 1.5 lets one build Anosov flows on closed 3-manifolds by gluing hyperbolic plugs. Proposition 1.6 gives a combinatorial criterion for the result to be transitive. Together they answer a question of Katok (Theorem 1.9) and questions of Barbot and Fenley on manifolds with several hyperbolic JSJ pieces supporting transitive Anosov flows (Theorem 1.13). They also show that transitive Anosov flows admit no fully canonical decomposition into finitely many transverse tori (Theorem 1.15). The results are proved in the source paper. None of them is formalized, and Mathlib has no theory of hyperbolic sets for flows, stable manifolds or laminations. A formal proof therefore needs a substantial amount of reusable smooth dynamics.

Difficulty

The glued vector field is generally not hyperbolic: perturbing the gluing map can create solid tori of parallel periodic orbits. The difficulty is to choose the gluing map (and the vector field within its topological equivalence class) so that cone fields on ∂inU\partial^{in}U∂inU are mapped into themselves by the return map. The return map is the composition of the crossing map of the plug with the gluing map. Contraction and expansion must therefore be controlled simultaneously along two transverse invariant foliations. The paper achieves this after reducing to plugs with an affine Markov partition. The naive approach — fixing φ\varphiφ and trying to verify hyperbolicity — fails in general (Question 1.4 of the paper remains open).

Formalization scope

  • Manifolds are modelled on the half-space EuclideanHalfSpace 3 with a C∞C^\inftyC∞ structure; closed manifolds are compact, Hausdorff and BoundarylessManifold, and connected where the paper's statements concern a single manifold. Orientability is given by an atlas with positive Jacobians.
  • Vector fields are C¹ sections; flows are encoded by integral curves, so that partial flows on manifolds with boundary make sense; flowMap X t x is xxx when the orbit is undefined.
  • Hyperbolicity is quantified over a continuous Riemannian metric, invariant line fields and constants C,λ>0C,\lambda>0C,λ>0; continuity of the splitting is not imposed (it is automatic).
  • Filling MS laminations are encoded through the strip condition (Lemma 3.21); leaves of LsL^sLs are path components of intersections of weak stable manifolds with ∂inU\partial^{in}U∂inU.
  • The glued manifold U/φU/\varphiU/φ is not a quotient type: statements quantify over every closed smooth 3-manifold NNN with a surjective C¹ immersion q:U→Nq:U\to Nq:U→N realising the identification. Lemma 3.27 (a milestone) guarantees such NNN exists, so these statements are not vacuous. The induced field is not required to be C¹ and "Anosov" there means hyperbolicity of the whole manifold.
  • Useful reusable infrastructure: flows of C¹ vector fields on compact manifolds (with boundary), stable manifold theory, the λ-lemma, laminations and foliations of surfaces, and gluing of manifolds along boundary components.

Selected references

  • F. Béguin, C. Bonatti, B. Yu, Building Anosov flows on 3-manifolds, Geom. Topol. 21 (2017) 1837–1930. https://doi.org/10.2140/gt.2017.21.1837
59 thms2 active usersReviewed
Differential Geometry·Captain: Lucas

Pugh's Closing LemmaResearch Paper

Motivation

A periodic point of a map f ⁣:M→Mf\colon M\to Mf:M→M is a point xxx with fn(x)=xf^n(x)=xfn(x)=x for some n≥1n\ge 1n≥1. A nonwandering point is a much weaker form of recurrence: every neighbourhood UUU of xxx eventually returns to meet itself, fn(U)∩U≠∅f^n(U)\cap U\ne\emptysetfn(U)∩U=∅ for some n≥1n\ge 1n≥1. Every periodic point is nonwandering, but a nonwandering point need not be periodic, and the orbit of such a point may never come back to xxx exactly.

Pugh's closing lemma asserts that this gap can be closed by an arbitrarily small change of the system: if xxx is nonwandering for a C1C^1C1 diffeomorphism fff of a compact manifold, then some diffeomorphism ggg, as close to fff as desired in the C1C^1C1 topology, has xxx as a periodic point (Wikipedia, "Pugh's closing lemma"). The result was proved by C. C. Pugh in 1967 (Pugh 1967), in the same paper as the General Density Theorem: for a C1C^1C1-generic diffeomorphism the periodic points are dense in the nonwandering set. The source article describes the lemma as establishing a close relationship between chaotic and periodic behaviour and notes that it underlies some autonomous convergence theorems. The article also points to Smale's problems as related material.

Setting

Let MMM be a compact smooth manifold of dimension ddd, Hausdorff and without boundary. Write Diff1(M)\mathrm{Diff}^1(M)Diff1(M) for the set of C1C^1C1 diffeomorphisms g ⁣:M→Mg\colon M\to Mg:M→M: bijections such that ggg and g−1g^{-1}g−1 are continuously differentiable. For g∈Diff1(M)g\in\mathrm{Diff}^1(M)g∈Diff1(M), Tg ⁣:TM→TMTg\colon TM\to TMTg:TM→TM denotes its tangent map on the tangent bundle.

The C1C^1C1 topology on Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is the coarsest topology for which g↦Tgg\mapsto Tgg↦Tg is continuous, where the space C(TM,TM)C(TM,TM)C(TM,TM) of continuous self-maps of TMTMTM carries the compact-open topology. Two diffeomorphisms are C1C^1C1-close when they, and their derivatives, are uniformly close.

For a map h ⁣:X→Xh\colon X\to Xh:X→X of a topological space:

  • xxx is nonwandering if for every neighbourhood UUU of xxx there is n≥1n\ge 1n≥1 with hn(U)∩U≠∅h^n(U)\cap U\ne\emptysethn(U)∩U=∅; the nonwandering set is Ω(h)\Omega(h)Ω(h);
  • Per(h)={x:∃ n≥1, hn(x)=x}\mathrm{Per}(h)=\{x : \exists\, n\ge 1,\ h^n(x)=x\}Per(h)={x:∃n≥1, hn(x)=x} is the set of periodic points.

Formalization targets

Goal: Pugh's closing lemma

For every f∈Diff1(M)f\in\mathrm{Diff}^1(M)f∈Diff1(M) and every x∈Ω(f)x\in\Omega(f)x∈Ω(f),

∀ U a C1-neighbourhood of f,∃ g∈U,  x∈Per(g).\forall\ \mathcal U \text{ a } C^1\text{-neighbourhood of } f,\quad \exists\, g\in\mathcal U,\ \ x\in\mathrm{Per}(g).∀ U a C1-neighbourhood of f,∃g∈U,  x∈Per(g).

Milestones

  1. Per(f)⊆Ω(f)\mathrm{Per}(f)\subseteq\Omega(f)Per(f)⊆Ω(f) for any map fff.
  2. Ω(f)\Omega(f)Ω(f) is closed for any map fff.
  3. f(Ω(f))=Ω(f)f(\Omega(f))=\Omega(f)f(Ω(f))=Ω(f) for a homeomorphism fff.
  4. Ω(f)≠∅\Omega(f)\ne\emptysetΩ(f)=∅ for any map of a nonempty compact space.
  5. General Density Theorem (Pugh 1967): there is a residual set G⊆Diff1(M)\mathcal G\subseteq\mathrm{Diff}^1(M)G⊆Diff1(M) with
Per(g)‾=Ω(g)(g∈G).\overline{\mathrm{Per}(g)}=\Omega(g)\qquad (g\in\mathcal G).Per(g)​=Ω(g)(g∈G).

Milestones 1–4 are elementary background facts that are not stated in the source article; milestone 5 is the second theorem named in the title of the source's reference.

Significance

The result. The closing lemma turns a topological recurrence property into periodicity after a C1C^1C1-small perturbation. Combined with genericity arguments it gives the General Density Theorem, so that for generic C1C^1C1 diffeomorphisms the whole nonwandering set is the closure of the periodic orbits. It is one of the basic perturbation tools of C1C^1C1 generic dynamics.

Formalizing it. The theorem is classical and proved in the literature. The drafter is not aware of a machine-checked proof. A formalization needs the C1C^1C1 topology on diffeomorphism groups, local perturbation lemmas in charts and the combinatorics of the closing argument. None of these is currently available in Mathlib as far as the drafter knows.

Difficulty

The first idea is to take the returning piece of orbit near xxx and push it back to xxx with a small local perturbation. This fails in the C1C^1C1 topology. Moving a point by distance δ\deltaδ with a bump supported in a ball of radius rrr costs C1C^1C1 size about δ/r\delta/rδ/r, and the return may happen at a distance comparable to the size of the only available ball. The perturbation then fails to be C1C^1C1-small. The derivative DfnDf^nDfn along the return can also distort any fixed neighbourhood shape without bound. Controlling this distortion is the central difficulty.

Formalization scope

  • Diff1(M)\mathrm{Diff}^1(M)Diff1(M) and its C1C^1C1 topology come from the published definition file BCWCentralizer_Basic. Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is M ≃ₘ^1⟮𝓡 d, 𝓡 d⟯ M, and the topology is induced by g↦Tgg\mapsto Tgg↦Tg into C(TangentBundle, TangentBundle) with the compact-open topology. On a compact manifold this is the usual C1C^1C1 topology.
  • "Compact smooth manifold": a Hausdorff compact space with a C∞C^\inftyC∞ atlas modelled on Rd\mathbb R^dRd, so without boundary. ddd is arbitrary.
  • "Arbitrarily close" means that every neighbourhood of fff in the C1C^1C1 topology contains a suitable ggg. "Periodic" requires a period n≥1n\ge 1n≥1. Allowing n=0n=0n=0 would make every point periodic and the statement trivial.
  • The perturbation ggg is only required to be a C1C^1C1 diffeomorphism, matching Diff1(M)\mathrm{Diff}^1(M)Diff1(M) in the source.
  • The nonwandering notion is the definition item PughClosingLemma_nonwandering, shared by all statements. It is reusable for any topological dynamics mission.

Welcome contributions: a general theory of the C1C^1C1 topology on Diff1(M)\mathrm{Diff}^1(M)Diff1(M) (for example, that it is Baire), local perturbation lemmas, and proofs of the milestones.

Selected references

  • C. C. Pugh, An Improved Closing Lemma and a General Density Theorem, American Journal of Mathematics 89 (4), 1967, 1010–1021. https://doi.org/10.2307/2373414
  • Wikipedia, Pugh's closing lemma, revision 1304222873. https://en.wikipedia.org/w/index.php?title=Pugh%27s_closing_lemma&oldid=1304222873
  • V. Araújo, M. J. Pacifico, Three-Dimensional Flows, Springer, 2010, ISBN 978-3-642-11414-4.
8 thms2 active usersReviewed
Captain: Lucas

The C¹-generic diffeomorphism has trivial centralizer (Bonatti–Crovisier–Wilkinson)Research Paper

Motivation

Two commuting diffeomorphisms f,gf,gf,g of a manifold MMM share all of their dynamics: ggg permutes the orbits of fff and preserves every smooth and topological invariant of fff. The centralizer of f∈Diffr(M)f\in\mathrm{Diff}^r(M)f∈Diffr(M),

Zr(f)={g∈Diffr(M):fg=gf},Z^r(f)=\{g\in\mathrm{Diff}^r(M): fg=gf\},Zr(f)={g∈Diffr(M):fg=gf},

always contains the cyclic group ⟨f⟩={fn:n∈Z}\langle f\rangle=\{f^n:n\in\mathbb Z\}⟨f⟩={fn:n∈Z}, and fff has trivial centralizer when Zr(f)=⟨f⟩Z^r(f)=\langle f\rangleZr(f)=⟨f⟩. S. Smale asked whether diffeomorphisms with trivial centralizer are dense, residual, or even open and dense in Diffr(M)\mathrm{Diff}^r(M)Diffr(M) (one of Smale's problems for the 21st century).

Timeline: Kopell (1970) answered the question for r≥2r\ge2r≥2 on the circle; Palis–Yoccoz, Fisher and Burslem obtained results under hyperbolicity or partial hyperbolicity assumptions; Togawa treated generic Axiom A diffeomorphisms in the C1C^1C1 topology; Bonatti–Crovisier–Vago–Wilkinson showed that trivial-centralizer diffeomorphisms do not contain an open dense set in Diff1(M)\mathrm{Diff}^1(M)Diff1(M); and Bonatti–Crovisier–Wilkinson (this paper, arXiv:0804.1416) proved residuality in Diff1(M)\mathrm{Diff}^1(M)Diff1(M) for every compact manifold.

Setting

MMM is a closed (compact, boundaryless), connected smooth manifold of dimension ddd. Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is the space of C1C^1C1 diffeomorphisms of MMM with the C1C^1C1 topology; a subset is residual if it contains a countable intersection of open dense sets.

Formalization targets

Goal (Main Theorem, p. 3)

There is a residual subset R⊂Diff1(M)\mathcal R\subset\mathrm{Diff}^1(M)R⊂Diff1(M) such that for every f∈Rf\in\mathcal Rf∈R and every g∈Diff1(M)g\in\mathrm{Diff}^1(M)g∈Diff1(M) with fg=gffg=gffg=gf, one has g=fng=f^ng=fn for some n∈Zn\in\mathbb Zn∈Z.

Milestones

Following Section 2 of the paper: the classical upper-semicontinuity lemma used for Proposition 2.5, the wandering part of Theorem A (unbounded distortion is C1C^1C1-generic), Proposition 2.5 (density of trivial Lipschitz centralizers implies residuality) and Theorem 2.3 (residuality of trivial Lipschitz centralizers when dim⁡M≥2\dim M\ge2dimM≥2).

Significance

The theorem answers the second (and hence the first) part of Smale's question in the C1C^1C1 topology, and exhibits a precise link between dynamical properties of fff (large derivative and unbounded distortion) and the algebraic structure of fff inside the group Diff1(M)\mathrm{Diff}^1(M)Diff1(M). The result is proved in the literature; it has not been formalized.

Difficulty

The density of trivial centralizers comes from perturbation results (Theorems A and B) that change the derivative without changing the topological dynamics (tidy perturbations in topological towers). Density alone does not give residuality, since the set of diffeomorphisms with the large derivative property is not residual (Appendix); the passage from dense to residual needs the Lipschitz centralizer and a semicontinuity argument.

Formalization scope

MMM is a charted space over Rd\mathbb R^dRd with a C∞C^\inftyC∞ atlas, Hausdorff, compact and connected; Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is Mathlib's type of C1C^1C1 diffeomorphisms. The C1C^1C1 topology is encoded as the topology induced by f↦Tff\mapsto Tff↦Tf into the compact-open topology on continuous self-maps of the tangent bundle TMTMTM. Powers fnf^nfn, n∈Zn\in\mathbb Zn∈Z, are taken in the permutation group of MMM. Bi-Lipschitz homeomorphisms are defined chart-locally (equivalent on a compact manifold to bi-Lipschitz for a Riemannian distance). Jacobians ∣det⁡Dfn∣|\det Df^n|∣detDfn∣ are computed with respect to an arbitrary continuous Riemannian metric; the unbounded-distortion property does not depend on this choice.

Contributions welcome: the C1C^1C1 topology API (Baire property, continuity of composition), the Kupka–Smale and closing-lemma genericity results, and the perturbation machinery of Sections 3–7.

Selected references

  • C. Bonatti, S. Crovisier, A. Wilkinson, The C1C^1C1 generic diffeomorphism has trivial centralizer, Publ. Math. IHÉS 109 (2009); arXiv:0804.1416. https://arxiv.org/abs/0804.1416
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998).
  • N. Kopell, Commuting diffeomorphisms, Proc. Sympos. Pure Math. 14 (1970).
7 thms2 active usersReviewed
Algebraic Geometry·Captain: Lucas

Albouy–Kaloshin: Finiteness of Planar Five-Body Central ConfigurationsResearch Paper

Motivation

A central configuration of the Newtonian nnn-body problem is a placement of nnn point masses in which the gravitational acceleration of every body points toward the centre of mass and is proportional to its distance from it. Central configurations generate the only explicitly known solutions of the nnn-body problem (the homographic, or self-similar, motions), they are the possible limiting shapes of total collisions, and they organise the topology of the integral manifolds. Counting them is therefore a basic question of celestial mechanics.

Timeline.

  • Euler (1767) and Lagrange (1772) found all central configurations of three bodies: three collinear ones and the equilateral triangle.
  • Moulton (1910) showed there are exactly n!/2n!/2n!/2 collinear central configurations for any positive masses.
  • Chazy (1918) postulated that all central configurations are nondegenerate, which would imply finiteness; Wintner (1941) stated finiteness as a conjecture.
  • Palmore (1975) gave a degenerate example, refuting Chazy's postulate but not finiteness.
  • Smale (1998) listed finiteness of relative equilibria for every choice of positive masses as the 6th of his problems for the 21st century.
  • Hampton and Moeckel (2006) proved finiteness for n=4n = 4n=4, using heavy computer algebra (BKK theory).
  • Albouy and Kaloshin (2012) gave a new proof for n=4n = 4n=4 that avoids heavy computation, and proved finiteness for n=5n = 5n=5 except possibly for masses in a codimension-2 algebraic subset of the mass space. The case n≥6n \ge 6n≥6, and the n=5n = 5n=5 case for the excluded masses, remain open.

Setting

Fix nnn bodies with masses m1,…,mnm_1,\dots,m_nm1​,…,mn​; body kkk sits at (xk,yk)∈R2(x_k,y_k)\in\mathbb R^2(xk​,yk​)∈R2. Write xkl=xl−xkx_{kl}=x_l-x_kxkl​=xl​−xk​, ykl=yl−yky_{kl}=y_l-y_kykl​=yl​−yk​ and rkl=xkl2+ykl2r_{kl}=\sqrt{x_{kl}^2+y_{kl}^2}rkl​=xkl2​+ykl2​​. A configuration with all rkl>0r_{kl}>0rkl​>0 is a central configuration (normalised so that the proportionality constant is 111) when, for every kkk,

(xkyk)=∑l≠kml rkl−3(xk−xlyk−yl).\begin{pmatrix}x_k\\ y_k\end{pmatrix}=\sum_{l\ne k} m_l\, r_{kl}^{-3}\begin{pmatrix}x_k-x_l\\ y_k-y_l\end{pmatrix}.(xk​yk​​)=l=k∑​ml​rkl−3​(xk​−xl​yk​−yl​​).

These equations are invariant under rotations of the plane; imposing y12=0y_{12}=0y12​=0 removes this freedom, and a solution with this normalisation is a positive normalized central configuration (Definition 1 of the paper; Lean: PosNormalizedCC n m).

The proof works in the complex domain. Introducing unknowns δkl\delta_{kl}δkl​ (inverse distances) with δkl2(xkl2+ykl2)=1\delta_{kl}^2(x_{kl}^2+y_{kl}^2)=1δkl2​(xkl2​+ykl2​)=1 turns the equations into the polynomial system (4) on C2n×Cn(n−1)/2\mathbb C^{2n}\times\mathbb C^{n(n-1)/2}C2n×Cn(n−1)/2:

xk=∑l≠kml δkl3 (xk−xl),yk=∑l≠kml δkl3 (yk−yl),y12=0.x_k=\sum_{l\ne k} m_l\,\delta_{kl}^3\,(x_k-x_l),\qquad y_k=\sum_{l\ne k} m_l\,\delta_{kl}^3\,(y_k-y_l),\qquad y_{12}=0 .xk​=l=k∑​ml​δkl3​(xk​−xl​),yk​=l=k∑​ml​δkl3​(yk​−yl​),y12​=0.

A complex solution is a normalized central configuration (Lean: NormalizedCC n m), a real one if all xk,ykx_k,y_kxk​,yk​ are real (Lean: RealNormalizedCC n m). The potential is U=∑k<lmkmlδklU=\sum_{k<l}m_km_l\delta_{kl}U=∑k<l​mk​ml​δkl​ (Lean: potential n m).

Formalization targets

Goal — Theorem 2 (planar five bodies)

There is a closed algebraic subset A⊂R5A\subset\mathbb R^5A⊂R5 of codimension at least 222 such that for all masses m∈(R>0)5∖Am\in(\mathbb R_{>0})^5\setminus Am∈(R>0​)5∖A,

#{positive normalized central configurations of the planar 5-body problem with masses m}<∞.\#\{\text{positive normalized central configurations of the planar 5-body problem with masses } m\}<\infty .#{positive normalized central configurations of the planar 5-body problem with masses m}<∞.

The exceptional set is not made explicit; only its existence and dimension bound are asserted.

Stronger — Theorem 6

The same statement with all complex solutions of system (4) in place of the positive real ones.

Four bodies — Theorems 1, 3, 4, 5

For n=4n=4n=4 and every positive masses: finitely many positive (Theorem 1, Hampton–Moeckel) and even real (Theorem 5) normalized central configurations; finitely many complex ones unless the masses satisfy explicit polynomial relations (Theorem 3) or are all equal (Theorem 4).

Tools — Lemmas 1 and 2 and an explicit example

Lemma 1 (a polynomial image of an affine variety is finite or cofinite), Lemma 2 (the potential takes finitely many values on the solution set), and the explicit mass vector (1,2,3,4,5)(1,2,3,4,5)(1,2,3,4,5).

Significance

The result. Theorem 2 is the first finiteness result for planar central configurations of five bodies, settling Smale's 6th problem for n=5n=5n=5 for generic masses; before it, no single 5-tuple of positive masses was known to have finitely many planar central configurations. Its four-body part gives a short proof of the Hampton–Moeckel theorem, including the real (not necessarily positive) solutions.

Formalizing it. The results are proved on paper; none of them is formalized. A formal development requires affine elimination theory (Chevalley's theorem on constructible images in the form of Lemma 1), a Sard-type argument on algebraic sets (Lemma 2), and the singular-sequence analysis of Sections 3–9, which is a long case analysis of limiting diagrams together with polynomial eliminations done by computer algebra in the paper.

Difficulty

Finiteness is not a local statement: nondegeneracy fails in general (Palmore), so no implicit-function argument applies, and a continuum of solutions would have to be excluded globally. In the complex domain continua genuinely exist for some masses (Roberts' continuum with a negative mass; its sign-modified version with positive masses solves system (4)), so any proof must use the positivity of the masses in an essential way, and the exceptional mass set of Theorem 2 cannot simply be dropped with the present method.

Formalization scope

  • Bodies are indexed by Fin n; the paper's bodies 111 and 222 are the indices 0 and 1, so the normalisation reads y 1 - y 0 = 0.
  • Masses are real (and hypothesised positive) in all main theorems; in the definition of NormalizedCC they are complex, as in Section 2 of the paper. Lemma 2 carries the paper's standing hypothesis that no nonempty subset of bodies has total mass zero (NoZeroSubMass).
  • A point of system (4) is a triple (x, y, δ); δ is a full n × n array constrained to be symmetric with zero diagonal, so it carries exactly the n(n−1)/2n(n-1)/2n(n−1)/2 unknowns δkl\delta_{kl}δkl​, k<lk<lk<l. Finiteness of the solution set is unaffected by this encoding.
  • "Closed algebraic subset of codimension 2 of the mass space" is encoded as the real zero locus massZeroLocus I of an ideal I of R[m1,…,m5]\mathbb R[m_1,\dots,m_5]R[m1​,…,m5​] with ringKrullDim (ℝ[m] ⧸ I) ≤ 3. Taking I=0I=0I=0 is impossible (the quotient has dimension 555), so the goal is not trivialised by an exceptional set equal to the whole mass space.
  • Finiteness is Set.Finite of the solution set.

Useful reusable infrastructure: finite-or-cofinite images of polynomial maps on affine varieties, and basic facts on central configurations (centre of mass, the identity I=UI=UI=U).

Selected references

  • A. Albouy, V. Kaloshin, Finiteness of central configurations of five bodies in the plane, Annals of Mathematics 176 (2012), 535–588. https://doi.org/10.4007/annals.2012.176.1.10
  • M. Hampton, R. Moeckel, Finiteness of relative equilibria of the four-body problem, Inventiones Mathematicae 163 (2006), 289–312. https://doi.org/10.1007/s00222-005-0461-0
  • S. Smale, Mathematical problems for the next century, The Mathematical Intelligencer 20 (1998), 7–15. https://doi.org/10.1007/BF03025291
10 thms2 active usersReviewed
Captain: Lucas

Hilbert's 16th Problem for Algebraic Limit Cycles (Llibre's Conjecture)Open Problem

Motivation

The second part of Hilbert's 16th problem (Paris, 1900) asks for the maximal number and the relative position of the limit cycles of a planar polynomial differential system

x˙=P(x,y),y˙=Q(x,y),\dot x = P(x,y),\qquad \dot y = Q(x,y),x˙=P(x,y),y˙​=Q(x,y),

where P,QP,QP,Q are real polynomials of degree at most ddd. Smale listed it in 1998 among the mathematical problems for the next century and remarked that, apart from the Riemann hypothesis, it seems the hardest of Hilbert's problems (Smale 1998). Even for d=2d = 2d=2 it is not known whether the number of limit cycles is uniformly bounded.

J. Llibre's survey Sobre el problema 16 de Hilbert (La Gaceta de la RSME 18 (2015), 543–554) organises the question into seven problems and concentrates on a more tractable restriction: algebraic limit cycles, i.e. limit cycles contained in a real algebraic curve. For this restriction there is an explicit conjecture for the maximal number (Conjecture 1 of the survey, first stated in Llibre–Ramírez–Sadovskaia 2010). This mission formalizes that conjecture as its goal, together with the results of the survey on which it rests.

Timeline (as reported in the survey):

  • 1891–1897 — Poincaré introduces limit cycles and proves finiteness for systems without saddle connections.
  • 1900 — Hilbert poses the 16th problem.
  • 1923 — Dulac claims every polynomial system has finitely many limit cycles; in 1985 Ilyashenko finds a gap.
  • 1957/1959 — Petrovskii and Landis claim H(2)=3H(2)=3H(2)=3 and later find an error; 1979 (Chen–Wang) and 1982 (Shi) give quadratic systems with 4 limit cycles.
  • 1986 — Bamon proves finiteness for quadratic systems; 1991/1992 — Ilyashenko and Écalle independently prove finiteness for all polynomial systems.
  • 2001 — Christopher realises any non-singular algebraic curve's bounded components as hyperbolic limit cycles of a system of the same degree (Christopher 2001).
  • 2004 — Llibre and Rodríguez show every configuration of limit cycles is realisable by algebraic limit cycles (Llibre–Rodríguez 2004).
  • 2007 — Llibre and Zhao give a cubic system with two algebraic limit cycles (Llibre–Zhao 2007).
  • 2010 — Llibre, Ramírez and Sadovskaia bound the number of algebraic limit cycles when all invariant algebraic curves are generic, and state the conjecture.

Setting

A polynomial vector field is a pair V=(P,Q)V = (P, Q)V=(P,Q) of real polynomials in x,yx,yx,y; its degree is max⁡(deg⁡P,deg⁡Q)\max(\deg P, \deg Q)max(degP,degQ). A solution is a differentiable curve γ:R→R2\gamma:\mathbb R\to\mathbb R^2γ:R→R2 with γ′(t)=(P,Q)(γ(t))\gamma'(t) = (P,Q)(\gamma(t))γ′(t)=(P,Q)(γ(t)) for all ttt. A periodic orbit is the image of a non-constant periodic solution. A limit cycle is a periodic orbit OOO that is isolated among periodic orbits: some open set U⊇OU \supseteq OU⊇O contains no periodic orbit other than OOO.

A limit cycle is algebraic if it is contained in the zero set {f=0}\{f = 0\}{f=0} of a non-zero real polynomial fff. The algebraic Hilbert number Ha(d)H_a(d)Ha​(d) is the supremum, over all polynomial vector fields of degree at most ddd, of the number of algebraic limit cycles (a value in N∪{∞}\mathbb N \cup \{\infty\}N∪{∞}).

A curve f=0f = 0f=0 is invariant with cofactor KKK if P fx+Q fy=KfP\,f_x + Q\,f_y = K fPfx​+Qfy​=Kf. A family of irreducible curves is generic if (i) no curve is singular, (ii) the top-degree homogeneous part of each curve is square-free, (iii) distinct curves meet transversally, (iv) no three distinct curves share a point, and (v) the top-degree homogeneous parts of distinct curves are coprime.

Formalization targets

Goal — Conjecture 1 (Llibre–Ramírez–Sadovskaia)

Ha(d)=1+(d−1)(d−2)2(d≥2).H_a(d) = 1 + \frac{(d-1)(d-2)}{2}\qquad (d \ge 2).Ha​(d)=1+2(d−1)(d−2)​(d≥2).

The equality asserts both that the number of algebraic limit cycles is bounded by the right-hand side for every field of degree at most ddd, and that the bound is attained.

Milestones (in the order of the survey)

  1. §2, Problem 1 — every polynomial vector field has finitely many limit cycles (Écalle, Ilyashenko).
  2. §3 — H(1)=0H(1) = 0H(1)=0: vector fields of degree at most 111 have no limit cycles.
  3. Theorem 1(a),(b) — every configuration of limit cycles is realised, and realised by algebraic limit cycles in degree ≤2(n+r)−1\le 2(n+r)-1≤2(n+r)−1.
  4. Theorem 2 (Christopher) — the bounded components of a non-singular curve f=0f = 0f=0 are exactly the limit cycles, all hyperbolic, of x˙=αf−Dfy\dot x = \alpha f - D f_yx˙=αf−Dfy​, y˙=βf+Dfx\dot y = \beta f + D f_xy˙​=βf+Dfx​.
  5. Proposition 3 — invariance of fff is equivalent to invariance of its irreducible factors, with Kf=∑niKfiK_f = \sum n_i K_{f_i}Kf​=∑ni​Kfi​​.
  6. Theorem 4(a),(b) — for degree d≥2d \ge 2d≥2 and generic invariant curves, at most 1+(d−1)(d−2)21 + \frac{(d-1)(d-2)}{2}1+2(d−1)(d−2)​ (even ddd) or (d−1)(d−2)2\frac{(d-1)(d-2)}{2}2(d−1)(d−2)​ (odd ddd) algebraic limit cycles, and the bounds are attained.
  7. §7 example — the cubic system x˙=2y(10+xy)\dot x = 2y(10+xy)x˙=2y(10+xy), y˙=20x+y−20x3−2x2y+4y3\dot y = 20x + y - 20x^3 - 2x^2 y + 4y^3y˙​=20x+y−20x3−2x2y+4y3 has two algebraic limit cycles in 2x4−4x2+4y2+1=02x^4 - 4x^2 + 4y^2 + 1 = 02x4−4x2+4y2+1=0.
  8. Conjecture 2 — Ha(2)=1H_a(2) = 1Ha​(2)=1.
  9. Theorem 5 (Giacomini–Llibre–Viano) — an inverse integrating factor vanishes on every limit cycle.

Significance

A proof of the goal would settle Problems 6 and 7 of the survey: it would give a uniform bound, depending only on the degree, for the number of algebraic limit cycles, and identify the sharp value. The conjecture is consistent with every example known to the survey: the generic bound of Theorem 4 is sharp for even ddd, and the known non-generic examples exceed the generic bound only in odd degree and by one. Conjecture 2 (d=2d = 2d=2) is its first open case.

On the formal side, the milestones require a reusable library of planar dynamics that is currently absent from Mathlib: periodic orbits and limit cycles of planar vector fields, hyperbolicity via the divergence integral, inverse integrating factors, invariant algebraic curves and Darboux-type arguments, and topological configurations of Jordan curves. Theorems 1, 2, 4 and 5, Proposition 3 and the cubic example are proved in the literature but, as far as the proposal author knows, not formalized; the goal and Conjecture 2 are open.

Difficulty

The obvious route bounds the number of ovals of the invariant curve (Harnack's theorem) and relates the degree of the curve to the degree of the field. This fails because a field of degree ddd can have invariant curves of arbitrarily high degree, so no a-priori degree bound on the curve is available; Theorem 4 obtains one only under the genericity conditions (i)–(v), and the degree-3 example shows that non-generic curves behave differently. On the formal side, the dynamical milestones (Theorems 2 and 5, the cubic example) need Poincaré–Bendixson-type planar topology and uniqueness of solutions, which Mathlib does not yet provide.

Formalization scope

  • Polynomials are MvPolynomial (Fin 2) ℝ with variable 0 as xxx and 1 as yyy; points are ℝ × ℝ. The degree of a field is the maximum of the total degrees of PPP and QQQ, and Ha(d)H_a(d)Ha​(d) ranges over fields of degree at most ddd, matching equation (1) of the survey.
  • Counts of limit cycles are Set.encard values in ℕ∞, so an infinite family is ∞\infty∞, never silently 000; Ha(d)H_a(d)Ha​(d) is an iSup in ℕ∞, so the goal also asserts finiteness.
  • Solutions are global (HasDerivAt at every real time). A limit cycle is isolated among periodic orbits contained in a neighbourhood. An algebraic limit cycle lies in the zero set of some non-zero polynomial, with no degree restriction on the curve.
  • Genericity conditions (i), (iii), (iv) are imposed at complex points of C2\mathbb C^2C2; (ii), (v) use square-freeness and coprimality in R[x,y]\mathbb R[x,y]R[x,y]; "distinct curves" means non-associated polynomials.
  • Hyperbolicity of a limit cycle is encoded by a non-zero divergence integral over one period.
  • Theorem 1(b) is formalized without its final sentence (existence of a Darboux first integral).
  • Trivializing encodings are ruled out: algebraic limit cycles require a non-zero polynomial, and the conjecture is an equality in ℕ∞, not an inequality over a possibly empty family.

Contributions welcome: a planar ODE library (uniqueness, flows, Poincaré–Bendixson), Darboux theory of integrability, and proofs of the classical milestones.

Selected references

  • J. Llibre, Sobre el problema 16 de Hilbert, La Gaceta de la RSME 18 (2015), no. 3, 543–554 (source of this mission).
  • J. Llibre, R. Ramírez, N. Sadovskaia, On the 16th Hilbert problem for algebraic limit cycles, J. Differential Equations 248 (2010), 1401–1409. https://doi.org/10.1016/j.jde.2009.11.023
  • J. Llibre, G. Rodríguez, Configurations of limit cycles and planar polynomial vector fields, J. Differential Equations 198 (2004), 374–380. https://doi.org/10.1016/j.jde.2003.10.008
  • C. Christopher, Polynomial vector fields with prescribed algebraic limit cycles, Geom. Dedicata 88 (2001), 255–258. https://doi.org/10.1023/a:1013171019668
  • H. Giacomini, J. Llibre, M. Viano, On the nonexistence, existence and uniqueness of limit cycles, Nonlinearity 9 (1996), 501–516. https://doi.org/10.1088/0951-7715/9/2/013
  • J. Llibre, Y. Zhao, Algebraic limit cycles in polynomial systems of differential equations, J. Phys. A 40 (2007), 14207–14222. https://doi.org/10.1088/1751-8113/40/47/012
  • Yu. Ilyashenko, Centennial history of Hilbert's 16th problem, Bull. Amer. Math. Soc. 39 (2002), 301–354. https://doi.org/10.1090/s0273-0979-02-00946-1
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998), no. 2, 7–15. https://doi.org/10.1007/bf03025291
15 thms2 active usersReviewed
Control TheoryLinear algebra·Captain: mikedeng1

Stabilization for a Perturbed Chain of Integrators in Prescribed Time I: Prescribed-Time Estimates for the Linear Time-Varying FeedbackResearch Paper

Motivation

Many control tasks have to settle at a given deadline, not merely eventually. Examples are missile guidance, where the interception time is fixed in advance, and rendezvous or consensus manoeuvres that must finish by a scheduled instant. Prescribed-time stabilization asks for a feedback that brings the state of a system to the origin at a time T>0T>0T>0 chosen by the designer, independently of the initial condition, and keeps this property under disturbances. It is stronger than finite-time stabilization, where the settling time depends on the initial state, and stronger than fixed-time stabilization, where it is only bounded uniformly.

Song, Wang, Holloway and Krstić (Automatica 2017) obtained prescribed-time regulation of normal-form systems with feedback gains that grow without bound as t→Tt\to Tt→T. The computations required explicit time derivatives of the gain function. Chitour, Ushirobira and Bouhemou (SIAM J. Control Optim. 2020) recast this construction as time-varying homogeneity: a time-dependent dilation of the state combined with a change of time turns the prescribed-time problem into a standard exponential-stabilization problem on an infinite horizon. The analysis then reduces to linear matrix inequalities. This mission formalizes the linear-feedback part of that paper (§3.1, pp. 1026–1030).

Timeline:

  • 2010: Chitour and Sigalotti (SIAM J. Control Optim. 48) prove a Lyapunov LMI for Jn−benKTJ_n - b e_n K^TJn​−ben​KT, uniform over a bounded range b‾≤b≤bˉ\underline b\le b\le\bar bb​≤b≤bˉ.
  • 2017: Song, Wang, Holloway and Krstić give prescribed-time regulation with a time-varying feedback.
  • 2020: Chitour, Ushirobira and Bouhemou remove the upper bound bˉ\bar bbˉ (Proposition 10) and derive the prescribed-time estimate by time-varying homogeneity (Corollary 14).

Setting

Fix a positive integer nnn and a prescribed time T>0T>0T>0. Let (ei)1≤i≤n(e_i)_{1\le i\le n}(ei​)1≤i≤n​ be the canonical basis of Rn\mathbb R^nRn, and let JnJ_nJn​ be the nnn-th Jordan block, Jnei=ei−1J_n e_i = e_{i-1}Jn​ei​=ei−1​ with e0=0e_0=0e0​=0. The perturbed chain of integrators is

x˙(t)=Jnx(t)+(d(t)+b(t)u(t))en,t∈[0,T),\dot x(t) = J_n x(t) + \big(d(t) + b(t)u(t)\big) e_n, \qquad t\in[0,T),x˙(t)=Jn​x(t)+(d(t)+b(t)u(t))en​,t∈[0,T),

with state x(t)∈Rnx(t)\in\mathbb R^nx(t)∈Rn and control u(t)∈Ru(t)\in\mathbb Ru(t)∈R. Here ddd is a measurable matched disturbance, and bbb is an uncertain control gain with b(t)≥b‾>0b(t)\ge\underline b>0b(t)≥b​>0 and no upper bound.

With weights ri=n−i+1r_i = n-i+1ri​=n−i+1, the dilation is Dμr=diag⁡(μr1,…,μrn)D^{\mathbf r}_\mu = \operatorname{diag}(\mu^{r_1},\dots,\mu^{r_n})Dμr​=diag(μr1​,…,μrn​) and Dr=diag⁡(r1,…,rn)D_{\mathbf r} = \operatorname{diag}(r_1,\dots,r_n)Dr​=diag(r1​,…,rn​). An admissible weight is a continuous function a≥0a\ge0a≥0 on [0,T][0,T][0,T] with ∫tTa>0\int_t^T a>0∫tT​a>0 for t<Tt<Tt<T. It defines

λ(t)=1∫tTa(ξ) dξ,s(t)=∫0tλ(ξ) dξ,0≤t<T.\lambda(t) = \frac{1}{\int_t^T a(\xi)\,d\xi},\qquad s(t) = \int_0^t\lambda(\xi)\,d\xi,\qquad 0\le t<T.λ(t)=∫tT​a(ξ)dξ1​,s(t)=∫0t​λ(ξ)dξ,0≤t<T.

The parameter λ\lambdaλ blows up at TTT, and sss maps [0,T)[0,T)[0,T) onto [0,∞)[0,\infty)[0,∞). In the coordinates y=Dλ(t)rxy = D^{\mathbf r}_{\lambda(t)}xy=Dλ(t)r​x and the time sss, the system becomes

y′=(aDr+Jn)y+(bu+d)en.y' = \big(a D_{\mathbf r} + J_n\big)y + (b u + d)e_n .y′=(aDr​+Jn​)y+(bu+d)en​.

The feedback studied is u=−KTDηryu = -K^T D^{\mathbf r}_\eta yu=−KTDηr​y, that is u(t)=−KTDηλ(t)rx(t)u(t) = -K^T D^{\mathbf r}_{\eta\lambda(t)}x(t)u(t)=−KTDηλ(t)r​x(t) in the original variables, where K∈RnK\in\mathbb R^nK∈Rn and η≥1\eta\ge1η≥1.

Formalization targets

Goal: Corollary 14 (corrected)

There is a rate μ>0\mu>0μ>0 depending only on nnn and b‾\underline bb​ such that, for every TTT and admissible aaa, there are KKK and C>0C>0C>0 with

∣xi(t)∣≤1(ηλ(t))n−i+1(Cηmax⁡(1,ηn−1)e−μηs(t)∥x(0)∥+Cmax⁡r∈[0,t]∣d(r)∣)|x_i(t)| \le \frac{1}{(\eta\lambda(t))^{n-i+1}}\Big(C\eta\max(1,\eta^{n-1})e^{-\mu\eta s(t)}\|x(0)\| + C\max_{r\in[0,t]}|d(r)|\Big)∣xi​(t)∣≤(ηλ(t))n−i+11​(Cηmax(1,ηn−1)e−μηs(t)∥x(0)∥+Cr∈[0,t]max​∣d(r)∣)

for every η≥1\eta\ge1η≥1, every b≥b‾b\ge\underline bb≥b​, every disturbance ddd, every closed-loop solution, every t∈[0,T)t\in[0,T)t∈[0,T) and every 1≤i≤n1\le i\le n1≤i≤n. Since λ(t)→∞\lambda(t)\to\inftyλ(t)→∞, every coordinate reaches 000 at the prescribed time TTT.

Milestones

  1. §3 (10): λ˙=aλ2\dot\lambda = a\lambda^2λ˙=aλ2, λ\lambdaλ is nondecreasing and tends to ∞\infty∞ at TTT, and sss is an increasing C1C^1C1 bijection [0,T)→[0,∞)[0,T)\to[0,\infty)[0,T)→[0,∞).
  2. §3 (7)–(11): the transformed dynamics.
  3. Proposition 10: ∃ρ,S,K\exists\rho,S,K∃ρ,S,K such that (Jn−benKT)TS+S(Jn−benKT)⪯−ρ Id(J_n - be_nK^T)^TS + S(J_n-be_nK^T)\preceq-\rho\,\mathrm{Id}(Jn​−ben​KT)TS+S(Jn​−ben​KT)⪯−ρId for all b≥b‾b\ge\underline bb≥b​.
  4. Proposition 11: the same LMI with aDraD_{\mathbf r}aDr​ added, uniformly in ∣a∣≤C0|a|\le C_0∣a∣≤C0​.
  5. Proposition 12 (corrected): the ISS estimate (17) in the time sss.
  6. Proposition 13: the η\etaη-scaled LMI (20).

Significance

Corollary 14 says that a linear feedback with a time-varying gain drives the chain of integrators to the origin at the designer's deadline TTT. The guarantee holds for every control gain b≥b‾b\ge\underline bb≥b​, however large, and gives an explicit input-to-state bound for the matched disturbance. The weight aaa is free, so the blow-up profile of the gain can be chosen, for example to converge faster than polynomially. Proposition 10 removes the upper bound on bbb from the classical LMI, and is of independent use for high-gain and persistently excited systems.

On formalization: the results are proved on paper; no formalization of them is known. The mission produces checked statements of the LMIs, the time change, and the prescribed-time estimate. Two printed estimates are false as stated, (17) and (23), and the mission states corrected versions (see Formalization scope). Formal proofs would certify the corrected constants.

Difficulty

The obvious approach is to take a Lyapunov function for the constant-coefficient closed loop and differentiate it along trajectories. This fails for two reasons. First, bbb ranges over an unbounded interval, so no compactness argument yields a common Lyapunov matrix, and a single SSS and KKK must work for all b≥b‾b\ge\underline bb≥b​ at once. Second, the transformed system carries the time-varying term a(s)Dra(s)D_{\mathbf r}a(s)Dr​, and in the original time the feedback gain λ(t)\lambda(t)λ(t) is unbounded. Estimates must survive both the rescaling by Dηλ(t)rD^{\mathbf r}_{\eta\lambda(t)}Dηλ(t)r​ and the change of time. Constants that look harmless in the new time, such as the condition number of SSS and the value λ(0)\lambda(0)λ(0), reappear in the original variables, and dropping them makes the printed estimates false.

Formalization scope

Lean representation: vectors of Rn\mathbb R^nRn are Fin n → ℝ, and coordinate i : Fin n is the paper's index i.val + 1, so rir_iri​ = n - i.val. Matrices are Matrix (Fin n) (Fin n) ℝ, and enKTe_nK^Ten​KT is vecMulVec (eN n) K. Matrix inequalities use the Loewner order (open scoped MatrixOrder), and "real symmetric positive definite" is PosDef. The norm ∥⋅∥\|\cdot\|∥⋅∥ is Euclidean, written out as eucNorm. Solutions are Carathéodory solutions in integral form: for every ttt in the interval, the right-hand side is integrable on [0,t][0,t][0,t] and the integral identity holds. This matches the paper's measurable bbb and ddd. The standing assumptions are n≥1n\ge1n≥1 (§3), T>0T>0T>0, aaa continuous and nonnegative on [0,T][0,T][0,T] with ∫tTa>0\int_t^Ta>0∫tT​a>0 on [0,T)[0,T)[0,T), and b≥b‾>0b\ge\underline b>0b≥b​>0. No upper bound on bbb is assumed anywhere. max⁡∣d∣\max|d|max∣d∣ is replaced by an arbitrary bound DDD of ∣d∣|d|∣d∣ on the interval.

Corrected statements, with milestone texts kept verbatim:

  • (17) as printed has no constant on the transient term and fails for n≥2n\ge2n≥2: with a≡1a\equiv1a≡1 and y(0)=e1y(0)=e_1y(0)=e1​, ∣y1∣|y_1|∣y1​∣ first increases. Proposition 12 is stated with CSC_SCS​ on that term.
  • (23) as printed fails at t=0t=0t=0 whenever ∫0Ta<1\int_0^Ta<1∫0T​a<1. The goal is stated with a constant CCC on the transient term, and KKK and CCC may depend on TTT and aaa. The rate μ\muμ and the disturbance gain CSC_SCS​ depend only on nnn and b‾\underline bb​, as on the page.
  • Proposition 13's undefined μ∗\mu_*μ∗​ is the ρ\rhoρ of its statement.
  • "λ\lambdaλ increasing" is read as nondecreasing.
  • Corollary 14's "t≥0t\ge0t≥0" is read as t∈[0,T)t\in[0,T)t∈[0,T).

Trivializing encodings are ruled out as follows. The integrability clause of IsIntegralSolution prevents a non-integrable right-hand side from integrating to 000. Every constant is quantified before the objects it must not depend on: the rate μ\muμ before TTT and aaa, KKK before η\etaη, and ρ,S,K\rho,S,Kρ,S,K before bbb. No statement weakens the estimates to mere convergence.

Needed infrastructure: Lyapunov estimates for absolutely continuous solutions, Loewner-order congruence, and interval-integral calculus for the time change. The LMI lemmas and the integral-form solution predicate are reusable in other control missions. Proofs of any milestone are welcome, and so are sharper constants.

Selected references

  • Y. Chitour, R. Ushirobira, H. Bouhemou, Stabilization for a Perturbed Chain of Integrators in Prescribed Time, SIAM J. Control Optim. 58(2):1022–1048, 2020. https://doi.org/10.1137/19M1285937
  • Y. Song, Y. Wang, J. Holloway, M. Krstić, Time-varying feedback for regulation of normal-form nonlinear systems in prescribed finite time, Automatica 83:243–251, 2017. https://doi.org/10.1016/j.automatica.2017.06.008
  • Y. Chitour, M. Sigalotti, On the stabilization of persistently excited linear systems, SIAM J. Control Optim. 48:4032–4055, 2010. https://doi.org/10.1137/080737812
10 thms2 active usersReviewed
ProbabilityReinforcement LearningStochastic Systems·Captain: mikedeng1

The O.D.E. Method for Convergence of Stochastic Approximation and Reinforcement Learning I: Stability and Almost-Sure Convergence under Tapering StepsizesResearch Paper

Motivation

Stochastic approximation is the family of recursive algorithms that locate a zero of a function observed only through noisy evaluations. It goes back to Robbins and Monro (1951) and today underlies stochastic gradient descent, temporal-difference learning, Q-learning and actor–critic methods in reinforcement learning, and models of learning by boundedly rational agents.

The standard analysis is the O.D.E. method (Ljung 1977; see Kushner and Yin 1997): the interpolated iterates are compared with the solutions of an ordinary differential equation, and convergence of the algorithm follows from the stability of that ODE. The method has one well-known gap. It assumes, rather than proves, that the iterates remain bounded with probability one. In applications this stability hypothesis is often the hardest part: for asynchronous Q-learning and adaptive critic algorithms, almost sure boundedness had been proved only for discounted cost or after adding a projection step (Borkar and Meyn, p. 460).

Borkar and Meyn (SIAM J. Control Optim. 38 (2000)) close this gap with a scaling argument borrowed from the fluid-model approach to the stability of queueing networks (Dai 1995; Dai and Meyn 1995). They show that boundedness itself follows from the asymptotic stability of the origin for a second, "fluid-limit" ODE obtained by rescaling the drift. This mission formalizes that stability theorem for tapering step sizes, and the convergence theorem that follows from it.

Setting

Fix d≥0d\ge 0d≥0 and work in Rd\mathbb R^dRd with the Euclidean norm. Let h:Rd→Rdh:\mathbb R^d\to\mathbb R^dh:Rd→Rd and let {a(n)}n≥0\{a(n)\}_{n\ge0}{a(n)}n≥0​ be a deterministic sequence of positive step sizes. On a probability space (Ω,F,P)(\Omega,\mathcal F,\mathsf P)(Ω,F,P), random vectors X(n)X(n)X(n) and M(n)M(n)M(n) satisfy the stochastic approximation recursion

X(n+1)=X(n)+a(n)[h(X(n))+M(n+1)],n≥0.(1.1)X(n+1) = X(n) + a(n)\big[h(X(n)) + M(n+1)\big], \qquad n\ge0. \tag{1.1}X(n+1)=X(n)+a(n)[h(X(n))+M(n+1)],n≥0.(1.1)

Its mean ODE is x˙=h(x)\dot x = h(x)x˙=h(x) (1.2). For r>0r>0r>0 the scaled field is hr(x)=h(rx)/rh_r(x)=h(rx)/rhr​(x)=h(rx)/r, with the scaled ODE x˙=hr(x)\dot x = h_r(x)x˙=hr​(x) (1.4).

  • (A1) hhh is Lipschitz; hr(x)→h∞(x)h_r(x)\to h_\infty(x)hr​(x)→h∞​(x) as r→∞r\to\inftyr→∞ for every xxx; and the origin is an asymptotically stable equilibrium of the fluid-limit ODE x˙=h∞(x)\dot x = h_\infty(x)x˙=h∞​(x) (1.5).
  • (A2) With Fn\mathcal F_nFn​ the history of the iterates up to time nnn, {M(n)}\{M(n)\}{M(n)} is a martingale difference sequence, E[M(n+1)∣Fn]=0\mathsf E[M(n+1)\mid\mathcal F_n]=0E[M(n+1)∣Fn​]=0, and for some constant C0<∞C_0<\inftyC0​<∞, E[∥M(n+1)∥2∣Fn]≤C0(1+∥X(n)∥2)\mathsf E[\|M(n+1)\|^2\mid\mathcal F_n]\le C_0(1+\|X(n)\|^2)E[∥M(n+1)∥2∣Fn​]≤C0​(1+∥X(n)∥2).
  • (TS) Tapering step sizes: 0<a(n)≤10<a(n)\le10<a(n)≤1, ∑na(n)=∞\sum_n a(n)=\infty∑n​a(n)=∞, ∑na(n)2<∞\sum_n a(n)^2<\infty∑n​a(n)2<∞.

A point x∗x^*x∗ is globally asymptotically stable for x˙=h(x)\dot x = h(x)x˙=h(x) if it is a Lyapunov-stable equilibrium and every solution converges to it.

Formalization targets

Goal: Theorem 2.2 (almost sure convergence)

Under (A1), (A2) and (TS), if x˙=h(x)\dot x=h(x)x˙=h(x) has a unique globally asymptotically stable equilibrium x∗x^*x∗, then for every initial condition X(0)∈RdX(0)\in\mathbb R^dX(0)∈Rd,

X(n)⟶x∗almost surely.X(n)\longrightarrow x^* \qquad \text{almost surely.}X(n)⟶x∗almost surely.

The goal contains no constants and no rates, only the qualitative conclusion.

Milestone: Theorem 2.1 (i) (almost sure boundedness)

Under (A1), (A2) and (TS), for every initial condition,

sup⁡n∥X(n)∥<∞almost surely.\sup_n \|X(n)\| < \infty \qquad \text{almost surely.}nsup​∥X(n)∥<∞almost surely.

Milestones: the lemmas of Section 4.1

  • Lemma 4.1: the fluid-limit ODE is globally exponentially asymptotically stable.
  • Lemma 4.2: the piecewise ODE solutions ϕ^\hat\phiϕ^​, ϕ∞\phi^\inftyϕ∞ used for comparison are bounded by a constant independent of the initial condition.
  • Lemma 4.3 (i), (ii): two discrete Bellman–Gronwall inequalities.
  • Lemma 4.4: for large scale rrr, every solution of x˙=hr(x)\dot x = h_r(x)x˙=hr​(x) from the unit ball is ϵ\epsilonϵ-small on a window [T,T+1][T,T+1][T,T+1].
  • Lemma 4.5: the rescaled iterates have uniformly bounded second moments, and the rescaled noise sum ξ\xiξ is an L2L^2L2-bounded martingale.
  • Lemma 4.6: almost surely the rescaled interpolated iterates ϕ\phiϕ track ϕ^\hat\phiϕ^​ and stay bounded.

Significance

The result. Theorem 2.1 (i) turns the stability hypothesis of the O.D.E. method into a checkable condition on a deterministic ODE. Theorem 2.2 then gives convergence to x∗x^*x∗ with no a priori boundedness assumption. The paper applies this to reinforcement learning, obtaining the first convergence proof for asynchronous Q-learning and adaptive critic algorithms for average-cost Markov decision processes (the asynchronous extension, Theorem 2.5, is sketched in the paper and is not part of this mission). The same fluid-limit criterion is now a textbook tool; see Borkar, Stochastic Approximation: A Dynamical Systems Viewpoint (2008), Chapter 3.

Formalizing it. The theorems are proved in the paper, and the proofs are short but rely on several standard facts stated informally: uniform convergence of hrh_rhr​ to h∞h_\inftyh∞​ on compact sets, continuous dependence of ODE solutions on initial data and on the vector field, and the martingale convergence theorem. No machine-checked version of the O.D.E. method or of this stability criterion is known to exist. A formal development would give a verified link between discrete-time stochastic recursions, martingale convergence in Mathlib, and the stability theory of Lipschitz ODEs.

Difficulty

The obvious approach is to compare the iterates with solutions of x˙=h(x)\dot x = h(x)x˙=h(x) over windows of fixed ODE time and to control the accumulated noise by martingale convergence. This fails without boundedness: the noise bound in (A2) grows with ∥X(n)∥\|X(n)\|∥X(n)∥, so the deviation from the ODE can only be controlled relative to the current size of the iterate, and nothing prevents the iterates from escaping to infinity.

A second difficulty is that the hypothesis (A1) concerns only the fluid limit h∞h_\inftyh∞​, which describes the drift at infinite scale. It says nothing directly about hhh at any finite state, and nothing about the noise. Any argument therefore has to transfer information from the limit r→∞r\to\inftyr→∞ to the recursion at random, path-dependent scales, uniformly over those scales, while the noise is controlled only relative to the current size of the iterate. In Lean this involves ODE comparison and Gronwall estimates on a random partition of the time axis, conditional second-moment estimates for a rescaled recursion, and a vector-valued L2L^2L2 martingale convergence argument, none of which is available off the shelf for this setting.

Formalization scope

The state space is EuclideanSpace ℝ (Fin d). An ODE solution is a forward solution on [0,∞)[0,\infty)[0,∞): the derivative is taken within [0,∞)[0,\infty)[0,∞) at each t≥0t\ge0t≥0, which makes solutions continuous there. Stability notions are the standard ones (Lyapunov stability; asymptotic, global asymptotic and global exponential stability, the last in the form ∥x(t)−x∗∥≤be−δt∥x(0)−x∗∥\|x(t)-x^*\|\le b e^{-\delta t}\|x(0)-x^*\|∥x(t)−x∗∥≤be−δt∥x(0)−x∗∥). All vector fields in the mission are Lipschitz, so forward solutions exist and are unique, and quantifying over "every solution" is meaningful.

The filtration in (A2) is the natural filtration of the iterates. Because a(n)>0a(n)>0a(n)>0, it carries the same information as the paper's σ(X(i),M(i),i≤n)\sigma(X(i),M(i),i\le n)σ(X(i),M(i),i≤n). (A2) includes integrability of M(n+1)M(n+1)M(n+1) and ∥M(n+1)∥2\|M(n+1)\|^2∥M(n+1)∥2, so that the conditional expectations are meaningful. The theorems quantify over every probability space and every noise process satisfying (A2); the goal and Theorem 2.1 (i) take a deterministic initial condition, as the paper does. Stating the goal for a particular noise model (no noise, or i.i.d. noise) would be a different and much weaker theorem, and is ruled out. "sup⁡n∥X(n)∥<∞\sup_n\|X(n)\|<\inftysupn​∥X(n)∥<∞" is boundedness above of the set of norms, not a real supremum, which Lean sets to 000 on unbounded sets. Second-moment suprema in Lemma 4.5 are taken in [0,∞][0,\infty][0,∞].

The proof objects of Section 4.1 (time grid t(n)t(n)t(n), blocks m(j)m(j)m(j) and T(j)T(j)T(j), scales r(j)r(j)r(j), the interpolation ϕ\phiϕ, the rescaled iterates and noise sum) are separate definitions built from the step sizes and the sample path, as on the page. The piecewise ODE solutions ϕ^\hat\phiϕ^​ and ϕ∞\phi^\inftyϕ∞ are characterized by a predicate, and the lemmas hold for every function satisfying it.

Useful infrastructure, reusable beyond this mission: Lipschitz ODE comparison and continuous-dependence estimates in Mathlib's ODE library, uniform convergence of hrh_rhr​ on compact sets, the discrete Gronwall lemmas, and L2L^2L2-bounded vector-valued martingale convergence. Contributions are welcome on any milestone. The two Gronwall lemmas and Lemma 4.1 are self-contained entry points.

Selected references

  • V. S. Borkar and S. P. Meyn, The O.D.E. Method for Convergence of Stochastic Approximation and Reinforcement Learning, SIAM J. Control Optim. 38(2):447–469, 2000. https://doi.org/10.1137/S0363012997331639
  • H. Robbins and S. Monro, A Stochastic Approximation Method, Ann. Math. Statist. 22(3):400–407, 1951. https://doi.org/10.1214/aoms/1177729586
  • L. Ljung, Analysis of Recursive Stochastic Algorithms, IEEE Trans. Automat. Control 22(4):551–575, 1977. https://doi.org/10.1109/TAC.1977.1101561
  • H. J. Kushner and G. G. Yin, Stochastic Approximation Algorithms and Applications, Springer, 1997. https://doi.org/10.1007/978-1-4899-2696-8
  • J. G. Dai, On Positive Harris Recurrence of Multiclass Queueing Networks: A Unified Approach via Fluid Limit Models, Ann. Appl. Probab. 5(1):49–77, 1995. https://doi.org/10.1214/aoap/1177004828
  • J. G. Dai and S. P. Meyn, Stability and Convergence of Moments for Multiclass Queueing Networks via Fluid Limit Models, IEEE Trans. Automat. Control 40(11):1889–1904, 1995. https://doi.org/10.1109/9.471210
  • V. S. Borkar, Stochastic Approximation: A Dynamical Systems Viewpoint, Cambridge University Press / Hindustan Book Agency, 2008. https://doi.org/10.1007/978-93-86279-38-5
17 thms2 active usersReviewed
EconomicsOperations ResearchOptimization·Captain: mikedeng1

Revenue Management in Crowdfunding 1: Optimal Pledge Level and Campaign Duration Under Triangular Valuations When Independent or Herding Backers DominateResearch Paper

Motivation

Reward-based crowdfunding platforms such as Kickstarter let a project creator collect pledges from the public for a fixed period. Two numbers are fixed before launch and cannot be changed afterwards: the pledge level ppp each backer pays, and the campaign duration TTT. A high pledge level earns more per backer but deters backers with low valuations; a long campaign gives more backers time to arrive but, because backers are paid out only at the end, discounts the project's value in their eyes. Zhang, Savin and Veeraraghavan (SSRN 3065267, published in Manufacturing & Service Operations Management, 2022, doi:10.1287/msom.2022.1147) model this trade-off as a revenue-management problem for a deterministic fluid model of the pledging process, with two kinds of backers: independent backers, who arrive on their own, and herding backers, who arrive at a rate proportional to the amount already pledged, in the spirit of the imitators of the Bass diffusion model. The mission formalizes the paper's model, its closed-form solution, and its main optimization result for valuations with a right-triangular distribution.

Setting

A campaign has a population I^>0\hat I>0I^>0 of independent backers, who arrive at rate k>0k>0k>0 times the number not yet arrived, and herding backers, who arrive at rate Λhqp\Lambda_h q pΛh​qp times the number of pledges made so far (Λh≥0\Lambda_h\ge0Λh​≥0 an arrival rate, q≥0q\ge0q≥0 a propensity). A backer's valuation VVV is drawn from a law on [0,vˉ][0,\bar v][0,vˉ] with survival function Fˉi\bar F_iFˉi​ (independent) or Fˉh\bar F_hFˉh​ (herding). A backer arriving at time t∈[0,T]t\in[0,T]t∈[0,T] pledges iff Ve−r(T−t)≥pVe^{-r(T-t)}\ge pVe−r(T−t)≥p, where r>0r>0r>0 is the backers' discount rate; that happens with probability Fˉ(per(T−t))\bar F(pe^{r(T-t)})Fˉ(per(T−t)). The numbers nip,niln^p_i,n^l_inip​,nil​ of pledging and lost independent backers obey the linear system (1)–(4),

dnipdt=k(I^−ni) Fˉi(per(T−t)),dnildt=k(I^−ni)(1−Fˉi(per(T−t))),ni=nip+nil,\frac{dn^p_i}{dt}=k(\hat I-n_i)\,\bar F_i(pe^{r(T-t)}),\qquad \frac{dn^l_i}{dt}=k(\hat I-n_i)\bigl(1-\bar F_i(pe^{r(T-t)})\bigr),\qquad n_i=n^p_i+n^l_i,dtdnip​​=k(I^−ni​)Fˉi​(per(T−t)),dtdnil​​=k(I^−ni​)(1−Fˉi​(per(T−t))),ni​=nip​+nil​,

and the herding counts nhp,nhln^p_h,n^l_hnhp​,nhl​ obey (8)–(10),

dnhpdt=Λhqp (nip+nhp) Fˉh(per(T−t)),dnhldt=Λhqp (nip+nhp)(1−Fˉh(per(T−t))),\frac{dn^p_h}{dt}=\Lambda_h q p\,(n^p_i+n^p_h)\,\bar F_h(pe^{r(T-t)}),\qquad \frac{dn^l_h}{dt}=\Lambda_h q p\,(n^p_i+n^p_h)\bigl(1-\bar F_h(pe^{r(T-t)})\bigr),dtdnhp​​=Λh​qp(nip​+nhp​)Fˉh​(per(T−t)),dtdnhl​​=Λh​qp(nip​+nhp​)(1−Fˉh​(per(T−t))),

all starting from 000. The total number of pledges is n(p,T)=nip(T)+nhp(T)n(p,T)=n^p_i(T)+n^p_h(T)n(p,T)=nip​(T)+nhp​(T), the revenue is π(p,T)=p n(p,T)\pi(p,T)=p\,n(p,T)π(p,T)=pn(p,T), and the creator solves

max⁡ π(p,T)over0<p≤vˉ,  0≤T≤1rln⁡(vˉ/p).(18)\max\ \pi(p,T)\quad\text{over}\quad 0<p\le\bar v,\ \ 0\le T\le\tfrac1r\ln(\bar v/p).\qquad(18)max π(p,T)over0<p≤vˉ,  0≤T≤r1​ln(vˉ/p).(18)

Two reduced revenue functions appear in the limiting regimes: without herding, Ri(p,T)=kI^pe−kT∫0TekxFˉi(perx)dxR_i(p,T)=k\hat Ipe^{-kT}\int_0^Te^{kx}\bar F_i(pe^{rx})dxRi​(p,T)=kI^pe−kT∫0T​ekxFˉi​(perx)dx (22); in the herding-dominated regime, the proxy Rh(p,T)=p∫0TFˉh(pery)dyR_h(p,T)=p\int_0^T\bar F_h(pe^{ry})dyRh​(p,T)=p∫0T​Fˉh​(pery)dy (27). A right-triangular law on [0,vˉ][0,\bar v][0,vˉ] has mode 000 (Fˉ(y)=(1−y/vˉ)2\bar F(y)=(1-y/\bar v)^2Fˉ(y)=(1−y/vˉ)2) or mode vˉ\bar vvˉ (Fˉ(y)=1−(y/vˉ)2\bar F(y)=1-(y/\bar v)^2Fˉ(y)=1−(y/vˉ)2).

Formalization targets

Goal: Proposition 7

With x0∗x^*_0x0∗​, x1∗x^*_1x1∗​ the explicit algebraic constants (34), (35):

  • (a) if k=rk=rk=r and Λh=0\Lambda_h=0Λh​=0, the unique maximizer of (18) is
(p∗,T∗)=(vˉx0∗−x0∗+1(x0∗)2+x0∗+1, 1rln⁡x0∗) (mode 0),(vˉ1+x1∗+(x1∗)2, 1rln⁡x1∗) (mode vˉ);(p^*,T^*)=\Bigl(\bar v\tfrac{x^*_0-\sqrt{x^*_0}+1}{(x^*_0)^2+x^*_0+1},\ \tfrac1r\ln x^*_0\Bigr)\ \text{(mode 0)},\qquad \Bigl(\tfrac{\bar v}{\sqrt{1+x^*_1+(x^*_1)^2}},\ \tfrac1r\ln x^*_1\Bigr)\ \text{(mode }\bar v);(p∗,T∗)=(vˉ(x0∗​)2+x0∗​+1x0∗​−x0∗​​+1​, r1​lnx0∗​) (mode 0),(1+x1∗​+(x1∗​)2​vˉ​, r1​lnx1∗​) (mode vˉ);
  • (b) the unique maximizer of RhR_hRh​ over the same feasible set is (β∗vˉ,1rln⁡1β∗)(\beta^*\bar v,\frac1r\ln\frac1{\beta^*})(β∗vˉ,r1​lnβ∗1​) with β∗\beta^*β∗ the unique root in (0,1)(0,1)(0,1) of ln⁡1β=32(β−43)2−16\ln\frac1\beta=\frac32(\beta-\frac43)^2-\frac16lnβ1​=23​(β−34​)2−61​ (mode 0), and (βvˉ,1rln⁡1β)(\beta\bar v,\frac1r\ln\frac1\beta)(βvˉ,r1​lnβ1​) with β=−W(−3e−3)/3\beta=\sqrt{-W(-3e^{-3})/3}β=−W(−3e−3)/3​ (mode vˉ\bar vvˉ).

Milestones

  1. Proposition 1 and Proposition 2: every solution of (1)–(4) and (8)–(10) equals the closed forms (5)–(7), (11)–(12), and these solve the systems.
  2. Corollary 2: n(p,T)n(p,T)n(p,T) equals the single integral (17); and (22): π=Ri\pi=R_iπ=Ri​ when Λh=0\Lambda_h=0Λh​=0.
  3. Proposition 4(a), (b): with Λh=0\Lambda_h=0Λh​=0, k=rk=rk=r, the optimal duration T∗(p)T^*(p)T∗(p) for each fixed ppp and the optimal pledge level p∗(T)p^*(T)p∗(T) for each fixed T>0T>0T>0, in closed form (23)–(26).
  4. Proposition 5(a), (b): the same for RhR_hRh​, (28)–(31).

Significance

Proposition 7 is the paper's answer, for triangular valuations, to the question that motivates it: how a creator should set both levers together. Its four cases show how the optimal pledge level and duration move between campaigns dominated by low- or high-valuation independent backers and those dominated by herding backers; in particular herding-dominated campaigns call for markedly longer durations. Propositions 4 and 5 are the "limited-flexibility" policies for platforms where one lever is fixed by convention, and they are what the joint optimization is built from.

The model results (Propositions 1–2, Corollary 2) are proved in the manuscript's Appendix. The proofs of Propositions 4, 5 and 7 are in the paper's online Technical Appendix, which is not part of the source this mission cites; the decomposition into milestones follows the statements of the main text. None of these results has a machine-checked proof. A formalization produces verified closed forms for a nonlinear-in-parameters pricing problem and pins down three printing slips of the source (below).

Difficulty

Propositions 1 and 2 concern linear ordinary differential equations whose coefficients jump whenever the valuation law has an atom, so the classical theory does not apply directly; solutions are absolutely continuous and must be handled in integral form, and uniqueness needs a Grönwall-type argument for measurable coefficients. Corollary 2 is an integration by parts and a change of variables inside a double integral with an exponential of an inner integral. For the optimization results the obstacle is not the first-order condition but the global statement: each "optimal" claim asserts a unique global maximizer over a curved feasible region whose boundary T=1rln⁡(vˉ/p)T=\frac1r\ln(\bar v/p)T=r1​ln(vˉ/p) is active in some cases (Proposition 5) and inactive in others (Proposition 4, Proposition 7(a)). The first-order conditions are cubic or quartic equations whose roots are given by trigonometric and Cardano-type formulas, and part (b) involves transcendental equations; matching the right root and excluding boundary maxima is where the work lies.

Formalization scope

The model is a structure Campaign with real parameters Ihat, k, r, Lh (Λh\Lambda_hΛh​), q, vbar and the survival functions Fbi, Fbh. Standing assumptions: I^,k,r,vˉ>0\hat I,k,r,\bar v>0I^,k,r,vˉ>0, Λh,q≥0\Lambda_h,q\ge0Λh​,q≥0, and each survival function is non-increasing, [0,1][0,1][0,1]-valued, 111 below 000 and 000 from vˉ\bar vvˉ on. The positivity p>0p>0p>0 is added to the feasible set of (18), since ln⁡(vˉ/p)\ln(\bar v/p)ln(vˉ/p) needs it and π(0,T)=0\pi(0,T)=0π(0,T)=0. The pledging probability P(Ve−r(T−t)≥p)\mathbb P(Ve^{-r(T-t)}\ge p)P(Ve−r(T−t)≥p) is written Fˉ(per(T−t))\bar F(pe^{r(T-t)})Fˉ(per(T−t)). The differential systems are stated in integral form with continuity on [0,T][0,T][0,T]; Propositions 1–2 assert both that every solution equals the closed forms and that the closed forms solve the system. "Optimal" always means: feasible, attaining the maximum, and the unique point that does. For a fixed TTT the optimal pledge level is posed only for T>0T>0T>0, because π(⋅,0)\pi(\cdot,0)π(⋅,0) and Rh(⋅,0)R_h(\cdot,0)Rh​(⋅,0) vanish identically.

Three corrections of printing slips are part of the statements: (12) is stated with the factor Λhqp\Lambda_h q pΛh​qp of (9) and with the inner integration limits read as uuu; (39) has the second root β=1\beta=1β=1, so uniqueness is posed on (0,1)(0,1)(0,1); (40) is printed with iii and a complex Lambert WWW, and is stated in the equivalent real form with W(−3e−3)W(-3e^{-3})W(−3e−3) characterized as the unique w∈(−1,0)w\in(-1,0)w∈(−1,0) with wew=−3e−3we^w=-3e^{-3}wew=−3e−3. Printed decimals (one of which, 0.191vˉ0.191\bar v0.191vˉ in (36), is wrong: the exact value is ≈0.198vˉ\approx0.198\bar v≈0.198vˉ) are not part of any statement.

Trivializing formalizations are ruled out: n(p,T)n(p,T)n(p,T) is built from (5) and (11), not defined as (17); the differential systems are integral equations, not their closed forms and not a classical-derivative condition that no solution of a discontinuous system satisfies; optimality is a unique-maximizer statement, not an sSup or a first-order condition; and part (b) maximizes the explicit function (27), not a limit Λh→∞\Lambda_h\to\inftyΛh​→∞.

The development needs interval integrals, the exponential, logarithm, square and cube roots from Mathlib, and a uniqueness argument for linear Volterra integral equations; the latter, and the change-of-variables identity behind (22) and Corollary 2, are reusable for other fluid models of diffusion. Proofs of any milestone, and alternative routes to Proposition 7 (for instance through the profile functions T↦π(p∗(T),T)T\mapsto\pi(p^*(T),T)T↦π(p∗(T),T)), are welcome.

Selected references

  • J. Zhang, S. Savin, S. Veeraraghavan, Revenue Management in Crowdfunding, manuscript of May 26, 2021, SSRN 3065267. https://ssrn.com/abstract=3065267 — published in Manufacturing & Service Operations Management, 2022. https://doi.org/10.1287/msom.2022.1147
  • F. M. Bass, A New Product Growth for Model Consumer Durables, Management Science 15(5), 1969, 215–227. https://doi.org/10.1287/mnsc.15.5.215
  • R. M. Corless, G. H. Gonnet, D. E. G. Hare, D. J. Jeffrey, D. E. Knuth, On the Lambert W function, Advances in Computational Mathematics 5, 1996, 329–359. https://doi.org/10.1007/BF02124750
10 thms1 active userReviewed
Group TheoryRepresentation Theory·Captain: Lucas

Spectral Gap Conjecture (Wikipedia): Random Elements of SU(2)Open Problem

Motivation

Finitely many rotations of the sphere generate a group whose orbits are typically dense. A basic quantitative question is how fast those orbits fill the sphere: after words of length ℓ\ellℓ in the generators, how uniformly are the points spread? The answer is controlled by the spectral gap of an averaging operator built from the generators. The question goes back to the Banach–Ruziewicz problem (uniqueness of rotation-invariant finitely additive measures on spheres), was studied by Lubotzky, Phillips and Sarnak in their work on distributing points on S2S^2S2 (LPS 1987), and was formulated as a conjecture about random generators by Gamburd, Jakobson and Sarnak. It also matters in quantum computing: a spectral gap for a gate set gives efficient approximation of every single-qubit gate by short gate sequences (Sawicki–Karnas 2017).

Timeline.

  • 1987 — Lubotzky, Phillips and Sarnak construct explicit rotations with optimal spectral gap using automorphic forms and pose the general question (LPS).
  • 2006 — Fisher proves a zero–one law: for n≥3n \ge 3n≥3 generators, either almost every nnn-tuple has a spectral gap or almost every nnn-tuple has none (Fisher, IMRN 2006, arXiv:math/0601050).
  • 2008 — Bourgain and Gamburd prove the spectral gap for elements of SU(2)SU(2)SU(2) with algebraic entries generating a free group (Invent. Math. 171).
  • 2012 — Bourgain and Gamburd extend this to dense subgroups of SU(d)SU(d)SU(d), d≥2d \ge 2d≥2, generated by finitely many elements with algebraic entries (JEMS 14, arXiv:1108.6264).

The tuples with algebraic entries form a Haar-null set, so the conjecture for random tuples remains open.

Setting

Let SU(d)SU(d)SU(d) be the group of complex d×dd\times dd×d matrices UUU with U∗U=UU∗=IU^*U = UU^* = IU∗U=UU∗=I and det⁡U=1\det U = 1detU=1, a compact group with its normalized Haar measure μd\mu_dμd​ (the unique left-invariant Borel probability measure). For g1,…,gn∈SU(d)g_1,\dots,g_n \in SU(d)g1​,…,gn​∈SU(d) the Hecke operator acts on functions f:SU(d)→Cf : SU(d) \to \mathbb Cf:SU(d)→C by

(zgf)(x)=∑j=1n(f(gjx)+f(gj−1x)).(z_g f)(x) = \sum_{j=1}^{n} \bigl( f(g_j x) + f(g_j^{-1} x) \bigr).(zg​f)(x)=j=1∑n​(f(gj​x)+f(gj−1​x)).

On L2(SU(d),μd)L^2(SU(d),\mu_d)L2(SU(d),μd​) it is bounded and self-adjoint, constants are eigenfunctions with eigenvalue 2n2n2n, and it preserves the space L02L^2_0L02​ of mean-zero functions. Writing λ1(zg)\lambda_1(z_g)λ1​(zg​) for the supremum of the spectrum of zgz_gzg​ on L02L^2_0L02​, one always has λ1≤2n\lambda_1 \le 2nλ1​≤2n, and zgz_gzg​ (or the tuple ggg) has a spectral gap when

λ1(zg)<2n.\lambda_1(z_g) < 2n .λ1​(zg​)<2n.

For SU(2)SU(2)SU(2), each UUU acts on the sphere S2S^2S2 by rotations, and zgz_gzg​ is the operator ϕU1+ϕU1−1+⋯+ϕUn+ϕUn−1\phi_{U_1} + \phi_{U_1}^{-1} + \dots + \phi_{U_n} + \phi_{U_n}^{-1}ϕU1​​+ϕU1​−1​+⋯+ϕUn​​+ϕUn​−1​ of the source.

Formalization targets

Goal: the spectral gap conjecture

For every n>2n > 2n>2, if U1,…,UnU_1,\dots,U_nU1​,…,Un​ are chosen independently and uniformly (Haar) at random in SU(2)SU(2)SU(2), then with probability 111

λ1(zU1,…,Un)<2n.\lambda_1\bigl(z_{U_1,\dots,U_n}\bigr) < 2n .λ1​(zU1​,…,Un​​)<2n.

Milestones from the literature

  1. Fisher's zero–one law (2006, Theorem 1.2): for n≥3n \ge 3n≥3, either almost every nnn-tuple has a spectral gap, or almost every nnn-tuple has none.
  2. Bourgain–Gamburd in SU(2)SU(2)SU(2) (2008): tuples with algebraic entries (up to simultaneous conjugation) that freely generate a free group of rank n≥2n\ge 2n≥2 have a spectral gap.
  3. Bourgain–Gamburd in SU(d)SU(d)SU(d) (2012, Theorem 1): for d≥2d \ge 2d≥2, tuples with algebraic entries generating a dense subgroup of SU(d)SU(d)SU(d) have a spectral gap.

By Fisher's law, the goal follows once a spectral gap is shown on a set of positive Haar measure.

Significance

A spectral gap for ggg means that random walks driven by g1±1,…,gn±1g_1^{\pm1},\dots,g_n^{\pm1}g1±1​,…,gn±1​ equidistribute in SU(2)SU(2)SU(2) (and orbits equidistribute on S2S^2S2) at an exponential rate, and that the action of the generated group on S2S^2S2 is strongly ergodic. In quantum computation it says that a universal single-qubit gate set is automatically efficiently universal. The conjecture asserts that this holds for a typical gate set, not just for the arithmetically special ones covered by Bourgain–Gamburd.

On the formal side, the milestones are proved theorems (Fisher; Bourgain–Gamburd) that have, to the knowledge of this proposal, no machine-checked proofs. Formalizing any of them requires substantial new libraries: Haar measure and harmonic analysis on SU(d)SU(d)SU(d), ergodicity of Aut(Fn)\mathrm{Aut}(F_n)Aut(Fn​) on Hom(Fn,SU(2))\mathrm{Hom}(F_n, SU(2))Hom(Fn​,SU(2)) (Goldman), and the arithmetic-combinatorial machinery of Bourgain–Gamburd. The goal itself is an open problem.

Difficulty

Spectral gap is not detected by density alone: every tuple generating a dense subgroup gives an ergodic action, but ergodicity only shows λ1\lambda_1λ1​ is not an eigenvalue, not that it is bounded away from 2n2n2n. Known proofs need either arithmetic structure (automorphic forms, or the algebraic entries used by Bourgain–Gamburd to rule out short relations that come too close to the identity) or rigidity (property (T)). A generic tuple has neither.

Formalization scope

  • SU(d)SU(d)SU(d) is Matrix.specialUnitaryGroup (Fin d) ℂ with the subspace topology and its Borel σ-algebra; it is shown to be a compact topological group, and haarSU d is the Haar measure normalized to total mass 111.
  • The Hecke operator acts on all functions f:SU(d)→Cf : SU(d) \to \mathbb Cf:SU(d)→C by the formula above.
  • "Spectral gap" is encoded through the quadratic form: there is ε>0\varepsilon > 0ε>0 such that Re⁡⟨zgf,f⟩≤(2n−ε) ∥f∥22\operatorname{Re}\langle z_g f, f\rangle \le (2n-\varepsilon)\,\|f\|_2^2Re⟨zg​f,f⟩≤(2n−ε)∥f∥22​ for every f∈L2f \in L^2f∈L2 with ∫f dμ=0\int f\,d\mu = 0∫fdμ=0. For a bounded self-adjoint operator this is exactly λ1<2n\lambda_1 < 2nλ1​<2n (one-sided gap, as in Fisher and Bourgain–Gamburd).
  • "Chosen uniformly at random" is the product Haar measure on SU(2)nSU(2)^nSU(2)n; "with probability 111" is an almost-everywhere statement.
  • The goal is stated on L2(SU(2))L^2(SU(2))L2(SU(2)), as in the source. The operator on L2(S2)L^2(S^2)L2(S2) is the restriction to a subrepresentation, so a gap on L02(SU(2))L^2_0(SU(2))L02​(SU(2)) implies a gap on L02(S2)L^2_0(S^2)L02​(S2). Fisher (2006, §1) remarks that the two versions of the conjecture are equivalent.
  • Trivializations are ruled out: for g1=⋯=gn=Ig_1=\dots=g_n=Ig1​=⋯=gn​=I the quadratic form equals 2n∥f∥22n\|f\|^22n∥f∥2, so no gap holds, and for n=0n=0n=0 the gap fails as well.

Useful reusable contributions include: basic harmonic analysis on compact groups (translation invariance in L2L^2L2, self-adjointness of zgz_gzg​), the Peter–Weyl decomposition of L2(SU(2))L^2(SU(2))L2(SU(2)), conjugation invariance of the gap, and monotonicity of the gap in the generating set.

Selected references

  • A. Lubotzky, R. Phillips, P. Sarnak, Hecke operators and distributing points on S2S^2S2. II, Comm. Pure Appl. Math. 40 (1987). https://doi.org/10.1002/cpa.3160400402
  • D. Fisher, Out(Fn)\mathrm{Out}(F_n)Out(Fn​) and the spectral gap conjecture, IMRN 2006. https://doi.org/10.1155/IMRN/2006/26028 (arXiv:math/0601050)
  • J. Bourgain, A. Gamburd, On the spectral gap for finitely-generated subgroups of SU(2)SU(2)SU(2), Invent. Math. 171 (2008). https://doi.org/10.1007/s00222-007-0072-z
  • J. Bourgain, A. Gamburd, A spectral gap theorem in SU(d)SU(d)SU(d), J. Eur. Math. Soc. 14 (2012). https://doi.org/10.4171/jems/337 (arXiv:1108.6264)
  • A. Sawicki, K. Karnas, Criteria for universality of quantum gates, Phys. Rev. A 95 (2017). https://doi.org/10.1103/PhysRevA.95.062303
  • Wikipedia, Spectral gap conjecture. https://en.wikipedia.org/wiki/Spectral_gap_conjecture
5 thms1 active userReviewed
Topology·Captain: Lucas

C^r Closing Lemma for DiffeomorphismsOpen Problem

Motivation

A central question in smooth dynamics is how much of the long-term behaviour of a system is captured by its periodic orbits. Every periodic point is nonwandering (each of its neighbourhoods returns to itself under some iterate), but a nonwandering point need not be periodic. The closing lemma asks whether this gap can be removed by an arbitrarily small perturbation: given a nonwandering point ppp of a diffeomorphism fff, is there a diffeomorphism ggg, as close to fff as desired, for which ppp is a periodic point?

The answer controls the generic picture of dynamics. Pugh's General Density Theorem, which rests on the closing lemma, says that for a generic C1C^1C1 diffeomorphism of a closed manifold the periodic points are dense in the nonwandering set. Results of this kind underlie the C1C^1C1-generic theory of dynamical systems (stability conjectures, generic properties of homoclinic classes). Whether the same holds for smoother perturbations is open; the question appears on the Open Problem Garden (closing lemma for diffeomorphisms, rated Outstanding) and is Problem 10 on Smale's 1998 list of mathematical problems for the next century.

Timeline.

  • 1967 — C. Pugh proves the closing lemma for C1C^1C1 perturbations of diffeomorphisms of a compact manifold, together with the General Density Theorem (Amer. J. Math. 89).
  • 1983 — C. Pugh and C. Robinson extend the C1C^1C1 closing lemma to flows and to conservative and Hamiltonian systems (Ergodic Theory Dynam. Systems 3).
  • 1987 — C. Gutierrez constructs examples on the torus showing that the local perturbation schemes used for C1C^1C1 cannot work in the C2C^2C2 topology (Ergodic Theory Dynam. Systems 7).
  • 1997 — S. Hayashi proves the C1C^1C1 connecting lemma (Ann. of Math. 145); the Open Problem Garden credits him with the C1C^1C1 case for flows.
  • 2016 — M. Asaoka and K. Irie prove a C∞C^\inftyC∞ closing lemma for Hamiltonian diffeomorphisms of closed surfaces (arXiv:1512.06336), a special conservative setting in which the closing is obtained near a given open set rather than at a prescribed point.

For general diffeomorphisms and every r>1r > 1r>1 the problem remains open.

Setting

Let MMM be a closed manifold: a compact Hausdorff smooth manifold without boundary, of dimension nnn. For r≥1r \ge 1r≥1, Diffr(M)\mathrm{Diff}^r(M)Diffr(M) is the set of CrC^rCr diffeomorphisms of MMM.

The CrC^rCr topology on Diffr(M)\mathrm{Diff}^r(M)Diffr(M) is defined through charts. For f∈Diffr(M)f \in \mathrm{Diff}^r(M)f∈Diffr(M), smooth charts (φ,U)(\varphi, U)(φ,U) and (ψ,V)(\psi, V)(ψ,V) of MMM, a compact set K⊆UK \subseteq UK⊆U with f(K)⊆Vf(K) \subseteq Vf(K)⊆V, and ε>0\varepsilon > 0ε>0, the basic set

Nr(f;φ,ψ,K,ε)={g:g(K)⊆V, ∥Dk(ψgφ−1)(x)−Dk(ψfφ−1)(x)∥<ε for all x∈φ(K), 0≤k≤r}\mathcal N^r(f;\varphi,\psi,K,\varepsilon) = \Big\{ g : g(K)\subseteq V,\ \big\|D^k(\psi g \varphi^{-1})(x) - D^k(\psi f \varphi^{-1})(x)\big\| < \varepsilon \text{ for all } x \in \varphi(K),\ 0 \le k \le r \Big\}Nr(f;φ,ψ,K,ε)={g:g(K)⊆V, ​Dk(ψgφ−1)(x)−Dk(ψfφ−1)(x)​<ε for all x∈φ(K), 0≤k≤r}

collects the diffeomorphisms whose local representative has all derivatives of order at most rrr uniformly within ε\varepsilonε of those of fff on φ(K)\varphi(K)φ(K). These sets generate the (weak) CrC^rCr topology; on a closed manifold it coincides with the Whitney CrC^rCr topology.

For a map f ⁣:M→Mf\colon M\to Mf:M→M, a point ppp is nonwandering if every neighbourhood UUU of ppp satisfies fk(U)∩U≠∅f^k(U)\cap U\neq\emptysetfk(U)∩U=∅ for some k≥1k\ge 1k≥1; the set of such points is the nonwandering set Ω(f)\Omega(f)Ω(f). A point ppp is periodic for ggg if gm(p)=pg^m(p)=pgm(p)=p for some m≥1m\ge1m≥1.

Formalization targets

Goal: the CrC^rCr closing lemma

For every closed manifold MMM, every r≥1r\ge 1r≥1, every f∈Diffr(M)f\in\mathrm{Diff}^r(M)f∈Diffr(M) and every p∈Ω(f)p\in\Omega(f)p∈Ω(f):

∀ V∋f a Cr-neighbourhood,∃ g∈V, ∃ m≥1: gm(p)=p.\forall\, \mathcal V \ni f \text{ a } C^r\text{-neighbourhood},\quad \exists\, g\in\mathcal V,\ \exists\, m\ge 1:\ g^m(p)=p .∀V∋f a Cr-neighbourhood,∃g∈V, ∃m≥1: gm(p)=p.

Milestones

  1. Compatibility of C1C^1C1 topologies. The C1C^1C1 topology defined above through charts coincides with the C1C^1C1 topology induced by the tangent maps g↦Tgg\mapsto Tgg↦Tg (compact-open topology on maps of the tangent bundle), used by the published statements of Pugh's theorems. Together with milestone 2 it yields the goal for r=1r = 1r=1.
  2. Pugh's C1C^1C1 closing lemma (1967) — the case r=1r=1r=1 (published platform statement).
  3. Pugh's General Density Theorem (1967) — for a residual set of g∈Diff1(M)g\in\mathrm{Diff}^1(M)g∈Diff1(M), Per(g)‾=Ω(g)\overline{\mathrm{Per}(g)}=\Omega(g)Per(g)​=Ω(g) (published platform statement).

Significance

A CrC^rCr closing lemma for r≥2r\ge2r≥2 would give, through the same Baire-category argument as in Pugh's work, a CrC^rCr General Density Theorem: CrC^rCr-generic diffeomorphisms would have periodic points dense in the nonwandering set. Much of the C1C^1C1-generic theory would then become available in the smoother topologies used in smooth ergodic theory, where distortion estimates need at least C1+αC^{1+\alpha}C1+α regularity.

On the formal side, the mission produces a reusable definition of the CrC^rCr topology on diffeomorphism groups, which Mathlib does not currently provide. The r=1r=1r=1 case is a theorem (Pugh 1967) without a machine-checked proof; formalizing it, and the compatibility of the two C1C^1C1 topologies, are concrete sub-goals. The case r≥2r\ge 2r≥2 is open, so a proof of the goal would be a new mathematical result.

Difficulty

A perturbation that makes an almost-returning orbit close up must move the orbit by a distance comparable to how close it comes back. With C1C^1C1 control, the perturbation can be spread over many iterates, and its C1C^1C1 size stays small because derivatives are only constrained to first order. For r≥2r\ge2r≥2, the CrC^rCr norm of a bump of displacement δ\deltaδ supported on a set of diameter ρ\rhoρ scales like δ/ρr\delta/\rho^rδ/ρr, and spreading the perturbation along the orbit no longer keeps it small. Gutierrez's examples show that the local perturbation schemes that work for r=1r=1r=1 do fail in the C2C^2C2 topology, so the natural first idea of copying Pugh's argument is ruled out.

Formalization scope

  • MMM is a type with a charted-space structure modelled on EuclideanSpace ℝ (Fin n) and a C∞C^\inftyC∞ manifold structure (IsManifold (𝓡 n) ∞ M), assumed compact and Hausdorff. Because the model space has no corners, MMM has no boundary.
  • Diffr(M)\mathrm{Diff}^r(M)Diffr(M) is Mathlib's Diffeomorph (𝓡 n) (𝓡 n) M M r, with rrr a natural number.
  • The CrC^rCr topology ClosingLemma.crTopology r is generated by Hirsch's basic sets, using charts of the maximal C∞C^\inftyC∞ atlas and Fréchet derivatives of order 0,…,r0,\dots,r0,…,r of the local representatives at points of φ(K)\varphi(K)φ(K). The goal quantifies over all neighbourhoods of fff for this topology.
  • The nonwandering set is the published PughClosingLemma.nonwanderingSet, shared with the existing statements of Pugh's theorems; periodic points are Mathlib's Function.periodicPts (period at least 111).
  • The hypothesis r≥1r\ge1r≥1 matches the source; r=1r=1r=1 is included in the goal, so the goal is a uniform statement for all finite r≥1r\ge1r≥1.

Infrastructure that would help: a usable API for the CrC^rCr topology (basic neighbourhoods, compatibility under change of charts, the Baire property of Diffr(M)\mathrm{Diff}^r(M)Diffr(M)), and local perturbation lemmas (bump-function perturbations of the identity supported in a chart, with CrC^rCr estimates). Contributions of these as separate lemmas are welcome.

Selected references

  • C. C. Pugh, An improved closing lemma and a general density theorem, Amer. J. Math. 89 (1967), 1010–1021. https://doi.org/10.2307/2373414
  • C. C. Pugh and C. Robinson, The C1C^1C1 closing lemma, including Hamiltonians, Ergodic Theory Dynam. Systems 3 (1983), 261–313.
  • C. Gutierrez, A counter-example to a C2C^2C2 closing lemma, Ergodic Theory Dynam. Systems 7 (1987), 509–530.
  • S. Hayashi, Connecting invariant manifolds and the solution of the C1C^1C1 stability and Ω\OmegaΩ-stability conjectures for flows, Ann. of Math. 145 (1997), 81–137.
  • M. Asaoka and K. Irie, A C∞C^\inftyC∞ closing lemma for Hamiltonian diffeomorphisms of closed surfaces, Geom. Funct. Anal. 26 (2016). https://arxiv.org/abs/1512.06336
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998), 7–15.
  • M. W. Hirsch, Differential Topology, Springer GTM 33, Ch. 2 (definition of the CrC^rCr topologies).
  • Open Problem Garden, Closing Lemma for Diffeomorphism (Dynamical Systems). https://www.openproblemgarden.org/op/closing_lemma_for_diffeomorphism_dynamical_systems
5 thms1 active userReviewed
ProbabilityStochastic Systems·Captain: mikedeng1

Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions 2: The Neuronal Network Converges in L² to Its McKean–Vlasov LimitResearch Paper

Motivation

Large networks of neurons are often modelled as systems of coupled stochastic differential equations: each neuron carries a low-dimensional state (a membrane potential and recovery variables, as in the FitzHugh–Nagumo model), receives synaptic input from the other neurons with a transmission delay, and is perturbed by noise. Because the number of neurons is large, one studies the mean-field limit: as the population grows, each neuron should evolve independently of every other fixed neuron, driven by its own noise and by an averaged population input. This asymptotic independence is called propagation of chaos, and the limiting single-neuron equation is a McKean–Vlasov equation.

Mehri, Scheutzow, Stannat and Zangeneh (arXiv:1805.01654v3, Ann. Appl. Probab. 2020, DOI 10.1214/19-AAP1499) prove propagation of chaos for a model combining features that earlier work treated separately: monotone (one-sided Lipschitz) local dynamics, general path-dependent delays, Lévy-type jump noise, spatial structure with several subpopulations, and a random environment (disorder). Earlier mean-field results for neuronal networks were obtained under global Lipschitz assumptions (Quiñinao and Touboul 2015; Touboul 2014, two papers), for locally Lipschitz coefficients (Baladron, Fasoli, Faugeras and Touboul 2012, with the clarification note of Bossy, Faugeras and Talay 2015) and for one-sided Lipschitz coefficients (Luçon and Stannat 2014; Touboul 2012); with jump noise, only under global Lipschitz or gradient-type local dynamics (Andreis, Dai Pra and Fischer 2018). This mission formalizes the paper's second main result, Theorem 1.8. The first mission of the series formalizes the well-posedness of the McKean–Vlasov equation (Theorem 1.5).

Setting

Neurons sit at positions rrr in a bounded set Γ⊂Rk\Gamma\subset\mathbb R^kΓ⊂Rk, partitioned into PPP measurable subpopulation regions Γα\Gamma_\alphaΓα​. The NNN-th network consists of a finite set AN⊂Γ\mathcal A_N\subset\GammaAN​⊂Γ of NNN positions, and neurons of subpopulation α\alphaα carry the weight 1/SAN,α1/\mathcal S_{\mathcal A_N,\alpha}1/SAN​,α​. The state Xtr,AN∈RdX^{r,\mathcal A_N}_t\in\mathbb R^dXtr,AN​​∈Rd of the neuron at rrr solves the network equation (1)

dXtr,AN=f dt+g dWtr+∫Uh N~r(dt,dξ)+∑α=1P1SAN,α∑r~∈AN∩Γα[θ dt+β dBtr,α+∫Uη N~r,α(dt,dξ)],dX^{r,\mathcal A_N}_t=f\,dt+g\,dW^r_t+\int_U h\,\tilde N^r(dt,d\xi)+\sum_{\alpha=1}^P\frac{1}{\mathcal S_{\mathcal A_N,\alpha}}\sum_{\tilde r\in\mathcal A_N\cap\Gamma_\alpha}\Big[\theta\,dt+\beta\,dB^{r,\alpha}_t+\int_U\eta\,\tilde N^{r,\alpha}(dt,d\xi)\Big],dXtr,AN​​=fdt+gdWtr​+∫U​hN~r(dt,dξ)+α=1∑P​SAN​,α​1​r~∈AN​∩Γα​∑​[θdt+βdBtr,α​+∫U​ηN~r,α(dt,dξ)],

where f,g,hf,g,hf,g,h are evaluated at (t,r,Xt−r,AN,ω′)(t,r,X^{r,\mathcal A_N}_{t-},\omega')(t,r,Xt−r,AN​​,ω′) and θ,β,η\theta,\beta,\etaθ,β,η at (t,r,r~,Xt−r,AN,X(t−τ)−:t−r~,AN,ω′)(t,r,\tilde r,X^{r,\mathcal A_N}_{t-},X^{\tilde r,\mathcal A_N}_{(t-\tau)^-:t^-},\omega')(t,r,r~,Xt−r,AN​​,X(t−τ)−:t−r~,AN​​,ω′), the last argument being the path of the presynaptic neuron over the delay window [t−τ,t][t-\tau,t][t−τ,t]. The noises WrW^rWr, Br,αB^{r,\alpha}Br,α are independent Brownian motions, N~r\tilde N^rN~r, N~r,α\tilde N^{r,\alpha}N~r,α independent compensated Poisson random measures with intensity dt⊗νdt\otimes\nudt⊗ν, and ω′\omega'ω′ is a random disorder with expectation E\mathcal EE. Each neuron starts from a path zrz^rzr on [−τ,0][-\tau,0][−τ,0].

Given a finite measure R\mathcal RR on Γ\GammaΓ with R(Γα)=1\mathcal R(\Gamma_\alpha)=1R(Γα​)=1, the McKean–Vlasov equation (6) describes a continuum of neurons XrX^rXr, r∈Γr\in\Gammar∈Γ, whose interaction is ∑α∫ΓαE~[θ(t,r,r′,Xt−r,X~(t−τ)−:t−r′,ω′)]R(dr′)\sum_\alpha\int_{\Gamma_\alpha}\tilde{\mathbb E}[\theta(t,r,r',X^r_{t-},\tilde X^{r'}_{(t-\tau)^-:t^-},\omega')]\mathcal R(dr')∑α​∫Γα​​E~[θ(t,r,r′,Xt−r​,X~(t−τ)−:t−r′​,ω′)]R(dr′), with X~\tilde XX~ an independent copy of XXX (and likewise for β\betaβ, η\etaη). The mean-field equation (5) for a neuron rrr of the network has the same form, with XrX^rXr replaced by a process Xˉr\bar X^rXˉr that starts from the same zrz^rzr and is driven by the same noises Wr,Br,α,N~r,N~r,αW^r, B^{r,\alpha}, \tilde N^r,\tilde N^{r,\alpha}Wr,Br,α,N~r,N~r,α as neuron rrr of the network, while the interaction is computed from the law of the solution of (6).

Formalization targets

Goal: Theorem 1.8

Under Hypothesis 1.6 and the chaotic initial condition (the zrz^rzr are independent, with zrz^rzr distributed as z^α\hat z^\alphaz^α for r∈Γαr\in\Gamma_\alphar∈Γα​),

lim⁡N→∞Esup⁡t∈[−τ,T], r∈ANE∣Xtr,AN−Xˉtr∣2=0.\lim_{N\to\infty}\mathcal E\sup_{t\in[-\tau,T],\,r\in\mathcal A_N}\mathbb E\big|X^{r,\mathcal A_N}_t-\bar X^r_t\big|^2=0 .N→∞lim​Et∈[−τ,T],r∈AN​sup​E​Xtr,AN​​−Xˉtr​​2=0.

The theorem asserts convergence without a rate, which is the stable form of the result.

Milestones

  1. Proposition 1.2: the network equation (1) is well posed.
  2. Lemma 1.7: positions in one cell Γαm,ε\Gamma^{m,\varepsilon}_\alphaΓαm,ε​ of the partition of Hypothesis 1.6 have solutions of (6) within C2(t,ω′)εC_2(t,\omega')\varepsilonC2​(t,ω′)ε in mean square.
  3. Display (18): the first moment estimate for Xr,AN−XˉrX^{r,\mathcal A_N}-\bar X^rXr,AN​−Xˉr, in terms of the fluctuation terms IαθI^\theta_\alphaIαθ​, IαβI^\beta_\alphaIαβ​, IαηI^\eta_\alphaIαη​.
  4. The bound (p. 20) of each III-term by 6(⋯ )C2(t,ω′)6(\cdots)C_2(t,\omega')6(⋯)C2​(t,ω′).
  5. The Gronwall bound (p. 21) with constant 363636, at a fixed disorder.
  6. The bound (p. 21) after integration over the disorder, with a constant C(T)C(T)C(T) independent of ε\varepsilonε and NNN.

The proof also uses Lemma 1.4 (the moment bound C1C_1C1​ for solutions of (6)), which is a milestone of the first mission of this series and is not restated here.

Significance

Theorem 1.8 justifies replacing a large, spatially structured network of delayed, jump-driven neurons by a single McKean–Vlasov equation indexed by position. The limit is the object on which neural field models and their bifurcation analysis are built; the theorem identifies the hypotheses on the spatial distribution of neurons (condition (10): the neuron counts per cell, normalized by the weights, converge to R\mathcal RR) under which that replacement is valid in a random environment.

The result is proved in the paper; no machine-checked proof exists. Formalizing it requires a coherent Lean layer for strong solutions of delay SDEs with jumps, mean-field interaction terms, Poisson random measures with product marks, and independence of countable families of drivers. The intermediate bounds of §3 are explicit and quantitative, and each is a self-contained target.

Difficulty

The interaction of the network is an empirical average over finitely many neurons, while the limit uses an expectation over a continuum of positions. The difference splits into three errors of different nature: a fluctuation term, whose control requires that the limit processes Xˉr~\bar X^{\tilde r}Xˉr~ of distinct neurons be independent (which holds only because each is driven by its own noise and starts from an independent initial condition); a spatial discretization error within each cell, which requires a quantitative regularity of the solution of (6) in the position variable; and a counting error between the neuron counts and the measure R\mathcal RR. A naive comparison of the network with (6) directly, without the coupled processes Xˉr\bar X^rXˉr of (5), gives no pathwise relation and does not work. The coefficients are only one-sided Lipschitz in the local variable, so moment bounds must come from monotonicity rather than from global Lipschitz estimates, and the disorder enters the constants through exponentials whose integrability is exactly assumption (H6).

Formalization scope

Positions are EuclideanSpace ℝ (Fin k), states EthierKurtz.SDEState d, and subpopulations Fin P (0-based). Neurons carry labels in ℕ with an injective position map, so AN\mathcal A_NAN​ is a finite set of labels and ⋃NAN\bigcup_N\mathcal A_N⋃N​AN​ is countable. Brownian integrals are the published EthierKurtz.HasBrownianItoIntegral per coordinate, compensated jump integrals the published JacodTodorov10.LLN.HasCompInt, and all Poisson measures of the network form one (𝓕_t)-Poisson random measure on a product mark space. Integrands are cut off after the horizon TTT. All expectations, suprema and the disorder expectation E\mathcal EE are taken in [0,∞][0,\infty][0,∞], so no statement can be satisfied by a junk value of a real integral or supremum; (H6) states the boundedness of its supremum explicitly. The copy X^\hat XX^ enters only through its law: the solution of (6) lives on its own probability space and the mean-field terms are expectations over it.

Conventions and corrections, all disclosed in the items: the theorem is stated for every family of solutions of (1), (5) and (6) (hypotheses), not for "the" solutions; (H1′) is printed with x−yx-yx−y and is read as x−x~x-\tilde xx−x~; IαηI^\eta_\alphaIαη​ carries the expectation of (17), which the display on p. 20 omits; the second Gronwall inequality on p. 21 (constant 144144144) drops a factor of C1C_1C1​ and is not posed; the coefficients' path argument carries the product σ-algebra; the filtration satisfies the usual conditions (Appendix A); the solution class of (6) is a bound for every time. The solution notions are not trivializing: every stochastic integral is tied to the given noise by a published predicate, the mean-field terms are computed from the solution of (6) itself, the limit processes share the network's noise and initial conditions, and the finite constant of the integrated bound is quantified before ε\varepsilonε and NNN.

Reusable beyond this mission: the strong-solution predicate for jump SDEs with delay, the noise predicates for countable families of drivers, and the network and mean-field interaction terms. Contributions toward a stochastic calculus for these predicates (Itô's formula for ∣X∣2|X|^2∣X∣2 with jumps, Gronwall arguments with left limits) are welcome.

Selected references

  • S. Mehri, M. Scheutzow, W. Stannat, B. Z. Zangeneh, Propagation of chaos for stochastic spatially structured neuronal networks with delay driven by jump diffusions, Ann. Appl. Probab. 30 (2020); arXiv:1805.01654v3. https://arxiv.org/abs/1805.01654
  • J. Baladron, D. Fasoli, O. Faugeras, J. Touboul, Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons, J. Math. Neurosci. 2:10 (2012). https://doi.org/10.1186/2190-8567-2-10
  • M. Bossy, O. Faugeras, D. Talay, Clarification and complement to "Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons", J. Math. Neurosci. 5:19 (2015). https://doi.org/10.1186/s13408-015-0031-8
  • J. Touboul, Propagation of chaos in neural fields, Ann. Appl. Probab. 24(3):1298–1328 (2014); arXiv:1108.2414. https://arxiv.org/abs/1108.2414
  • J. Touboul, Spatially extended networks with singular multi-scale connectivity patterns, J. Stat. Phys. 156(3):546–573 (2014).
  • C. Quiñinao, J. Touboul, Limits and dynamics of randomly connected neuronal networks, Acta Appl. Math. 136(1):167–192 (2015).
  • E. Luçon, W. Stannat, Mean field limit for disordered diffusions with singular interactions, Ann. Appl. Probab. 24(5):1946–1993 (2014).
  • J. Touboul, Limits and dynamics of stochastic neuronal networks with random heterogeneous delays, J. Stat. Phys. 149(4):569–597 (2012).
  • L. Andreis, P. Dai Pra, M. Fischer, McKean–Vlasov limit for interacting systems with simultaneous jumps, Stoch. Anal. Appl. (2018).
15 thms1 active userReviewed
Control TheoryGraph TheoryLinear algebra·Captain: mikedeng1

Sub/Super-Stochastic Matrix with Applications to Bipartite Tracking Control over Signed Networks 3: ψ < 1/(τd_M), Structural Balance and Leader Reachability Give Asynchronous Bipartite TrackingResearch Paper

Motivation

Networks of agents that interact both cooperatively and competitively are modelled by signed graphs: a positive edge weight means that one agent moves towards another, a negative weight means that it moves towards the other's opposite. Since Altafini's work on consensus over antagonistic networks (IEEE TAC 2013), the standard target on such networks has been bipartite consensus or bipartite tracking: the agents split into two camps that converge to values of equal size and opposite sign. With a leader, the camp containing the leader tracks the leader's state and the other camp tracks its negative.

Most analyses assume that all agents update at the same instants. In practice agents sample and communicate on their own clocks. Shi, Zheng, Shao and Cheng (arXiv:2004.01867v2, SIAM J. Control Optim. 2021) handle this asynchronous setting with a matrix tool: products of sub-stochastic matrices (nonnegative, row sums at most one) whose row-sum deficits propagate along the communication graph. This mission formalizes their first application, bipartite tracking of first-order agents with a static leader (§3).

Setting

There is one leader v0v_0v0​ and nnn followers v1,…,vnv_1,\dots,v_nv1​,…,vn​. Follower weights form a matrix A=[aij]∈Rn×n\mathcal A=[a_{ij}]\in\mathbb R^{n\times n}A=[aij​]∈Rn×n: the edge (vj,vi)(v_j,v_i)(vj​,vi​) exists iff aij≠0a_{ij}\neq 0aij​=0, cooperative if aij>0a_{ij}>0aij​>0, competitive if aij<0a_{ij}<0aij​<0. The number ai0a_{i0}ai0​ is the weight of the leader edge (v0,vi)(v_0,v_i)(v0​,vi​), which exists iff ai0≠0a_{i0}\ne 0ai0​=0. The digraph G~\tilde{\mathcal G}G~​ consists of the followers' digraph, the leader and the leader edges.

  • C1 (structural balance). The agents split as V1∪V2\mathcal V_1\cup\mathcal V_2V1​∪V2​ with v0∈V1v_0\in\mathcal V_1v0​∈V1​, every weight inside a set is ≥0\ge 0≥0 and every weight between the sets is ≤0\le 0≤0.
  • C2 (leader reachability). Every follower is reached from v0v_0v0​ by a directed path in G~\tilde{\mathcal G}G~​.

Time is discrete with step size τ>0\tau>0τ>0. Follower viv_ivi​ communicates only at its own instants s0iτ<s1iτ<⋯s^i_0\tau<s^i_1\tau<\cdotss0i​τ<s1i​τ<⋯ with s0i=0s^i_0=0s0i​=0 and

sk+1i−ski≤h(2.10)s^i_{k+1}-s^i_k\le h\qquad(2.10)sk+1i​−ski​≤h(2.10)

for a constant h∈Z+h\in\mathbb Z_+h∈Z+​. Positions xi(k)∈Rpx_i(k)\in\mathbb R^pxi​(k)∈Rp evolve by x0(k+1)=x0(k)x_0(k+1)=x_0(k)x0​(k+1)=x0​(k) and xi(k+1)=xi(k)+τui(k)x_i(k+1)=x_i(k)+\tau u_i(k)xi​(k+1)=xi​(k)+τui​(k), with the asynchronous protocol

ui(k)=ψ∑vj∈Ni∣aij∣[sgn⁡(aij)xj(k)−xi(k)]+ψ∣ai0∣[sgn⁡(ai0)x0(k)−xi(k)]u_i(k)=\psi\sum_{v_j\in\mathcal N_i}|a_{ij}|\big[\operatorname{sgn}(a_{ij})x_j(k)-x_i(k)\big]+\psi|a_{i0}|\big[\operatorname{sgn}(a_{i0})x_0(k)-x_i(k)\big]ui​(k)=ψvj​∈Ni​∑​∣aij​∣[sgn(aij​)xj​(k)−xi​(k)]+ψ∣ai0​∣[sgn(ai0​)x0​(k)−xi​(k)]

at the instants of viv_ivi​, and ui(k)=0u_i(k)=0ui​(k)=0 otherwise. Here ψ>0\psi>0ψ>0 is a gain. Bipartite tracking (Definition 3.1) means ∥xi(k)−x0(k)∥→0\|x_i(k)-x_0(k)\|\to 0∥xi​(k)−x0​(k)∥→0 for vi∈V1v_i\in\mathcal V_1vi​∈V1​ and ∥xi(k)+x0(k)∥→0\|x_i(k)+x_0(k)\|\to 0∥xi​(k)+x0​(k)∥→0 for vi∈V2v_i\in\mathcal V_2vi​∈V2​. With dM=max⁡i(∑vj∈Ni∣aij∣+∣ai0∣)d_M=\max_i\big(\sum_{v_j\in\mathcal N_i}|a_{ij}|+|a_{i0}|\big)dM​=maxi​(∑vj​∈Ni​​∣aij​∣+∣ai0​∣), the gain condition is

ψ<1τdM.(3.7)\psi<\frac{1}{\tau d_M}.\qquad(3.7)ψ<τdM​1​.(3.7)

In the error coordinates ei=xi−x0e_i=x_i-x_0ei​=xi​−x0​ on V1\mathcal V_1V1​ and ei=−xi−x0e_i=-x_i-x_0ei​=−xi​−x0​ on V2\mathcal V_2V2​, the closed loop is e(k+1)=(M(k)⊗Ip)e(k)e(k+1)=(M(k)\otimes I_p)e(k)e(k+1)=(M(k)⊗Ip​)e(k) with M(k)=In−τψD(k)−τψB(k)+τψ∣A(k)∣M(k)=I_n-\tau\psi\mathcal D(k)-\tau\psi\mathcal B(k)+\tau\psi|\mathcal A(k)|M(k)=In​−τψD(k)−τψB(k)+τψ∣A(k)∣, where only the rows of followers active at time kτk\taukτ differ from the identity.

Formalization targets

Goal: Theorem 3.3, sufficiency

ψ<1τdM,  C1,  C2 ⟹ lim⁡k→∞∥xi(k)−x0(k)∥=0 (vi∈V1),lim⁡k→∞∥xi(k)+x0(k)∥=0 (vi∈V2),\psi<\frac1{\tau d_M},\ \ \mathrm{C1},\ \ \mathrm{C2}\ \Longrightarrow\ \lim_{k\to\infty}\|x_i(k)-x_0(k)\|=0\ (v_i\in\mathcal V_1),\quad \lim_{k\to\infty}\|x_i(k)+x_0(k)\|=0\ (v_i\in\mathcal V_2),ψ<τdM​1​,  C1,  C2 ⟹ k→∞lim​∥xi​(k)−x0​(k)∥=0 (vi​∈V1​),k→∞lim​∥xi​(k)+x0​(k)∥=0 (vi​∈V2​),

for every choice of instants satisfying (2.10) and every initial state.

Milestones

  1. Theorem 2.4 1): a product Fq⋯F1F_q\cdots F_1Fq​⋯F1​ of sub-stochastic matrices is sub-stochastic.
  2. Theorem 2.4 2): with positive diagonals, if every row i2i_2i2​ is fed through [Fs2]i2i1>0[F_{s_2}]_{i_2i_1}>0[Fs2​​]i2​i1​​>0 by a row i1i_1i1​ with Λi1[Fs1]<1\Lambda_{i_1}[F_{s_1}]<1Λi1​​[Fs1​​]<1, s1<s2s_1<s_2s1​<s2​, then ∥∏s=1qFs∥∞<1\|\prod_{s=1}^qF_s\|_\infty<1∥∏s=1q​Fs​∥∞​<1 and ρ(∏s=1qFs)<1\rho(\prod_{s=1}^qF_s)<1ρ(∏s=1q​Fs​)<1.
  3. The matrices M(k)M(k)M(k) (p. 15): under (3.7) they are sub-stochastic with positive diagonals, and Λi[M(k)]<1\Lambda_i[M(k)]<1Λi​[M(k)]<1 exactly when viv_ivi​ hears the leader at kτk\taukτ.
  4. Error system (3.6): under C1, ei(k+1)=∑j[M(k)]ijej(k)e_i(k+1)=\sum_j[M(k)]_{ij}e_j(k)ei​(k+1)=∑j​[M(k)]ij​ej​(k).
  5. Lemma 3.2: under (3.7), C1 and C2, ∥∏s=kk+Ph−1M(s)∥∞<1\big\|\prod_{s=k}^{k+Ph-1}M(s)\big\|_\infty<1​∏s=kk+Ph−1​M(s)​∞​<1 for every kkk, where P=max⁡id(v0,vi)P=\max_i d(v_0,v_i)P=maxi​d(v0​,vi​) is the largest directed distance from the leader.

Significance

The theorem says that asynchrony costs nothing qualitatively: as long as every follower communicates at least once every hhh steps and the gain respects (3.7), the network reaches bipartite tracking under the same topological conditions C1 and C2 as in the synchronous case. No common clock, dwell-time condition or joint connectivity of the switching graphs is required. The same product argument is reused in the rest of the paper for second-order and general linear agents, delays and switching topologies, so the milestones here are the base case of that series.

The result is proved in the paper; it has not been formalized. Formalizing it produces a checked theory of products of sub-stochastic matrices with row-sum deficits (Theorem 2.4), which applies to positive switched systems in general, and a reusable encoding of signed digraphs with a leader, structural balance and asynchronous protocols.

Difficulty

Each single matrix M(k)M(k)M(k) is only marginally stable: its rows of followers that do not hear the leader at time kτk\taukτ sum to exactly one, so no single step contracts, and the spectral radius of an individual M(k)M(k)M(k) may equal one. Contraction appears only in products, and only once a deficit created at a leader edge has had time to travel along the paths of C2, one edge per window of hhh steps; this requires that deficits never disappear again, which is where positive diagonals (from (3.7)) enter. The passage from "every window product has ∥⋅∥∞<1\|\cdot\|_\infty<1∥⋅∥∞​<1" to convergence also needs a uniform bound below one over all windows; the paper's (3.14) uses it without comment. The bound holds because M(k)M(k)M(k) depends on kkk only through the set of active followers, so the window products range over a finite set.

Formalization scope

Followers are Fin n (0-based) and the leader is not an index; aija_{ij}aij​ is a i j and ai0a_{i0}ai0​ is b i. Positions lie in EuclideanSpace ℝ (Fin p); the paper's norm is unspecified and all norms on Rp\mathbb R^pRp give the same limits. Eigenvalues are complex: ρ(F)<1\rho(F)<1ρ(F)<1 means every element of spectrum ℂ of the complexified matrix has modulus <1<1<1. ∥F∥∞\|F\|_\infty∥F∥∞​ is the largest absolute row sum. Products multiply later factors on the left. sgn⁡\operatorname{sgn}sgn is Real.sign. The maxima dMd_MdM​ and PPP are given as values with IsGreatest hypotheses over exactly the printed sets, and (3.7) is kept as printed. C1 is stated for the partition V1={v0}∪V1\mathcal V_1=\{v_0\}\cup V_1V1​={v0​}∪V1​, V2=\mathcal V_2=V2​= the remaining followers; fixing the leader in V1\mathcal V_1V1​ is the paper's "with no loss of generality" convention. Definition 3.1 is stated for that same partition.

Only the "if" half of Theorem 3.3 is a target. Definition 3.1 presupposes the partition of C1, so necessity of C1 has no formal meaning, and the printed necessity argument is an informal case discussion. Theorem 2.4 2) is stated with one (i1,s1,s2)(i_1,s_1,s_2)(i1​,s1​,s2​) per row i2i_2i2​, as its proof and the example on p. 8 use it; this is implied by the literal reading.

Three formalizations would trivialize the goal and are ruled out: a protocol in which every follower updates at every step (the synchronous special case, which drops the asynchronous instants); dropping the sign conditions of C1, or leaving the leader's side free, under which the followers of V2\mathcal V_2V2​ need not approach −x0-x_0−x0​; and a goal stated about the error system (3.6) instead of the agents' positions xix_ixi​.

The development needs finite matrix products, the ∞-norm bound on eigenvalues (Gershgorin), and elementary walk reachability in digraphs. All of these exist in Mathlib in some form. Contributions are welcome on every milestone. The product theorem 2.4 does not depend on the network model and is reusable for positive switched systems.

Selected references

  • L. Shi, W. X. Zheng, J. Shao, Y. Cheng, Sub/super-stochastic matrix with applications to bipartite tracking control over signed networks, arXiv:2004.01867v2, 2020; SIAM J. Control Optim. 59 (2021). https://arxiv.org/abs/2004.01867, https://doi.org/10.1137/19M1239982
  • C. Altafini, Consensus problems on networks with antagonistic interactions, IEEE Trans. Automat. Control 58(4), 2013. https://doi.org/10.1109/TAC.2012.2224251
9 thms1 active userReviewed
ProbabilityStochastic Systems·Captain: mikedeng1

Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions 1: The Spatially Structured McKean–Vlasov Delay Equation with Jumps Is Well-PosedResearch Paper

Motivation

Networks of conductance-based neurons, such as FitzHugh–Nagumo networks, are modelled by systems of stochastic differential equations in which each neuron interacts with the others through synapses, and the signal from one neuron reaches another only after a transmission delay. Biological neurons sit at positions in space, belong to a few distinct subpopulations, are driven by Brownian and Poisson (jump) noise, and vary from one to another; the last feature is modelled by a random disorder parameter. When the number of neurons tends to infinity, the state of a typical neuron is expected to follow a McKean–Vlasov equation: an SDE whose coefficients depend on the law of its own solution. S. Mehri, M. Scheutzow, W. Stannat and B. Z. Zangeneh (arXiv:1805.01654; Ann. Appl. Probab. 30 (2020), DOI 10.1214/19-AAP1499) prove that this limit equation is well-posed, with coefficients that are only monotone (one-sided Lipschitz), a general delay, jump noise, spatial structure and disorder all at once, and then prove propagation of chaos towards it.

Earlier work, as surveyed on p. 3 of the paper, covered parts of this setting: global Lipschitz coefficients (Quiñinao and Touboul 2015, and the paper's references [10, 11]), locally Lipschitz coefficients (Baladron, Fasoli, Faugeras and Touboul 2012, with the clarification of Bossy, Faugeras and Talay 2015 on the localization by hitting times; the same issue affects Touboul 2012), one-sided Lipschitz coefficients with diffusive noise (Luçon and Stannat 2014), and Lévy noise under global Lipschitz assumptions or gradient-type local dynamics (Andreis, Dai Pra and Fischer 2018). The paper constructs the solution by an Euler approximation, which, by the authors' account, had not been applied to McKean–Vlasov equations before.

Setting

Fix dimensions ddd (state), mmm, nnn (noise), kkk (space), a delay τ>0\tau > 0τ>0 and P≥1P \ge 1P≥1 subpopulations, located at pairwise disjoint measurable regions Γ1,…,ΓP⊂Rk\Gamma_1,\dots,\Gamma_P \subset \mathbb R^kΓ1​,…,ΓP​⊂Rk whose union Γ\GammaΓ is bounded. A finite Borel measure R\mathcal RR on Γ\GammaΓ with R(Γα)=1\mathcal R(\Gamma_\alpha) = 1R(Γα​)=1 describes the spatial distribution of neurons. A disorder probability space (Ω′,F′,P′)(\Omega',\mathcal F',\mathbb P')(Ω′,F′,P′) is fixed. On a filtered probability space (Ω,F,(Ft),P)(\Omega,\mathcal F,(\mathcal F_t),\mathbb P)(Ω,F,(Ft​),P) there are an mmm-dimensional Brownian motion WWW, nnn-dimensional Brownian motions B1,…,BPB^1,\dots,B^PB1,…,BP, Poisson random measures N,N1,…,NPN, N^1, \dots, N^PN,N1,…,NP on [0,∞)×U[0,\infty)\times U[0,∞)×U with intensity dt⊗νdt\otimes\nudt⊗ν (ν\nuν σ-finite; N~=N−dt⊗ν\tilde N = N - dt\otimes\nuN~=N−dt⊗ν), all independent, and initial paths z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd))\hat z^\zeta \in L^2(\Omega;\text{Càdlàg}([-\tau,0];\mathbb R^d))z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd)).

For a path yyy, write y(t−τ)−:t−y_{(t-\tau)^-:t^-}y(t−τ)−:t−​ for the segment u↦y(t+u)−u\mapsto y_{(t+u)^-}u↦y(t+u)−​, u∈[−τ,0]u\in[-\tau,0]u∈[−τ,0]. The equation is

dXtr=f(t,r,Xt−r,ω′)dt+g(⋅)dWt+∫Uh(⋅,ξ)N~(dt,dξ)+∑α=1P∫ΓαE~[θ(t,r,r′,Xt−r,X~(t−τ)−:t−r′,ω′)]R(dr′)dtdX^r_t = f(t,r,X^r_{t-},\omega')dt + g(\cdot)dW_t + \int_U h(\cdot,\xi)\tilde N(dt,d\xi) + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}\big[\theta(t,r,r',X^r_{t-},\tilde X^{r'}_{(t-\tau)^-:t^-},\omega')\big]\mathcal R(dr')dtdXtr​=f(t,r,Xt−r​,ω′)dt+g(⋅)dWt​+∫U​h(⋅,ξ)N~(dt,dξ)+α=1∑P​∫Γα​​E~[θ(t,r,r′,Xt−r​,X~(t−τ)−:t−r′​,ω′)]R(dr′)dt +∑α=1P∫ΓαE~[β(⋯ )]R(dr′)dBtα+∑α=1P∫Γα∫UE~[η(⋯ ,ξ)]R(dr′)N~α(dt,dξ),Xtr=z^tζ (r∈Γζ, t∈[−τ,0]),(6)+ \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}[\beta(\cdots)]\mathcal R(dr')dB^\alpha_t + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\int_U\tilde{\mathbb E}[\eta(\cdots,\xi)]\mathcal R(dr')\tilde N^\alpha(dt,d\xi),\qquad X^r_t = \hat z^\zeta_t\ (r\in\Gamma_\zeta,\ t\in[-\tau,0]), \tag{6}+α=1∑P​∫Γα​​E~[β(⋯)]R(dr′)dBtα​+α=1∑P​∫Γα​​∫U​E~[η(⋯,ξ)]R(dr′)N~α(dt,dξ),Xtr​=z^tζ​ (r∈Γζ​, t∈[−τ,0]),(6)

where X~\tilde XX~ is an independent copy of the solution XXX and E~\tilde{\mathbb E}E~ its expectation. The local dynamics f,g,hf, g, hf,g,h satisfy the monotonicity and growth conditions (H1)–(H3) of Hypothesis 1.1 with locally integrable random rates Lt(ω′)L_t(\omega')Lt​(ω′), Kt(ω′)K_t(\omega')Kt​(ω′), K~t(R,ω′)\tilde K_t(R,\omega')K~t​(R,ω′); the synaptic coefficients θ,β,η\theta, \beta, \etaθ,β,η are Lipschitz (H4) and of linear growth (H5) in (x,y)(x, y)(x,y), with rates Lˉt(ω′)\bar L_t(\omega')Lˉt​(ω′), Kˉt(ω′)\bar K_t(\omega')Kˉt​(ω′), the path variable measured through a probability measure λ\lambdaλ on [−τ,0][-\tau,0][−τ,0]. In Lean, the model is the definition module NeuroMV.WellPosed.Setting: Space, Coeffs, Hyp1_1, Noise/IsNoise, IsStrongSol6, InClass and the constant C1 of (7).

Formalization targets

Goal: Theorem 1.5 (p. 7)

For every T>0T>0T>0 there is a process Xtr(ω;ω′)X^r_t(\omega;\omega')Xtr​(ω;ω′), measurable in (r,ω′,ω)(r,\omega',\omega)(r,ω′,ω), such that for P′\mathbb P'P′-almost every ω′\omega'ω′, X(ω′)X(\omega')X(ω′) is a strong solution of (6) on [−τ,T][-\tau,T][−τ,T],

X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),X(\omega') \in L^\infty\big([-\tau,T],dt;L^2(\Omega\times\Gamma,\mathbb P\otimes\mathcal R;\mathbb R^d)\big),X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),

and every other strong solution YYY in that class satisfies ∫ΓE∣Xtr−Ytr∣2R(dr)=0\int_\Gamma\mathbb E|X^r_t - Y^r_t|^2\mathcal R(dr) = 0∫Γ​E∣Xtr​−Ytr​∣2R(dr)=0 for all t∈[−τ,T]t\in[-\tau,T]t∈[−τ,T].

Milestones

  1. Theorem A.2 (p. 23): well-posedness of the general path-dependent delay SDE (20) with jumps under the monotonicity Hypothesis A.1, joint measurability in (t,ω,ω′)(t,\omega,\omega')(t,ω,ω′), the moment bound (22), and convergence of the Euler approximation (21).
  2. The scheme (11) exists and is measurable (p. 9), and satisfies the uniform bound (12): sup⁡t∈[−τ,T]E∣Xtn,r∣2≤C1(T,ω′)\sup_{t\in[-\tau,T]}\mathbb E|X^{n,r}_t|^2 \le C_1(T,\omega')supt∈[−τ,T]​E∣Xtn,r​∣2≤C1​(T,ω′).
  3. Claims (iv) and (v) (p. 10): the schemes are Cauchy in probability uniformly on [0,T][0,T][0,T], and their limit solves (6).
  4. Lemma 1.4 (p. 6): every solution in the class satisfies sup⁡s∈[−τ,t]E∣Xsr∣2≤C1(t,ω′)\sup_{s\in[-\tau,t]}\mathbb E|X^r_s|^2 \le C_1(t,\omega')sups∈[−τ,t]​E∣Xsr​∣2≤C1​(t,ω′).
  5. Uniqueness (pp. 16–17): two solutions in the class agree in L2(Ω×Γ)L^2(\Omega\times\Gamma)L2(Ω×Γ) at every time.

Significance

Theorem 1.5 makes the infinite-population limit of the network well defined; the second main result of the paper, Theorem 1.8, proves that the network converges to it in L2L^2L2. The theorem applies to coefficients that are only monotone in the state, which covers the cubic nonlinearity of FitzHugh–Nagumo neurons (Example 1.3), and to synaptic weights of conductance type driven by jump noise. Theorem A.2, proved in the appendix, is a well-posedness and Euler-convergence result for monotone stochastic delay equations with jumps and random coefficients, stated by the authors as new in this generality; it is reusable beyond this paper.

The results are proved in the paper; none of them has a machine-checked proof. The mission produces a Lean statement of the limit equation with the published Brownian and compensated Poisson integral relations, and invites formal proofs of the scheme estimates, the Cauchy property, the identification of the limit, the moment bound and uniqueness.

Difficulty

Under monotone coefficients there is no global contraction, so the Picard iteration that proves McKean–Vlasov well-posedness under Lipschitz assumptions does not apply. Localization by stopping times, the standard replacement for SDEs with monotone coefficients, does not localize the mean-field terms, which depend on the law of the solution at all positions; mishandling this step is the gap that Bossy, Faugeras and Talay pointed out in earlier work, and the acknowledgements (p. 30) record that the first version of this paper contained an unjustified application of the moment estimate of Lemma 1.4. A priori bounds must therefore be uniform in the approximation, and the limit of the mean-field stochastic integrals must be identified, with jumps and delay present. A second difficulty is measurability: the mean-field integrals require the solution to be measurable in the position r′r'r′, and the theorem asserts measurability in (r,ω′)(r,\omega')(r,ω′).

Formalization scope

  • Representation. Positions are EuclideanSpace ℝ (Fin k), states EthierKurtz.SDEState d, matrices Matrix (Fin d) (Fin m) ℝ with the Hilbert–Schmidt norm; subpopulations are Fin P, 0-based. Processes are indexed by ℝ on [−τ,T][-\tau,T][−τ,T]; drivers by ℝ≥0. Path segments are functions ℝ → ℝ^d read on [−τ,0][-\tau,0][−τ,0] with the product (cylinder) σ-algebra; the paper's sup-norm Borel σ-algebra is larger, so joint measurability of the coefficients for the cylinder σ-algebra is a mild added requirement.
  • Noise and integrals. Brownian integrals are the published EthierKurtz.HasBrownianItoIntegral, compensated jump integrals the published JacodTodorov10.LLN.HasCompInt, coordinatewise, with integrands cut off after TTT. All Poisson measures are one JacodTodorov10.LLN.IsFPoisson measure on a product mark space, equivalent to independent measures N,NαN, N^\alphaN,Nα. Independence of the initial data from the drivers is encoded by F0\mathcal F_0F0​-measurability.
  • Mean field. The copy X~\tilde XX~ enters only through its law, so E~\tilde{\mathbb E}E~ is an expectation over XXX itself; the mean-field integrands are required to be integrable on Γα×Ω\Gamma_\alpha\times\OmegaΓα​×Ω. Expectations and suprema are in [0,∞][0,\infty][0,∞]; Bochner integrals carry integrability clauses.
  • Hypotheses. Hypothesis 1.1 (H1)–(H5) and the regularity of p. 2; (H6) is omitted from every item, because it involves the network data of (1) only and the proof never uses it. The class L∞L^\inftyL∞–L2L^2L2 is a bound for every ttt rather than a.e. ttt.
  • Every position. The goal requires the integral identity at every r∈Γr\in\Gammar∈Γ, as (6) is posed; §2 proves it for R×P′\mathcal R\times\mathbb P'R×P′-a.e. (r,ω′)(r,\omega')(r,ω′) (p. 16), and on the remaining null set of positions (6) is an ordinary delay SDE solved by Theorem A.2 — a step the paper leaves implicit. Claim (v) keeps the R\mathcal RR-a.e. reading.
  • No trivialization. The stochastic integrals are the published relations tied to WWW, BαB^\alphaBα, NNN, NαN^\alphaNα, not free processes; the mean-field terms are computed from the solution's own segments; the solution class is non-empty for zero coefficients (a sorry-free check accompanies the mission); and the scheme and limit are the paper's, not new processes with their own noise.
  • Not stated. Claims (i)–(iii) of §2 (the remainder estimate and the a priori bounds before the stopping time) are not separate items.
  • Welcome contributions. Itô's formula for jump diffusions in this encoding, Gronwall-type lemmas in [0,∞][0,\infty][0,∞], stability of the published integral relations under convergence in probability, and the monotone delay SDE theory of Appendix A are all reusable beyond this mission.

Selected references

  • S. Mehri, M. Scheutzow, W. Stannat, B. Z. Zangeneh, Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions, arXiv:1805.01654v3, 2019; Ann. Appl. Probab. 30, 2020. https://arxiv.org/abs/1805.01654, https://doi.org/10.1214/19-AAP1499
  • J. Baladron, D. Fasoli, O. Faugeras, J. Touboul, Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons, J. Math. Neurosci. 2:10, 2012.
  • M. Bossy, O. Faugeras, D. Talay, Clarification and complement to "Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons", J. Math. Neurosci. 5:19, 2015.
  • E. Luçon, W. Stannat, Mean field limit for disordered diffusions with singular interactions, Ann. Appl. Probab. 24(5):1946–1993, 2014.
  • C. Quiñinao, J. Touboul, Limits and dynamics of randomly connected neuronal networks, Acta Appl. Math. 136(1):167–192, 2015.
  • J. Touboul, Limits and dynamics of stochastic neuronal networks with random heterogeneous delays, J. Stat. Phys. 149(4):569–597, 2012.
  • L. Andreis, P. Dai Pra, M. Fischer, McKean–Vlasov limit for interacting systems with simultaneous jumps, Stoch. Anal. Appl., 2018.
  • W. Liu, M. Röckner, Stochastic Partial Differential Equations: An Introduction, Universitext, Springer, 2015.

The bibliographic data of the last seven entries are taken from the reference list of the paper (pp. 30–31).

17 thms1 active userReviewed
AnalysisStochastic Systems·Captain: mikedeng1

On Well-Posedness of Forward–Backward SDEs—A Unified Approach 3: With Constant Coefficients, σ₃ ≠ 0, σ₃h ≠ 1 the Dominating ODE Keeps y and (1 − σ₃y)⁻¹ Bounded for Every T Iff One of Four Cases HoldsResearch Paper

Motivation

A forward–backward stochastic differential equation (FBSDE) couples a forward diffusion XXX with a backward equation for a pair (Y,Z)(Y,Z)(Y,Z) whose terminal value depends on XTX_TXT​. Such systems arise from the stochastic maximum principle, from option pricing with large investors, and from stochastic differential games. Whether an FBSDE with Lipschitz coefficients has a unique solution on an arbitrary horizon [0,T][0,T][0,T] is a classical question: small-time solvability is easy, but global solvability can fail even for linear equations.

J. Ma, Z. Wu, D. Zhang and J. Zhang, On well-posedness of forward–backward SDEs—a unified approach (arXiv:1110.4658v2, Ann. Appl. Probab. 25 (2015)), reduce well-posedness to the existence of bounded solutions of two deterministic dominating ordinary differential equations, obtained from the difference quotients of the coefficients. For linear FBSDEs with constant coefficients the two dominating ODEs coincide, and the authors give sharp criteria for global solvability. This mission formalizes the criterion in the case σ3≠0\sigma_3\neq0σ3​=0, where the dominating ODE has a rational right-hand side with a pole.

Earlier global results for coupled FBSDEs rested on the four-step scheme (Ma–Protter–Yong 1994) or on monotonicity conditions (Hu–Peng 1995); §7.4 of the paper compares the dominating-ODE approach with these methods.

Setting

The linear FBSDE (4.1) with constant coefficients is determined by nine reals b1,b2,b3,σ1,σ2,σ3,f1,f2,f3b_1,b_2,b_3,\sigma_1,\sigma_2,\sigma_3,f_1,f_2,f_3b1​,b2​,b3​,σ1​,σ2​,σ3​,f1​,f2​,f3​ and a terminal slope hhh. Its dominating function is (3.9),

F(y)=f1+f2y+y(b1+b2y)+(f3+b3y) y (σ1+σ2y)1−σ3y,F(y)=f_1+f_2y+y(b_1+b_2y)+\frac{(f_3+b_3y)\,y\,(\sigma_1+\sigma_2y)}{1-\sigma_3y},F(y)=f1​+f2​y+y(b1​+b2​y)+1−σ3​y(f3​+b3​y)y(σ1​+σ2​y)​,

defined for y≠1/σ3y\neq1/\sigma_3y=1/σ3​. When σ3≠0\sigma_3\neq0σ3​=0 it can be rewritten as (5.8),

F(y)=α01/σ3−y+α1+α2y+α3y2,α3=b2−b3σ2σ3,F(y)=\frac{\alpha_0}{1/\sigma_3-y}+\alpha_1+\alpha_2y+\alpha_3y^2,\qquad \alpha_3=b_2-\frac{b_3\sigma_2}{\sigma_3},F(y)=1/σ3​−yα0​​+α1​+α2​y+α3​y2,α3​=b2​−σ3​b3​σ2​​,

for constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​. The dominating ODE (5.3) is the backward integral equation

yt=h+∫tTF(ys) ds,t∈[0,T].y_t=h+\int_t^TF(y_s)\,ds,\qquad t\in[0,T].yt​=h+∫tT​F(ys​)ds,t∈[0,T].

The paper needs a solution satisfying (5.9): both yyy and (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1 are bounded on [0,T][0,T][0,T]. Since yT=hy_T=hyT​=h, this forces σ3h≠1\sigma_3h\neq1σ3​h=1 (Remark 5.5).

The comparison tool is Lemma 5.1. For measurable F0,F1,F2F^0,F^1,F^2F0,F1,F2 it gives a unique solution of yt0=h0+∫tTF0(s,ys0) dsy^0_t=h^0+\int_t^TF^0(s,y^0_s)\,dsyt0​=h0+∫tT​F0(s,ys0​)ds lying between a sub-solution y1y^1y1 and a super-solution y2y^2y2 of perturbed equations (5.2).

Formalization targets

Goal: Theorem 5.6 (corrected)

For σ3≠0\sigma_3\neq0σ3​=0 and hσ3≠1h\sigma_3\neq1hσ3​=1, the ODE (5.3) has a solution satisfying (5.9) for every T>0T>0T>0 if and only if one of the following holds:

  1. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (−∞,h](-\infty,h](−∞,h] or α3=0\alpha_3=0α3​=0;
  2. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,∞)[h,\infty)[h,∞) or α3=0\alpha_3=0α3​=0;
  3. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,1/σ3)[h,1/\sigma_3)[h,1/σ3​) or F(y)→0F(y)\to0F(y)→0 as y↑1/σ3y\uparrow1/\sigma_3y↑1/σ3​;
  4. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (1/σ3,h](1/\sigma_3,h](1/σ3​,h] or F(y)→0F(y)\to0F(y)→0 as y↓1/σ3y\downarrow1/\sigma_3y↓1/σ3​.

The limit alternatives in cases 3 and 4 are not printed in the paper. Without them the equivalence is false. Take σ3=1\sigma_3=1σ3​=1, f1=1f_1=1f1​=1, f2=−1f_2=-1f2​=−1, all other coefficients 000, and h=0h=0h=0. Then F(y)=1−yF(y)=1-yF(y)=1−y, and yt=1−et−Ty_t=1-e^{t-T}yt​=1−et−T satisfies (5.9) on every horizon, yet none of the printed cases holds. The gap is in the Appendix (p. 48): it asserts that FFF is positive on the closed interval [h,σ3−1][h,\sigma_3^{-1}][h,σ3−1​] when α0=0\alpha_0=0α0​=0, which fails when the polynomial part vanishes at the pole. A companion item records the counterexample.

Milestones

The milestones follow the paper's proof:

  • the decomposition (5.8);
  • the comparison Lemma 5.1;
  • the three sufficiency arguments of p. 23 (case (i) with a zero, case (i) with α3=0\alpha_3=0α3​=0, case (iii));
  • the necessity bounds of the Appendix:
    • in case (i): a zero exists when α3>0\alpha_3>0α3​>0, and F(y)≤−ε(h+1−y)2F(y)\le-\varepsilon(h+1-y)^2F(y)≤−ε(h+1−y)2 when α3<0\alpha_3<0α3​<0 and there is no zero;
    • in case (iii): a zero exists when α0<0\alpha_0<0α0​<0, and F(y)≥ε(σ3−1−y)−1F(y)\ge\varepsilon(\sigma_3^{-1}-y)^{-1}F(y)≥ε(σ3−1​−y)−1 when α0>0\alpha_0>0α0​>0 and there is no zero;
  • the comparison with the explicit solution (σ3−1−y~t)2=(σ3−1−h)2−2ε(T−t)(\sigma_3^{-1}-\tilde y_t)^2=(\sigma_3^{-1}-h)^2-2\varepsilon(T-t)(σ3−1​−y~​t​)2=(σ3−1​−h)2−2ε(T−t);
  • the case α0=0\alpha_0=0α0​=0, with the endpoint positivity made a hypothesis.

Significance

In the paper, Theorem 5.6 is the sharp solvability criterion for linear FBSDEs with constant coefficients and σ3≠0\sigma_3\neq0σ3​=0. The paper describes these sharp conditions as setting the "limits" for the solvability of general FBSDEs, and the nonlinear Theorems 5.9–5.11 and the main well-posedness Theorem 7.4 are modelled on them. Because the criterion is an equivalence, it also says when no regular decoupling field can be built from the dominating ODE, whatever the horizon.

The result is proved in the paper, but the printed statement is not correct as an equivalence (see above). The mission states and asks for a corrected version, a machine-checked counterexample to the printed one, and formal versions of each step of the proof. The deterministic parts (comparison for backward integral equations, finite-time blow-up of scalar autonomous ODEs, pole-reaching for rational vector fields) are basic real analysis with no current Lean library. They are reusable well beyond FBSDEs. No part of this paper has a machine-checked proof.

Difficulty

Each sufficiency case is an a priori bound: a comparison with a constant or explicitly solvable equation keeps the solution in a fixed interval away from the pole. The difficulty is on the necessity side, where three kinds of failure must be excluded:

  • blow-up to ±∞\pm\infty±∞ when α3≠0\alpha_3\neq0α3​=0 has the wrong sign;
  • reaching the pole in finite time when α0>0\alpha_0>0α0​>0;
  • reaching the pole when α0=0\alpha_0=0α0​=0.

The obvious argument for the last case, "FFF is bounded below by a positive constant up to the pole", is exactly what fails when FFF tends to 000 at the pole. There the solution approaches the pole only asymptotically, and the right criterion is the corrected one above. A second subtlety is that FFF is only locally Lipschitz off the pole, so comparison must be carried out on a band in which the solution provably stays.

Formalization scope

Time is real, with 0≤t≤T0\le t\le T0≤t≤T and T>0T>0T>0. The coefficients form a record Coeffs of nine reals, and Coeffs.F is (3.9) verbatim. A solution on [0,T][0,T][0,T] is a function y:R→Ry:\mathbb R\to\mathbb Ry:R→R such that, for every t∈[0,T]t\in[0,T]t∈[0,T], the integrand s↦F(ys)s\mapsto F(y_s)s↦F(ys​) is integrable on [t,T][t,T][t,T] and yt=h+∫tTF(ys) dsy_t=h+\int_t^TF(y_s)\,dsyt​=h+∫tT​F(ys​)ds; values outside [0,T][0,T][0,T] are irrelevant. Condition (5.9) is a uniform bound on ∣y∣|y|∣y∣ together with ∣1−σ3yt∣≥κ|1-\sigma_3y_t|\ge\kappa∣1−σ3​yt​∣≥κ for some κ>0\kappa>0κ>0. "For arbitrary TTT" is a universal quantifier over T>0T>0T>0 outside the existential.

Lean's conventions are total, so several trivializing formalizations are ruled out explicitly:

  • Lean's integral of a non-integrable function is 000, so integrability is part of the solution predicate.
  • Lean's x/0=0x/0=0x/0=0 gives Coeffs.F a junk value at the pole. No statement evaluates FFF there: every zero point, bound and limit in the statements lives strictly on one side of 1/σ31/\sigma_31/σ3​.
  • (5.9) is never encoded as a bound on the Lean inverse (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1, which is 000 at the pole.
  • σ3≠0\sigma_3\neq0σ3​=0 is assumed wherever α3\alpha_3α3​ or 1/σ31/\sigma_31/σ3​ appears.
  • Lemma 5.1 adds the hypothesis y1≤y2y^1\le y^2y1≤y2, without which it is false, and asks the cic^ici to be integrable.

The constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​ of (5.8) enter the necessity milestones only through the decomposition hypothesis, never through a formula.

The development needs a Picard–Lindelöf or comparison argument for backward scalar integral equations with locally Lipschitz right-hand sides, monotonicity of autonomous scalar solutions, and the intermediate value theorem. Contributions of a general comparison lemma for scalar integral equations would serve this mission and both other missions of the series.

Selected references

  • J. Ma, Z. Wu, D. Zhang, J. Zhang, On well-posedness of forward–backward SDEs—a unified approach, Ann. Appl. Probab. 25(4):2168–2214, 2015. arXiv:1110.4658v2, doi:10.1214/14-AAP1046
  • J. Ma, P. Protter, J. Yong, Solving forward–backward stochastic differential equations explicitly—a four step scheme, Probab. Theory Related Fields 98:339–359, 1994. doi:10.1007/BF01192258
  • Y. Hu, S. Peng, Solution of forward–backward stochastic differential equations, Probab. Theory Related Fields 103:273–283, 1995. doi:10.1007/BF01204218
  • J. Ma, J. Yong, Forward–Backward Stochastic Differential Equations and Their Applications, Lecture Notes in Math. 1702, Springer, 1999. doi:10.1007/978-3-540-48831-6
14 thms1 active userReviewed
ProbabilityStochastic Systems·Captain: mikedeng1

Coexistence and Extinction for Stochastic Kolmogorov Systems 2: If a Boundary Ergodic Measure Is a Sink, then E(min_i X_i(t))^δ → 0 for Every Small δ > 0Research Paper

Why stochastic extinction matters

A population can disappear because its average growth rate is negative when it is rare, even if its deterministic dynamics would support coexistence. Interactions among several species make this harder to assess: a species may be rare while the remaining species fluctuate among several possible long-run configurations. Hening and Nguyen study this problem for nonlinear systems driven by correlated environmental Brownian noise. Their analysis treats the noncompact state space [0,∞)n[0,\infty)^n[0,∞)n, where population sizes have no fixed upper bound. The central result of this mission gives a quantitative form of approach to the boundary when one boundary community acts as a sink: the expected positive moment of the smallest population size tends to zero. The source is Hening and Nguyen, Coexistence and extinction for stochastic Kolmogorov systems, arXiv:1704.06984v1, Theorems 1.2 and 5.1.

The population system and its boundary laws

There are n≥1n\ge1n≥1 species. Their abundances form X(t)=(X1(t),…,Xn(t))∈R+n=[0,∞)nX(t)=(X_1(t),\ldots,X_n(t))\in\mathbb R^n_+=[0,\infty)^nX(t)=(X1​(t),…,Xn​(t))∈R+n​=[0,∞)n. Species iii has per capita drift fi(x)f_i(x)fi​(x) and environmental noise intensity gi(x)g_i(x)gi​(x) at state xxx. A matrix Γ\GammaΓ correlates the noise: E=Γ⊤BE=\Gamma^\top BE=Γ⊤B for a vector BBB of independent standard Brownian motions, and Σ=Γ⊤Γ=(σij)\Sigma=\Gamma^\top\Gamma=(\sigma_{ij})Σ=Γ⊤Γ=(σij​). The stochastic Kolmogorov system is

dXi(t)=Xi(t)fi(X(t)) dt+Xi(t)gi(X(t)) dEi(t),i=1,…,n.dX_i(t)=X_i(t)f_i(X(t))\,dt+X_i(t)g_i(X(t))\,dE_i(t),\qquad i=1,\ldots,n.dXi​(t)=Xi​(t)fi​(X(t))dt+Xi​(t)gi​(X(t))dEi​(t),i=1,…,n.

The factor XiX_iXi​ makes the state Xi=0X_i=0Xi​=0 absorbing in that coordinate. Consequently each collection of present species defines an invariant face of the orthant. The interior R+n,∘=(0,∞)n\mathbb R^{n,\circ}_+=(0,\infty)^nR+n,∘​=(0,∞)n consists of states where every species is present. The paper uses ∥x∥=∑i∣xi∣\|x\|=\sum_i|x_i|∥x∥=∑i​∣xi​∣ throughout. Its standing Assumption 1.1 requires local Lipschitz coefficients, nondegenerate noise in each population subspace, and a negative large-state drift condition (1.2) expressed through positive cic_ici​ and γb\gamma_bγb​. These conditions place the same control on the unbounded part of the orthant in every theorem below. Source, §1.1, pp. 3–4.

A probability measure μ\muμ is invariant if the law of X(t)X(t)X(t) remains μ\muμ when X(0)X(0)X(0) has law μ\muμ. It is ergodic if it is an extreme point of the invariant probability measures. Let MMM contain the ergodic invariant measures supported on the boundary ∂R+n\partial\mathbb R^n_+∂R+n​. This set includes the Dirac law δ∗\delta_*δ∗​ at zero. For any invariant μ\muμ, the invasion rate of species iii is

λi(μ)=∫(fi(x)−12σiigi(x)2) μ(dx).\lambda_i(\mu)=\int\left(f_i(x)-\tfrac12\sigma_{ii}g_i(x)^2\right)\,\mu(dx).λi​(μ)=∫(fi​(x)−21​σii​gi​(x)2)μ(dx).

The term σiigi2/2\sigma_{ii}g_i^2/2σii​gi2​/2 records the effect of environmental variation on logarithmic population growth. For μ∈M\mu\in Mμ∈M, let IμI_\muIμ​ be its present species and R+μ\mathbb R^\mu_+R+μ​ its coordinate face. The set MμM_\muMμ​ contains boundary ergodic measures supported on the boundary of that face. Assumption 1.3 requires λi(μ)<0\lambda_i(\mu)<0λi​(μ)<0 for every i∉Iμi\notin I_\mui∈/Iμ​ and, when Iμ≠∅I_\mu\ne\varnothingIμ​=∅, a positive invasion rate among IμI_\muIμ​ for every finite convex combination of measures in MμM_\muMμ​. Thus the missing species decline near μ\muμ, while the community on its face resists collapse to a smaller face. Source, pp. 5–6.

Formalization targets

The goal is Theorem 1.2 in the explicit quantification of Theorem 5.1. Let δ0>0\delta_0>0δ0​>0 satisfy the paper's bound (3.2). For every 0<δ<δ00<\delta<\delta_00<δ<δ0​ and every x∈R+n,∘x\in\mathbb R^{n,\circ}_+x∈R+n,∘​,

lim⁡t→∞Ex(min⁡1≤i≤nXi(t))δ=0.\lim_{t\to\infty}\mathbb E_x\left(\min_{1\le i\le n}X_i(t)\right)^\delta=0.t→∞lim​Ex​(1≤i≤nmin​Xi​(t))δ=0.

This is the moment form of approach to the boundary. It does not specify which species tends to zero on a given path. The companion targets retain the paper's route: strong solutions and face invariance in Lemma 3.1, moment and Feller estimates in Lemma 3.2, zero resident invasion rates in Lemma 5.1, the weighted negative margin (5.1)–(5.2), the averaged drift bound in Lemma 5.2, local contraction in Proposition 5.1, global control in Lemma 5.3, the capped one-step bound (5.11)–(5.12), and transience in the interior. Source, §§3 and 5.

What the result gives

The conclusion detects extinction pressure without asking in advance which coordinate disappears. Since the minimum of the coordinates is small whenever the system is near any boundary face, it applies even when trajectories may approach different faces. The paper uses this result before its stronger classification theorem, which adds assumptions to determine the fate of particular species. Theorem 1.2 is proved in the cited paper; this mission seeks a machine-checked development of that known result and its supporting stochastic estimates. In particular, the formalization makes explicit how invariant measures on smaller faces control a statement about solutions starting in the full interior. Source, Theorems 1.2 and 1.3.

Where the difficulty lies

A negative invasion rate at one boundary law does not by itself control the whole trajectory. The surviving species can fluctuate toward a still smaller face, where a missing species may have a different growth rate. Assumption 1.3 excludes that obstruction by quantifying over boundary ergodic laws of the selected face. Another obstacle is unbounded population size: a local bound near the face cannot alone give convergence of expected moments. The paper combines face-specific estimates with global moment control; encoding both regimes faithfully is the main mathematical burden. The compact-state intuition cited in the paper does not immediately apply to the noncompact orthant. Source, Remark 1.6 and §5.

Formalization scope

Lean represents Rn\mathbb R^nRn by the published EthierKurtz.SDEState n, with coordinates indexed by Fin n from zero to n−1n-1n−1. The SDE uses the published strong Brownian solution interface; a common probability space, Brownian motion, and solution family replace the paper's notation Px\mathbb P_xPx​ and Ex\mathbb E_xEx​. The model reads coefficients at the componentwise positive part off the orthant, where the source never evaluates them. Assumption 1.1(3)'s strict limit superior becomes an equivalent eventual negative ε\varepsilonε bound. Ergodicity is extremality. The index set IμI_\muIμ​ is defined through positive μ\muμ-mass of xi>0x_i>0xi​>0. Finite convex combinations, rather than a closure of their hull, implement the paper's Conv⁡\operatorname{Conv}Conv.

The stated goal requires n≥1n\ge1n≥1 and δ>0\delta>0δ>0; δ=0\delta=0δ=0 would make the displayed expectation equal to one. Theorem 5.1 suppresses the latter restriction, while Theorem 1.2 states it. Lemma 5.2's displayed average divides by TTT, so its TeT_eTe​ is positive, as its proof says, despite the printed Te≥0T_e\ge0Te​≥0. The weights, time threshold, and contraction exponent are chosen before the points and times over which their bounds hold. Boundary ergodic measures are not assumed to be absent; the explicit δ∗∈M\delta_*\in Mδ∗​∈M target records nonemptiness. The definitions of UθU_\thetaUθ​, invariant measures and invasion rates, together with finite-dimensional stochastic integration and moment estimates, are reusable beyond this mission. Contributions that establish these interfaces or prove the listed paper statements are in scope.

The radius MMM of (3.1) is positive. The freely chosen δ0\delta_0δ0​ is below one, as Appendix A uses, and the extinction weights are selected with ∑i∈Iμp^i≤δ0\sum_{i\in I_\mu}\widehat p_i\le\delta_0∑i∈Iμ​​p​i​≤δ0​. Scaling all positive weights and the margin preserves (5.2) and makes the paper's CUC_UCU​ finite. Bounds involving real expectations explicitly include integrability, so Lean's value for a nonintegrable integral cannot satisfy them by default. The transience target applies to each compact interior set with nonempty interior, as the proof on p. 24 does.

Selected references

  • Alexandru Hening and Dang H. Nguyen, Coexistence and extinction for stochastic Kolmogorov systems, Annals of Applied Probability 28(3), 2018. Formalization uses arXiv:1704.06984v1, 23 April 2017, especially pp. 3–7, 13–14, and 20–24.
18 thms1 active userReviewed
ProbabilityStochastic Systems·Captain: mikedeng1

Coexistence and Extinction for Stochastic Kolmogorov Systems 3: Almost Surely the Occupation Measures Settle on One Sink Measure µ, and Every Species Absent from µ Dies Out at Rate λ_i(µ) < 0Research Paper

Motivation

Ecologists model interacting populations — competitors, predators and prey, food chains — by Kolmogorov systems, in which the growth of each species is proportional to its current abundance. Environmental fluctuations turn these into stochastic differential equations, and the basic question becomes which species persist and which go extinct. Hening and Nguyen (arXiv:1704.06984, Ann. Appl. Probab. 28(3), 2018) gave sharp answers for a general class of such systems on the non-compact state space [0,∞)n[0,\infty)^n[0,∞)n, extending the compact-simplex theory of Schreiber, Benaïm and Atchadé (SBA11).

The paper has three main results: persistence when every boundary ergodic measure repels (Theorem 1.1), extinction in mean when one boundary measure attracts (Theorem 1.2), and a classification of which species die out (Theorem 1.3). This mission formalizes the third. When the community does not persist, Theorem 1.3 says that each path settles near exactly one "sink" measure on the boundary, and identifies the species that vanish and their rates of decay.

Timeline: Schreiber, Benaïm and Atchadé (2011) proved persistence criteria for stochastic population models on the simplex {y∈R+n:y1+⋯+yn=1}\{y \in \mathbb R^n_+ : y_1 + \dots + y_n = 1\}{y∈R+n​:y1​+⋯+yn​=1}. Evans, Hening and Schreiber (EHS15, 2015), studying patch-selection strategies in stochastic environments, extended the limit theorem for occupation measures to locally compact state spaces. Hening and Nguyen (2017/2018) proved persistence with exponential convergence and the extinction classification for general Kolmogorov systems.

Setting

Let n≥1n \ge 1n≥1, R+n=[0,∞)n\mathbb R^n_+ = [0,\infty)^nR+n​=[0,∞)n, R+n,∘=(0,∞)n\mathbb R^{n,\circ}_+ = (0,\infty)^nR+n,∘​=(0,∞)n, ∂R+n=R+n∖R+n,∘\partial\mathbb R^n_+ = \mathbb R^n_+\setminus\mathbb R^{n,\circ}_+∂R+n​=R+n​∖R+n,∘​, and ∥x∥=∑i∣xi∣\|x\| = \sum_i |x_i|∥x∥=∑i​∣xi​∣. The abundances X=(X1,…,Xn)X = (X_1,\dots,X_n)X=(X1​,…,Xn​) solve

dXi(t)=Xi(t)fi(X(t)) dt+Xi(t)gi(X(t)) dEi(t),i=1,…,n,dX_i(t) = X_i(t)f_i(X(t))\,dt + X_i(t)g_i(X(t))\,dE_i(t),\qquad i = 1,\dots,n,dXi​(t)=Xi​(t)fi​(X(t))dt+Xi​(t)gi​(X(t))dEi​(t),i=1,…,n,

where E=Γ⊤BE = \Gamma^\top BE=Γ⊤B for an nnn-dimensional standard Brownian motion BBB, and Σ=Γ⊤Γ=(σij)\Sigma = \Gamma^\top\Gamma = (\sigma_{ij})Σ=Γ⊤Γ=(σij​). Assumption 1.1 asks that (gigjσij)(g_ig_j\sigma_{ij})(gi​gj​σij​) be positive definite, that fi,gif_i, g_ifi​,gi​ be locally Lipschitz, and that a dissipativity condition (1.2) with a vector c>0c > 0c>0 and a constant γb>0\gamma_b > 0γb​>0 hold at infinity.

An invariant probability measure μ\muμ is one with ∫P(t,x,A) μ(dx)=μ(A)\int P(t,x,A)\,\mu(dx) = \mu(A)∫P(t,x,A)μ(dx)=μ(A) for all ttt; it is ergodic if it is an extreme point of the invariant probability measures. M\mathcal MM is the set of ergodic invariant probability measures supported on ∂R+n\partial\mathbb R^n_+∂R+n​; it contains the Dirac mass δ∗\delta^*δ∗ at the origin. For μ∈M\mu \in \mathcal Mμ∈M, IμI_\muIμ​ is the set of species charged by μ\muμ and IμcI^c_\muIμc​ its complement. The Lyapunov exponent of species iii at μ\muμ is

λi(μ)=∫(fi(x)−σiigi2(x)2)μ(dx).\lambda_i(\mu) = \int\Big(f_i(x) - \frac{\sigma_{ii}g_i^2(x)}{2}\Big)\mu(dx).λi​(μ)=∫(fi​(x)−2σii​gi2​(x)​)μ(dx).

A measure μ∈M\mu \in \mathcal Mμ∈M is a sink (Assumption 1.3) if λi(μ)<0\lambda_i(\mu) < 0λi​(μ)<0 for all i∈Iμci \in I^c_\mui∈Iμc​ and, if Iμ≠∅I_\mu \ne \emptysetIμ​=∅, every finite convex combination ν\nuν of ergodic measures living on the relative boundary of the face of μ\muμ has max⁡i∈Iμλi(ν)>0\max_{i\in I_\mu}\lambda_i(\nu) > 0maxi∈Iμ​​λi​(ν)>0. M1\mathcal M^1M1 is the set of sinks and M2=M∖M1\mathcal M^2 = \mathcal M\setminus\mathcal M^1M2=M∖M1.

The occupation measures of a path are Π~t=1t∫0t1{X(s)∈⋅}ds\widetilde\Pi_t = \frac1t\int_0^t\mathbf 1_{\{X(s)\in\cdot\}}dsΠt​=t1​∫0t​1{X(s)∈⋅}​ds, and U(ω)\mathcal U(\omega)U(ω) is the set of weak limits of Π~t(ω)\widetilde\Pi_t(\omega)Πt​(ω) as t→∞t\to\inftyt→∞. Assumption 1.4 asks that ∥x∥δ1∑igi2/(1+∑i(∣fi∣+gi2))→0\|x\|^{\delta_1}\sum_ig_i^2/(1+\sum_i(|f_i|+g_i^2)) \to 0∥x∥δ1​∑i​gi2​/(1+∑i​(∣fi​∣+gi2​))→0 for some δ1>0\delta_1 > 0δ1​>0; Assumption 1.5 asks that M2=∅\mathcal M^2 = \emptysetM2=∅ or that every finite convex combination ν\nuν of measures of M2\mathcal M^2M2 has max⁡iλi(ν)>0\max_i\lambda_i(\nu) > 0maxi​λi​(ν)>0.

Formalization targets

Goal: Theorem 1.3

Under Assumptions 1.1, 1.4, 1.5 and M1≠∅\mathcal M^1 \ne \emptysetM1=∅, for every x∈R+n,∘x \in \mathbb R^{n,\circ}_+x∈R+n,∘​,

∑μ∈M1Pxμ=1,Pxμ:=Px{U(ω)={μ}, lim⁡t→∞ln⁡Xi(t)t=λi(μ)<0, i∈Iμc}>0.\sum_{\mu\in\mathcal M^1} P^\mu_x = 1,\qquad P^\mu_x := \mathbb P_x\Big\{\mathcal U(\omega) = \{\mu\},\ \lim_{t\to\infty}\frac{\ln X_i(t)}{t} = \lambda_i(\mu) < 0,\ i\in I^c_\mu\Big\} > 0 .μ∈M1∑​Pxμ​=1,Pxμ​:=Px​{U(ω)={μ}, t→∞lim​tlnXi​(t)​=λi​(μ)<0, i∈Iμc​}>0.

Milestones

In the order the proof uses them: δ∗∈M\delta^* \in \mathcal Mδ∗∈M; Lemma 3.3 (moment bound and a zero-mean identity for invariant measures); Lemma 5.1 (λi(μ)=0\lambda_i(\mu) = 0λi​(μ)=0 for i∈Iμi \in I_\mui∈Iμ​); Lemma 5.4 (bounded weighted time averages and a strong law for the stochastic integral); Lemma 5.5 (time spent in a compact set, and staying away from a face on a finite horizon); Lemma 5.6 (convergence of unbounded time averages); Lemma 5.7 (U(ω)\mathcal U(\omega)U(ω) consists of invariant measures); Lemma 5.8 (a limit set inside the face of a sink is that sink); Lemma 5.9 (sinks attract nearby paths with high probability); and the case M2=∅\mathcal M^2 = \emptysetM2=∅, where M=M1={δ∗}\mathcal M = \mathcal M^1 = \{\delta^*\}M=M1={δ∗}.

Significance

Theorem 1.3 turns local information — the signs of finitely many Lyapunov exponents at boundary ergodic measures — into a global almost-sure description of long-run behaviour: the community converges, in the sense of empirical distributions, to one of the sinks, each sink is reached with positive probability, and the species absent from it decay exponentially at explicit rates. In the applications of §2 of the paper (competitive Lotka–Volterra systems, food chains) this answers which species survive.

The theorem is proved on paper. No part of it is machine-checked. A formalization would produce a checked interface between Itô calculus for multidimensional SDEs, ergodic theory of Feller processes (occupation measures, invariant and ergodic measures), and the stochastic-persistence framework; the statements of Lemmas 5.4–5.7 are reusable for other SDE models with a Lyapunov-type condition.

Difficulty

The obvious argument — the occupation measures converge to some invariant measure, and the Lyapunov exponents at that measure decide the fate of each species — breaks down at two points. First, the state space is not compact and the functions fi−σiigi2/2f_i - \sigma_{ii}g_i^2/2fi​−σii​gi2​/2 are unbounded, so weak convergence of occupation measures does not by itself give convergence of time averages of these functions; a pathwise uniform-integrability bound (Lemmas 5.4 and 5.6) is required, and this is where Assumption 1.4 enters. Second, a limit point of occupation measures is in general a mixture of ergodic measures, possibly including repellers; ruling out every mixture that is not a single sink requires the separate arguments of Lemma 5.8 and of the M2\mathcal M^2M2 step, together with a supermartingale built from a Lyapunov function near each sink (Lemma 5.9).

Formalization scope

The state space is EuclideanSpace ℝ (Fin n) with the published Ethier–Kurtz strong-SDE layer; coordinates are indexed by Fin n, the norm in every assumption is the ℓ1\ell^1ℓ1 norm, and n≥1n \ge 1n≥1 is a hypothesis. The process is a family of strong solutions XxX^xXx, one from each x∈R+nx \in \mathbb R^n_+x∈R+n​, driven by one Brownian motion on one probability space. The coefficients are read at the positive part of the state, which is the state itself on R+n\mathbb R^n_+R+n​. Ergodic means extremal among invariant probability measures, IμI_\muIμ​ is the set of coordinates that are not μ\muμ-a.s. zero, Conv\mathrm{Conv}Conv means finite convex combinations with positive weights (as on p. 5), and weak limits are taken along sequences, tested against bounded continuous functions. The sum in (1.11) is an unconditional sum in [0,∞][0,\infty][0,∞] over the set M1\mathcal M^1M1, with no finiteness assumption.

Deviations from the page, each disclosed in the item: (5.19) is stated for every finite horizon rather than for neTen_eT_ene​Te​, which is undefined under the lemma's hypotheses; Lemma 5.9 takes k≥1k \ge 1k≥1; the convention δ1≤δ0\delta_1 \le \delta_0δ1​≤δ0​ of Assumption 1.4 is an explicit hypothesis where the exponent δ1\delta_1δ1​ appears; integrability claims that the paper treats as automatic are part of the conclusions; and (5.17) is stated for every continuous version of the Itô integral. Lemma 5.6 is stated for each path that stays in the orthant, which the solution does almost surely. The proof's claim "U(ω)⊂Conv(M)∖Conv(M2)\mathcal U(\omega) \subset \mathrm{Conv}(\mathcal M)\setminus\mathrm{Conv}(\mathcal M^2)U(ω)⊂Conv(M)∖Conv(M2)" is left as source context: its inclusion in the finite convex hull of M\mathcal MM requires an additional argument when M\mathcal MM is infinite.

The statements cannot be made vacuous by the definitions: δ∗∈M\delta^* \in \mathcal Mδ∗∈M is itself a milestone, so M\mathcal MM is never empty, and the occupation measures are probability measures for t>0t > 0t>0; every constant (K^\widehat KK, K^1\widehat K_1K1​, β\betaβ, Δ\DeltaΔ) is chosen before the points it must be uniform in.

A complete development needs Itô's formula for ln⁡Xi\ln X_ilnXi​, the strong law for continuous martingales with bounded quadratic-variation growth, Prokhorov's theorem and lower semicontinuity of integrals under weak convergence, and the Feller and strong Markov properties of (1.1). Contributions of any of these, and of the milestones in any order, are welcome.

Selected references

  • A. Hening, D. H. Nguyen, Coexistence and extinction for stochastic Kolmogorov systems, Ann. Appl. Probab. 28(3), 2018, DOI 10.1214/17-AAP1347; arXiv:1704.06984v1. https://arxiv.org/abs/1704.06984
  • S. J. Schreiber, M. Benaïm, K. A. S. Atchadé, Persistence in fluctuating environments, J. Math. Biol. 62(5), 655–683, 2011. MR 2786721, https://mathscinet.ams.org/mathscinet-getitem?mr=2786721
  • S. N. Evans, A. Hening, S. J. Schreiber, Protected polymorphisms and evolutionary stability of patch-selection strategies in stochastic environments, J. Math. Biol. 71(2), 325–359, 2015. MR 3367678, https://mathscinet.ams.org/mathscinet-getitem?mr=3367678
  • R. Khasminskii, Stochastic Stability of Differential Equations, 2nd ed., Springer, 2012. MR 2894052, https://mathscinet.ams.org/mathscinet-getitem?mr=2894052
20 thms1 active userReviewed
AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Averaging Dynamics Driven by Fractional Brownian Motion: Young Solutions of dxⁿ = fₙ(t, xⁿ)dB Converge in Probability in C^α to the Solution of dx = f̄(x)dB When |fₙ − f̄|_{−κ,γ} → 0Research Paper

Why oscillating coefficients matter

An equation driven by fractional Brownian motion can respond to a rapidly varying coefficient even when that coefficient has no useful pointwise limit. Hairer and Li study this issue for fractional Brownian motion with Hurst index above one half. Their Section 3 isolates a deterministic averaging statement: if the time antiderivatives of the coefficients approach those of a limiting coefficient in a suitable negative Hölder norm, the solutions approach the limiting solution in probability. This statement supplies a common target for averaging models whose fast variables have very different origins. The authors use it later with mixing fast processes, and also present a quasi-periodic example. The result and its role in the paper are stated in Hairer and Li, Section 3.

The problem sits at the boundary of two familiar views of differential equations. A pathwise Young equation is defined from individual sufficiently regular paths, whereas the available estimates for the oscillating coefficient and the fractional Brownian driver involve probability and conditional expectation. The mission records the precise point where these descriptions meet. It treats the published article, rather than a preprint, and targets its Theorem 3.13.

Driver, coefficients, and solutions

An mmm-dimensional fractional Brownian motion B=(B1,…,Bm)B=(B^1,\ldots,B^m)B=(B1,…,Bm) with index HHH is a centered Gaussian process with independent coordinates and covariance

E[BsiBtj]=1i=j∣s∣2H+∣t∣2H−∣t−s∣2H2.\mathbb E[B_s^iB_t^j]=\mathbf1_{i=j}\frac{|s|^{2H}+|t|^{2H}-|t-s|^{2H}}2.E[Bsi​Btj​]=1i=j​2∣s∣2H+∣t∣2H−∣t−s∣2H​.

The paper works with a two-sided process and 1/2<H<11/2<H<11/2<H<1. It uses a version whose sample paths are locally β\betaβ-Hölder for every β<H\beta<Hβ<H. The mission names that version condition separately, because the covariance law alone does not select particular sample paths. The relevant past sigma algebra at time sss is generated by increments Bu−BvB_u-B_vBu​−Bv​ with u,v≤su,v\le su,v≤s. These conventions come from pp. 1826 and 1831–1832 of the article.

For a path xxx on [0,T][0,T][0,T], write ∣x∣α|x|_\alpha∣x∣α​ for its homogeneous Hölder seminorm and ∣x∣∞|x|_\infty∣x∣∞​ for its supremum norm. The norm on Cα[0,T]C^\alpha[0,T]Cα[0,T] is ∣x∣∞+∣x∣α|x|_\infty+|x|_\alpha∣x∣∞​+∣x∣α​. A Young integral ∫stfr dbr\int_s^t f_r\,db_r∫st​fr​dbr​ is the limit of left-point sums over partitions of [s,t][s,t][s,t] as the largest cell shrinks to zero. A Young solution from x0x_0x0​ is an α\alphaα-Hölder path satisfying its integral equation at every time, with value x0x_0x0​ at time zero. Here BC2BC^2BC2 means bounded, twice continuously differentiable maps with bounded derivatives through order two; Cζ,2C^{\zeta,2}Cζ,2 means ζ\zetaζ-Hölder in time with values in BC2BC^2BC2. These are the paper's conventions on pp. 1829 and 1835–1838.

The negative Hölder bound ∣f∣−κ,γ≤K|f|_{-\kappa,\gamma}\le K∣f∣−κ,γ​≤K means that the time antiderivative of fff has increments bounded by K∣t−s∣1−κK|t-s|^{1-\kappa}K∣t−s∣1−κ, and that the difference of those increments at spatial points x,yx,yx,y is bounded by K∣t−s∣1−κ∣x−y∣γK|t-s|^{1-\kappa}|x-y|^\gammaK∣t−s∣1−κ∣x−y∣γ. Both bounds apply on the time window in question when ∣t−s∣≤1|t-s|\le1∣t−s∣≤1. This is equation (3.12) in the article. It measures cancellation over time; it does not require f(t,x)f(t,x)f(t,x) itself to be small.

Formalization targets

The goal is the dBdBdB part of Theorem 3.13. Let fnf_nfn​ be Cζ,2C^{\zeta,2}Cζ,2, let the limiting fˉ\bar ffˉ​ be autonomous and in BC2BC^2BC2, and suppose ∣fn−fˉ∣−κ,γ→0|f_n-\bar f|_{-\kappa,\gamma}\to0∣fn​−fˉ​∣−κ,γ​→0. The exponents satisfy 1/2<α<H−κ1/2<\alpha<H-\kappa1/2<α<H−κ, H−κ>1/2H-\kappa>1/2H−κ>1/2, H−κ+γα>1H-\kappa+\gamma\alpha>1H−κ+γα>1, and α<ζ≤1\alpha<\zeta\le1α<ζ≤1. For Young solutions with the same starting point,

dxtn=fn(t,xtn) dBt,dxt=fˉ(xt) dBt,dx_t^n=f_n(t,x_t^n)\,dB_t,\qquad dx_t=\bar f(x_t)\,dB_t,dxtn​=fn​(t,xtn​)dBt​,dxt​=fˉ​(xt​)dBt​,

the target is

∀ε>0,P(∥xn−x∥Cα[0,T]>ε)⟶0.\forall\varepsilon>0,\qquad P\bigl(\|x^n-x\|_{C^\alpha[0,T]}>\varepsilon\bigr)\longrightarrow0.∀ε>0,P(∥xn−x∥Cα[0,T]​>ε)⟶0.

The milestone list follows the statements used around this target: the Hölder composition estimate of Lemma 2.1, the RKHS estimate of Lemma 3.3, the fractional Brownian integral estimate of Lemma 3.4, the stochastic sewing lemma of Lemma 3.5, the Young case of (3.18) from Lemmas 3.10 and 3.12, the Kolmogorov inclusions (3.24), and the deterministic stability estimate of Lemma 2.2. Each is a separate formal theorem. The authors' proofs follow their statements in Sections 2 and 3 and the Appendix; Lemma 3.5 is quoted from Lê, Theorem 2.1 without proof in the article.

What the result provides

The target gives convergence of entire solution paths in a Hölder topology, in probability. In the paper, this lets a model-specific estimate of the negative Hölder distance be used to conclude convergence of the corresponding dynamical system. Theorem A is obtained by adding such an estimate for a stationary mixing fast process; the deterministic statement here isolates the part independent of that model. These uses are described in Sections 1 and 3.

The published paper proves the result. This mission asks for machine-checked proofs of the stated Lean theorems. Its reusable work would include a pathwise Young integral over arbitrary partitions, Hölder norms that retain the value +∞+\infty+∞, a two-sided vector fractional Brownian motion interface, and stochastic estimates for time-dependent integrands. The goal and milestones in this proposal are statements with proof placeholders; the local build checks their types, not their proofs.

Main obstruction

Pointwise control of fn−fˉf_n-\bar ffn​−fˉ​ is unavailable: a rapidly oscillating function can be large at most times and still have small time antiderivatives. Applying a pathwise Young stability estimate directly to fn−fˉf_n-\bar ffn​−fˉ​ therefore leaves a coefficient norm that need not tend to zero. The integral estimate must connect cancellation measured by ∣⋅∣−κ,γ|\cdot|_{-\kappa,\gamma}∣⋅∣−κ,γ​ with LpL^pLp bounds on the driven equation. The dependence on the past of the fractional Brownian motion makes this step more delicate than an estimate for a deterministic integrand. The required estimates and their domains appear in Lemmas 3.4–3.12.

Formalization scope

Time is R\mathbb RR for the two-sided driver; coefficient and solution assertions use [0,T][0,T][0,T] with T>0T>0T>0. State spaces are finite-dimensional real Euclidean spaces. The goal takes H∈(1/2,1)H\in(1/2,1)H∈(1/2,1) from the standing setting of Section 3.1, and it assumes the locally Hölder version of BBB described on p. 1826. The solutions are required almost surely to satisfy the Young equation from the same x0x_0x0​. This requirement fixes the processes to the equations; the convergence claim cannot be obtained by choosing arbitrary paths. Probability of the norm event uses the measure of that set, and the conclusion is convergence in probability in the full CαC^\alphaCα norm.

The Lean definitions use [0,∞][0,\infty][0,∞] for path and process seminorms, so unbounded suprema are not replaced by a default real value. The negative Hölder hypothesis uses real bounds Kn→0K_n\to0Kn​→0 instead of an infimum that could be meaningless on an empty class. The Young integral quantifies over every monotone partition and the mesh limit of its left-point sums. The fBm definition includes Gaussianity, means, and every cross-coordinate covariance; its path version is explicit. Interval integrals in the coefficient bound are applied to time-continuous coefficients in the goal. Lemmas 3.4 and 3.10 use the increment filtration, the case needed for this theorem.

The paper's Lemma 2.2 needs a common initial value for its homogeneous-seminorm estimate; the formal statement includes it and records the printed issue. The paper writes the limiting coefficient with a time argument but uses an autonomous coefficient in (3.23), which the goal adopts. This proposal covers the dBdBdB equation. The final dtdtdt extension in Theorem 3.13 and the conditional-expectation estimate (3.19) remain outside its current items. Contributions that close these gaps, or supply a general conditional Wiener integral matching the article's notation, would extend the development.

Selected references

  • M. Hairer and X.-M. Li, Averaging dynamics driven by fractional Brownian motion, Annals of Probability 48(4), 2020, 1826–1860. DOI.
  • K. Lê, A stochastic sewing lemma and applications, 2018, arXiv:1810.10500, cited as [23] in Hairer and Li. arXiv.
9 thms1 active userReviewed
PreviousPage 2 of 4Next

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paper
SKILL.mdTourFAQContactTerms
© 2026 Prove2Me