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Furstenberg-Type Theorem: Non-Stationary Matrix Products

Updated 23 December 2025
  • The theorem extends classical Furstenberg results to non-stationary settings, analyzing asymptotic exponential growth in products of independent, non-identically distributed matrices.
  • It employs finite moment, no common invariant measure, and no finite-union-of-subspaces conditions to ensure effective mixing and exponential norm growth.
  • Sharp quantitative bounds and large deviation principles are derived, with applications ranging from Anderson localization to robust random dynamical systems.

A Furstenberg-type theorem for non-stationary matrix products concerns the almost-sure asymptotic behavior of random products of independent, not necessarily identically distributed, matrices. The theory extends the classical Furstenberg theorem—originally formulated for i.i.d. random matrices—to highly non-stationary sequences, encompassing arbitrary (possibly Markov-dependent) randomness, additive noise, and parameter families. The modern theory develops a framework for exponential norm growth, almost-sure approximation by deterministic sequences, large deviation principles, and spectral gap estimates, with sharp quantitative control under explicit irreducibility and moment conditions.

1. Genericity and Hypotheses for Non-stationary Products

Let KK be a compact set of probability measures on $\SL(d, \mathbb{R})$. Consider a sequence of independent random matrices AiμiA_i \sim \mu_i, where each μiK\mu_i \in K may vary with ii. The main Furstenberg-type results assert exponential behavior under three uniform “genericity” or non-degeneracy conditions (Gorodetski et al., 2022):

  1. Finite-moment condition: There exist γ>0\gamma>0, C<C < \infty such that

μK,SL(d,R)Aγdμ(A)C.\forall \mu \in K, \quad \int_{SL(d, \mathbb{R})} \|A\|^\gamma\, d\mu(A) \leq C.

This ensures bounded exponential moments for all μK\mu \in K.

  1. No common invariant measure: For every μK\mu \in K, no probability measures ν1,ν2\nu_1, \nu_2 on RPd1\mathbb{R}P^{d-1} satisfy (fA)ν1=ν2(f_A)_*\nu_1 = \nu_2 for μ\mu-almost every AA.
  2. No finite-union-of-subspaces invariance: For every μK\mu \in K, there is no pair of finite unions of proper subspaces U,URdU, U' \subset \mathbb{R}^d with A(U)=UA(U) = U' for μ\mu-almost every AA.

These hypotheses provide non-stationary analogues of Furstenberg’s strong irreducibility and proximality conditions, guaranteeing effective mixing on projective space and precluding algebraic obstructions to exponential growth.

2. Main Theorem and Quantitative Statements

Given the above data, the non-stationary Furstenberg theorem quantifies the almost-sure exponential growth of the product norm, and provides sharp large deviation control (Gorodetski et al., 2022):

  • Matrix products: Tn=AnA1T_n = A_n \cdots A_1.
  • Expectation sequence: Ln:=E[logTn]L_n := \mathbb{E}[ \log \|T_n\| ].

Theorem:

There exists λ>0\lambda > 0 such that for all nn and all sequences μiK\mu_i \in K,

Lnnλ.L_n \geq n \lambda.

Moreover, almost surely under the random matrix law, one has

limn1n(logTnLn)=0,\lim_{n \to \infty} \frac{1}{n} \Big(\log \|T_n\| - L_n\Big) = 0,

that is,

logTn=Ln+o(n).\log \|T_n\| = L_n + o(n).

Additionally, for every ε>0\varepsilon > 0 there exist δ(ε)>0\delta(\varepsilon)>0, C(ε)<C(\varepsilon)<\infty such that for all large nn,

P{logTnLn>εn}Ceδn,\mathbb{P}\left\{\, |\log \|T_n\| - L_n| > \varepsilon n\, \right\} \leq C e^{-\delta n},

with the same bound valid for any fixed vRdv \in \mathbb{R}^d.

This result applies to highly non-stationary settings and also admits substantially quantitative forms, including explicit large deviation rates that depend on γ\gamma and block size (Gorodetski et al., 2022). The theory extends to Markov-dependent sequences, with appropriate spectral gap and non-degeneracy requirements (Goldsheid, 2020).

3. Probabilistic and Structural Tools

The proofs exploit probabilistic block decompositions, entropy additivity, and fine control of projective measures:

  • Key sequences:

For a block-length k1k \gg 1, set Bj=AjkA(j1)k+1B_j = A_{jk}\cdots A_{(j-1)k+1} (so that Tmk=BmB1T_{mk} = B_m \cdots B_1). Define ξj=logBj\xi_j = \log \|B_j\|, Rj=logBjlogBjvj1R_j = \log \|B_j\| - \log |B_j v_{j-1}|, and recursively normalize vjv_j as vj=Bjvj1/Bjvj1v_j = B_j v_{j-1}/|B_j v_{j-1}|. Then

logTmk=j=1mξjj=1mRj.\log \|T_{mk}\| = \sum_{j=1}^m \xi_j - \sum_{j=1}^m R_j.

The ξj\xi_j are i.i.d. (in blocks), and possess uniform exponential moments.

  • Atom-dissolving and subspace-avoidance:

The atom-dissolving theorem asserts that under the genericity conditions, the largest atomic weight in any convolution on RPd1\mathbb{R}P^{d-1} decays exponentially, ensuring that projective randomness spreads effectively (Gorodetski et al., 2022). This controls the RjR_j correction terms and eliminates the effect of initial alignment (subspace trapping) in the norm.

  • Entropy additivity and Furstenberg entropy:

The lower bound LnnλL_n \geq n\lambda is proved using a non-stationary additivity property of Furstenberg (Kullback–Leibler) entropy, which quantifies the exponential contraction in projective space under non-degenerate convolutions.

  • Large deviation principles:

Blockwise i.i.d. structure, subadditivity, and exponential moment control allow application of Chernoff bounds and classical large deviations to the sums jξj\sum_j \xi_j, with all error terms dominated for suitable block size.

A schematic of the block decomposition and error control employed in the proof is as follows:

Term Role Estimate/Method
ξj\sum \xi_j Leading exponential sum i.i.d., Chernoff/LDP
Rj\sum R_j Misalignment penalty Atom-dissolving
Blocks Sufficient mixing in each block Quantitative bounds

4. Extensions: Markov Dependence, Additive Noise, and Parameter Families

The non-stationary framework generalizes to several advanced contexts:

  • Non-stationary Markov chains:

In (Goldsheid, 2020), for matrix products Sn=GnGn1G1S_n = G_n G_{n-1} \cdots G_1 where each GnG_n depends Markovly on a time-inhomogeneous chain, exponential norm growth is proved under a spectral gap for the chain and uniform non-degeneracy for the associated Furstenberg group. The proof uses operator-theoretic contractions on X×Sm1X \times S^{m-1}, quantifying failure of projective invariance.

  • Additive small noise:

(Bednarski et al., 5 Jul 2025) establishes quantitative Furstenberg-type singular value separation for non-stationary products Bn=i=1n(Ai+ϵEi)B^n = \prod_{i=1}^n (A_i + \epsilon E_i), where AiA_i are bounded, deterministic matrices and EiE_i are i.i.d. noise with absolutely continuous law. The gap between log-singular values grows linearly in nn at rate Θ(ϵ2n)\Theta(\epsilon^2 n), with explicit entropy-based lower bounds.

  • Parameter-dependent products and Anderson localization:

(Gorodetski et al., 24 Mar 2024, Zieber, 20 Dec 2025) show continuity and positivity of parameter-dependent Lyapunov exponents associated to Schrödinger cocycles with independent, non-identically distributed random potentials. Large deviation estimates and Hölder continuity in the spectral parameter establish spectral and dynamical localization.

  • Nonconventional (long-range) products:

(Kifer et al., 2018) handles products Xn=F(ξq1(n),,ξq(n))X_n = F(\xi_{q_1(n)}, \dots, \xi_{q_\ell(n)}) for (possibly) Markov, long-range dependent ξi\xi_i and arbitrary time-shifts qj(n)q_j(n). Subadditive ergodic theorem and large deviation methods ensure existence of Lyapunov exponents as long as the Markov chain of Ξn\Xi_n is time-homogeneous (linear shifts), under strong irreducibility and proximality.

5. Topological and Ergodic Generalizations

A topological version of the Furstenberg–Kesten theorem for matrix cocycles (A(ω))(A(\omega)) over ergodic, non-stationary dynamical bases is established in (Fan et al., 2022). Given any continuous cocycle A:ΩMd(R0)A: \Omega \to M_d(\mathbb{R}_{\geq 0}) over a subshift (Ω,σ)(\Omega, \sigma) and an ergodic measure ν\nu, if there are uniform positivity blocks and lower bounds on matrix entries, then for ν\nu-generic points ω\omega,

λ(ω)=limn1nlogA(ω)A(σn1ω)\lambda(\omega) = \lim_{n\to\infty} \frac{1}{n} \log \|A(\omega) \cdots A(\sigma^{n-1} \omega)\|

exists and equals the space average except in the exceptional case of finite-time vanishing. This result highlights the role of orbit decomposition, local Kingman subadditivity, and quasi-multiplicativity from cone contraction rather than invertibility.

Applications include weighted ergodic averages, unique ergodicity scenarios, and analytic dependence in parameter families, unifying probabilistic and topological aspects of random matrix product theory.

6. Applications and Impact

Furstenberg-type theorems for non-stationary matrix products underlie rigorous analysis in several areas:

  • Spectral and dynamical localization: Control of Lyapunov exponents for general random Schrödinger operators under minimal stationarity assumptions yields Anderson localization, dynamical localization, and sharp exponential localization of eigenfunctions (Gorodetski et al., 24 Mar 2024, Zieber, 20 Dec 2025).
  • Robustness to dependence and inhomogeneity: Exponential growth persists under non-stationarity, inhomogeneous Markov dependence, or long-range dependencies as long as explicit irreducibility, moment, and mixing properties are maintained (Goldsheid, 2020, Kifer et al., 2018).
  • Separation of Lyapunov exponents: Quantitative, entropy-based results give order-ϵ2n\epsilon^2 n separation between the log-singular values of noisy matrix products, directly generalizing classical multiplicative ergodic theorems to non-stationary, non-elliptic regimes (Bednarski et al., 5 Jul 2025).
  • Topological dynamical systems: Existence of Lyapunov exponents, large deviation principles, and variational formulas extend to continuous matrix cocycles over non-stationary subshifts (Fan et al., 2022).

The non-stationary theory thus provides a comprehensive quantitative framework that supports a variety of localization and stability phenomena, with broad applicability in random dynamical systems, random operators, and ergodic theory.

7. Table: Summary of Principal Non-stationary Furstenberg-type Theorems

Setting Key Hypotheses Main Result/Behavior
Arbitrary i.i.d. sequence Moment, non-degeneracy/irreducibility logTn=Ln+o(n)\log\|T_n\| = L_n + o(n), Tneλn\|T_n\| \gtrsim e^{\lambda n} (Gorodetski et al., 2022)
Markov-dependent Uniform spectral gap, Furstenberg group non-deg. Exponential norm growth, robust to non-stationarity (Goldsheid, 2020)
Additive noise Compactly supported, smooth noise law Singular value gaps ϵ2n\sim \epsilon^2 n (Bednarski et al., 5 Jul 2025)
Parameter cocycle Uniform moment, Furstenberg-type irreducibility Continuity/positivity of Lyapunov exponent (localization) (Gorodetski et al., 24 Mar 2024, Zieber, 20 Dec 2025)
Topological subshift Cone-contraction, positivity, ergodicity Existence of limnn1logA(n)(ω)\lim_n n^{-1}\log\|A^{(n)}(\omega)\| (Fan et al., 2022)
Nonconventional (long-range) Homogeneity, strong irred./proximality n1logΠnλn^{-1}\log\|\Pi_n\| \to \lambda a.s. (Kifer et al., 2018)

In all these regimes, the non-stationary theory recovers and extends the classical exponential growth law, with explicit quantification and robust error bounds. The key ingredients—irreducibility, finite moment, and entropy or atom-dissolving techniques—enable transfer of much of the stationary random matrix product theory to highly non-homogeneous settings.

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