Statement

Let TT be an invertible transformation of a and let A:X→GLd(R)A:X\to GL_d(\mathbb R) be measurable with

log⁡+∥A∥, log⁡+∥A−1∥∈L1,log⁡+t=max⁡(0,log⁡t).\log^+\|A\|,\ \log^+\|A^{-1}\|\in L^1, \qquad\log^+t=\max(0,\log t).

There are real numbers λ1>⋯>λr\lambda_1>\cdots>\lambda_r and, on an invariant conull set, a measurable direct sum

Rd=E1(x)⊕⋯⊕Er(x),A(x)Ei(x)=Ei(Tx),\mathbb R^d=E_1(x)\oplus\cdots\oplus E_r(x),\qquad A(x)E_i(x)=E_i(Tx),

such that for every nonzero v∈Ei(x)v\in E_i(x),

lim⁡n→±∞1nlog⁡∥A(n)(x)v∥=λi.\lim_{n\to\pm\infty}\frac1n\log\|A^{(n)}(x)v\|=\lambda_i.

This is the invertible finite-dimensional form of the multiplicative ergodic theorem.

Applications and hypotheses

The theorem makes Lyapunov exponents and invariant growth directions available in smooth dynamics and random matrix products. Integrability of the inverse is used for the two-sided finite-exponent splitting stated here. Versions with weaker assumptions give filtrations or allow infinite exponents.

References
  1. Simion Filip, Notes on the Multiplicative Ergodic Theorem, Theorem 2.2.6 and Variant 2.2.10.