The forward Koopman operator of a TT is

UT:L2(X,μ)⟶L2(X,μ),UTf=f∘T.U_T:L^2(X,\mu)\longrightarrow L^2(X,\mu),\qquad U_Tf=f\circ T.

It is a linear isometry. If TT is invertible modulo null sets, it is , with UT−1f=f∘T−1U_T^{-1}f=f\circ T^{-1}.

Verification

Measure preservation gives ∥UTf∥22=∫∣f∣2∘T dμ=∥f∥22\|U_Tf\|_2^2=\int|f|^2\circ T\,d\mu=\|f\|_2^2. It also sends equality almost everywhere to equality almost everywhere, so the formula is independent of representatives. Composition respects linear combinations of functions without requiring any linear structure on XX.

Direction of time

This convention gives UTnf=f∘TnU_T^nf=f\circ T^n, as in time averages. For the left action n↦Tnn\mapsto T^n, the instead has κ(n)=UT−n\kappa(n)=U_T^{-n}. Under noncommuting transformations, forward pullback reverses composition order.

Noninvertible example

For the doubling map, UTek=e2kU_T e_k=e_{2k}. Odd Fourier frequencies are absent from its range. Thus it is an isometry that is not onto, and its nonnegative powers do not extend to a unitary representation of Z\mathbb Z.

References
  1. Jesse Peterson, Lecture notes on ergodic theory, 2011. §2.2.