Abstract
This Letter demonstrates for chaotic maps (logistic, classical and quantum standard maps (SMs)) that the exponential growth rate () of the out-of-time-ordered four-point correlator (OTOC) is equal to the classical Lyapunov exponent () \textit{plus} fluctuations ($Δ^{\mbox{\tiny (fluc)}}$) of the one-step finite-time Lyapunov exponents (FTLEs). Jensen's inequality provides the upper bound for the considered systems. Equality is restored with $Λ= λ+ Δ^{\mbox{\tiny (fluc)}}$, where $Δ^{\mbox{\tiny (fluc)}}$ is quantified by -higher-order cumulants of the FTLEs. Exact expressions for are derived and numerical results using furnish $Δ^{\mbox{\tiny (fluc)}} \sim\ln{(\sqrt{2})}$ for \textit{all maps} (large kicking intensities in the SMs).
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