The emergence of heavy-tailed statistics in complex systems is conventionally attributed to nonlocal stochastic jumps or non-Markovian memory. Here, we present a one-dimensional random walk where power-law behaviors arise instead from a strictly local, discrete-time Markovian mechanism. The step length is governed by a deterministic function of the walker's position, establishing a positive feedback loop that induces strong effective correlations along the trajectories. Through analytical derivations in the continuum limit and extensive numerical simulations, we show that this rule yields a robust, non-Gaussian stationary state. The exact analytical solution is obtained in the closed form of a symmetric, Lorentz-like distribution ${\rho }_{\text{st}}\left(x\right)\propto {\left(\right|x|/l+r\mathrm{\Delta }x)}^{-2}$, confirming asymptotic power-law tails that decay as ${\left|x\right|}^{-2}$ over six decades. Furthermore, by employing the Onsager-Machlup path-integral formalism, we demonstrate that effective velocity and acceleration acquire physical meaning along the shortest fluctuation trajectories. Crucially, we find that a nonzero initial acceleration acts as the fundamental mechanism driving the walker away from the origin, ensuring both the emergence of scale-free statistics and the normalizability of the stationary distribution. This minimal pathway provides a microscopic foundation for the widespread $-2$ power law observed across multidisciplinary complex systems.

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• Anomalous diffusion
• Complex systems
• Diffusion
• Fluctuations & noise
• Stochastic processes