The Tremor of Predictions: How Energy Dissipation Calms Randomness ✎

Original: "Universal thermokinetic decomposition of short-time information fluctuations"
arXiv:2605.29957 · 2026-05-28 · arXiv non-exclusive · independent analysis · 2 min
Energy expenditure does not make the future more certain on average, but it does dampen the spread of predictions along each trajectory.

A shooter at the firing line fires a series of shots. The average point of impact stays the same, but the spread of the bullet holes changes depending on how much the hands tremble. In the world of random processes, fluctuations play the role of the tremor, and dissipation, that is, energy loss, plays the role of the calmer.

Researchers considered an arbitrary stochastic system, where the future state depends on the current one only with some probability. For each pair of states, one can compute the "pointwise mutual information": a measure of how well one state predicts another. It turned out that the average predictability does not depend on thermodynamic characteristics: it is determined only by the stationary distribution and the noise intensity. However, the variance of this predictability, that is, its spread along a trajectory, obeys a universal decomposition.

The variance of predictability is made up of three contributions: noise, geometric, and thermokinetic. Dissipation enters with a negative sign, while dynamical activity enters with a positive one.

In linear systems, these two contributions exactly cancel each other, so energy cannot influence fluctuations. Only nonlinear forces allow dissipation to suppress the spread. Using the example of a Brownian motor on a ring, it is clear that as the nonequilibrium force increases, the fluctuations of predictability decrease monotonically and approach a lower bound set only by noise. For the Stuart-Landau stochastic oscillator, it was found that short-time accuracy and long-time coherence are governed by different mechanisms: angular velocity affects only coherence, while radial dissipation affects only fluctuations.

In linear systems, dissipation and dynamical activity always cancel each other, so fluctuations of predictability do not depend on nonequilibriumness. Only nonlinear forces allow energy to influence the reliability of information transfer.

The work shifts the focus from average quantities to fluctuations, showing that the thermodynamic signature manifests precisely in them. This is the first universal decomposition for the variance of predictability, valid for any Langevin dynamics. The result changes the understanding of the role of dissipation: it does not create information but stabilizes its transfer, reducing the spread of predictability along a trajectory.

Now the shooter understands that the calmer does not shift the average point of impact but only reduces the tremor of the hands. In cellular sensors and control systems, this means that energy expenditure may not increase accuracy on average, but it makes accuracy more stable from attempt to attempt.

In linear systems, dissipation and dynamic activity always cancel each other, so fluctuations in predictability do not depend on how far from equilibrium the system is. Only nonlinear forces allow energy to influence the reliability of information transfer.

F_\tau = \frac{N}{2} + F_H[-\log p_{st}] - 2\tau(\Sigma - 4T)
Fluctuations in predictability equal the sum of the noise contribution (N/2), the geometric contribution (varientropy of the stationary distribution), and the thermokinetic contribution, where dissipation (Σ) suppresses and traffic (T) amplifies the fluctuations.
\Sigma = \int dx \frac{J_{st}(x)^T D^{-1} J_{st}(x)}{p_{st}(x)}
A measure of the irreversibility of the process, determined by the stationary probability flux and the diffusion matrix.
T = \frac{1}{4} \int dx \, p_{st}(x) F(x)^T D^{-1} F(x) + \frac{1}{2} \int dx \, p_{st}(x) \nabla \cdot F(x)
A measure of the frequency and speed of transitions regardless of their direction; it reflects the kinetic activity of the system.
Concepts
fluctuation-dissipation theorem information thermodynamics natural variability information theory heat heat dissipation second law of thermodynamics Boltzmann equation Landauer's principle stochastic self organization random fluctuation stochastic dynamical system efficiency energy distribution data transmission Dynamical Systems climate network energy conservation data compression fluctuation