Planckian bound for thermalization

Consider a quantum thermalization process that, for a set of distinct Hamiltonians, prepares states close to the corresponding thermal ensembles at temperature TT. The Planckian thermalization problem asks whether there is a universal lower bound on the thermalization time τ\tau, independent of the details of the system, namely τ≥τPl2=ℏ2kBT\tau\geq \frac{\tau_{\mathrm{Pl}}}{2}=\frac{\hbar}{2k_{\mathrm{B}}T}. In the low-temperature regime, where the relevant energy scale is the spectral gap Δ\Delta between the ground and first excited states, the corresponding bound is τ≥ℏΔ\tau\geq \frac{\hbar}{\Delta}; the regimes are characterized by βΔ≲1\beta\Delta\lesssim 1 and βΔ≫1\beta\Delta\gg 1, respectively, with β=(kBT)−1\beta=(k_{\mathrm{B}}T)^{-1}.

References

Primary source

Nature Physics

Additional references

Progress summary

Refreshed
Claimed solved

A 2025 paper claims to prove a universal lower limit on how quickly systems can reach thermal equilibrium, with a different limit at very low temperature.

The problem concerns a general lower bound on thermalization time. Abiuso, Rolandi, Calsamiglia, Sekatski, and Perarnau-Llobet claim an information-theoretic derivation in a June 2025 preprint.

Information-theoretic proof, June 2025

The authors claim that, for their operational notion of thermalization, τ≥τPl/2\tau \ge \tau_{\rm Pl}/2 when βΔ≲1\beta\Delta\lesssim 1, with τPl=ℏ/(kBT)\tau_{\rm Pl}=\hbar/(k_{\rm B}T), and τ≥ℏ/Δ\tau\ge\hbar/\Delta when βΔ≫1\beta\Delta\gg 1. The argument uses Hamiltonian estimation, quantum information geometry, and metrology, and connects the bound to the adiabatic theorem. The claim is reported in a Nature Physics article but remains unverified here.

Current status (as of September 2026): The operational thermalization bound is claimed in a preprint and Nature Physics article, while broader interpretations of a universal Planckian timescale and independent verification remain open.

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