We investigate the dynamics of the Fermi-Pasta-Ulam-Tsingou chain with long-wavelength random initial data. When the energy per particle is small, thermal equilibrium is not reached on a fast timescale, and the system enters prethermalization. The formation of the prethermal state is characterized by the development of a Burgers-type shock and the onset of a turbulentlike spectrum with a time dependent exponent zeta(t) in the inertial range. We perform a significant step forward by demonstrating that these features are robust under generic long-wavelength random initial conditions. By employing advanced probabilistic techniques inspired by the works of Dudley and Talagrand, we derive a sharp asymptotic expression for the average shock time in the thermodynamic limit. For large p, this time scales as (p ffiffiffiffiffiffiffiffiffiffi plog p)-1, where p is the number of excited modes, proving that it is an intensive quantity up to a logarithmic correction in the size of the system.
Random Initial Data and Average Shock Time in the Fermi-Pasta-Ulam-Tsingou Chain / Gallone, M., Grande, R., Ponno, A., Ruffo, S., Druais, E.. - In: PHYSICAL REVIEW LETTERS. - ISSN 0031-9007. - 136:21(2026). [10.1103/qxzs-1t1l]
Random Initial Data and Average Shock Time in the Fermi-Pasta-Ulam-Tsingou Chain
Gallone, Matteo
;Grande, Ricardo;Ponno, Antonio;Ruffo, Stefano;
2026-01-01
Abstract
We investigate the dynamics of the Fermi-Pasta-Ulam-Tsingou chain with long-wavelength random initial data. When the energy per particle is small, thermal equilibrium is not reached on a fast timescale, and the system enters prethermalization. The formation of the prethermal state is characterized by the development of a Burgers-type shock and the onset of a turbulentlike spectrum with a time dependent exponent zeta(t) in the inertial range. We perform a significant step forward by demonstrating that these features are robust under generic long-wavelength random initial conditions. By employing advanced probabilistic techniques inspired by the works of Dudley and Talagrand, we derive a sharp asymptotic expression for the average shock time in the thermodynamic limit. For large p, this time scales as (p ffiffiffiffiffiffiffiffiffiffi plog p)-1, where p is the number of excited modes, proving that it is an intensive quantity up to a logarithmic correction in the size of the system.| File | Dimensione | Formato | |
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