Abstract
We show that in generic one-dimensional Hamiltonian lattices the diffusion coefficient of the maximum Lyapunov exponent diverges in the thermodynamic limit. We trace this back to the long-range correlations associated with the evolution of the hydrodynamic modes. In the case of normal heat transport, the divergence is even stronger, leading to the breakdown of the usual single-function Family-Vicsek scaling ansatz. A similar scenario is expected to arise in the evolution of rough interfaces in the presence of a suitably correlated background noise.
| Original language | English |
|---|---|
| Article number | 034101 |
| Pages (from-to) | 1-5 |
| Number of pages | 5 |
| Journal | Physical Review Letters |
| Volume | 117 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 14 Jul 2016 |
Bibliographical note
D. P. acknowledges support by MINECO (Spain) under a Ramón y Cajal fellowship. We acknowledge support by MINECO (Spain) under Project No. FIS2014-59462-P.Fingerprint
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