We introduce non-trivial contributions to diffusion constant in generic many-body systems arising from quadratic fluctuations of ballistically propagating, i.e. convective, modes. Our result is obtained by expanding the current operator in the vicinity of equilibrium states in terms of powers of local and quasi-local conserved quantities. We show that only the second-order terms in this expansion carry a finite contribution to diffusive spreading. Our formalism implies that whenever there are at least two coupled modes with degenerate group velocities, the system behaves super-diffusively, in accordance with the non-linear fluctuating hydrodynamics theory. Finally, we show that our expression saturates the exact diffusion constants in quantum and classical interacting integrable systems, providing a general framework to derive these expressions.
Cited by 3
Rebekka Koch et al., Adiabatic formation of bound states in the one-dimensional Bose gas
Phys. Rev. B 103, 165121 (2021) [Crossref]
Javier Lopez-Piqueres et al., Hydrodynamics of nonintegrable systems from a relaxation-time approximation
Phys. Rev. B 103, L060302 (2021) [Crossref]
Marko Medenjak et al., Thermal transport in
-deformed conformal field theories: From integrability to holography
Phys. Rev. D 103, 066012 (2021) [Crossref]
Authors / Affiliations: mappings to Contributors and OrganizationsSee all Organizations.
- 1 École Normale Supérieure [ENS]
- 2 Universiteit Gent / Ghent University
- 3 King's College London [KCL]
- Fonds Wetenschappelijk Onderzoek (FWO) (through Organization: Fonds voor Wetenschappelijk Onderzoek - Vlaanderen / Research Foundation - Flanders [FWO])
- 東京工業大学 / Tokyo Institute of Technology [TIT]