- Photon Transport in a Bose-Hubbard Chain of Superconducting Artificial Atoms

G. P. Fedorov et al., Phys. Rev. Lett.**126**, 180503 (2021) - Path-Dependent Supercooling of the
He3 Superfluid A-B Transition

Dmytro Lotnyk et al., Phys. Rev. Lett.**126**, 215301 (2021) - Superconductivity in an extreme strange metal

D. H. Nguyen et al., Nat Commun**12**, 4341 (2021) - High-Q Silicon Nitride Drum Resonators Strongly Coupled to Gates

Xin Zhou et al., Nano Lett.**21**, 5738-5744 (2021) - Measurement of the
^{229}Th isomer energy with a magnetic micro-calorimeter

T. Sikorsky et al., Phys. Rev. Lett.**125**(2020) 142503

## Discrete and mesoscopic regimes of finite-size wave turbulence

*V. S. L’vov and S. Nazarenko*

Bounding volume results in discreteness of eigenmodes in wave systems. This leads to a depletion or complete loss of wave resonances (three-wave, four-wave, etc.), which has a strong effect on *wave turbulence* (WT) i.e., on the statistical behavior of broadband sets of weakly nonlinear waves. This paper describes three different regimes of WT realizable for different levels of the wave excitations: *discrete, mesoscopic and kinetic WT*. *Discrete WT* comprises chaotic dynamics of interacting wave “clusters” consisting of discrete (often finite) number of connected resonant wave triads (or quarters). *Kinetic WT* refers to the infinite-box theory, described by well-known wave-kinetic equations. *Mesoscopic WT* is a regime in which either the discrete and the kinetic evolutions alternate or when none of these two types is purely realized. We argue that in mesoscopic systems the wave spectrum experiences a *sandpile* behavior. Importantly, the mesoscopic regime is realized for a *broad range* of wave amplitudes which typically spans over several orders on magnitude, and not just for a particular intermediate level.

*Phys. Rev. E*

**82**, 056322 (2010)doi:

*10.1103/PhysRevE.82.056322*