Abstract

We report an exact unique constant-flux power-law analytical solution of the wave kinetic equation for the turbulent energy spectrum, E(k)=C1ε acs/kE(k)=C_1 \sqrt{\varepsilon\, a c_{\rm s} }/k, of acoustic waves in 2D with almost linear dispersion law, ωk=csk[1+(ak)2]ω_k = c_{\rm s} k[1+(ak)^2], ak≪1 ak \ll 1. Here ε\varepsilon is the energy flux over scales, and C1C_1 is the universal constant which was found analytically. Our theory describes, for example, acoustic turbulence in 2D Bose-Einstein condensates (BECs). The corresponding 3D counterpart of turbulent acoustic spectrum was found over half a century ago, however, due to the singularity in 2D, no solution has been obtained until now. We show the spectrum E(k)E(k) is realizable in direct numerical simulations of forced-dissipated Gross-Pitaevskii equation in the presence of strong condensate.

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