Abstract

Starting from action-angle variables and using a standard asymptotic expansion, we present an original and coincise derivation of the Wave Kinetic equation for a resonant process of the type . Despite not being more rigorous than others, our procedure has the merit of being straightforward; it allows for a direct control of the random phases and random action of the initial wave field. We show that the Wave Kinetic equation can be derived assuming only initial random phases. The random action approximation has to be taken only after the weak nonlinearity and large box limits are taken. The reason is that the oscillating terms in the evolution equation for the action contain, as an argument, the action-dependent nonlinear corrections which is dropped, using the large box limit. We also show that a discrete version of the Wave Kinetic Equation can be obtained for the Nonlinear Schrödinger equation; this is because the nonlinear frequency correction terms give a zero contribution and the large box limit is not needed. In our calculation we do not make an explicitly use of the Wick selection rule.

Highlights

  • To cite this article: M Onorato and G Dematteis 2020 J

  • We show that the Wave Kinetic equation can be derived assuming only initial random and DOI

  • We show that a discrete version of the Wave Kinetic Equation can be obtained for the Nonlinear Schrödinger equation; this is because the nonlinear frequency correction terms give a zero contribution and the large box limit is not needed

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Summary

September 2020

A straightforward derivation of the four-wave kinetic equation in action-angle variables. Our derivation does not pretend to be more rigorous than the existing ones; according to us, it has the merit of being straightforward It is based on a direct expansion of the variables angle and action in powers of the small parameter in front of the interaction Hamiltonian. It turns out that the phase average has to be taken before the action one; a consistent action average procedure can only be taken after the large box limit: this is because the nonlinear, amplitude dependent, frequency shift is contained as an argument of oscillating functions that appear in the equation for the amplitudes. Despite the quite large literature on the subject, we feel that a didactic derivation of the four-wave kinetic equation is still lacking and we hope that newcomers in the field may benefit from our approach

The hamiltonian model
The ò-expansion
Averaging over initial angles: the discrete wave kinetic equation
The thermodynamic limit: the standard wave kinetic equation
Conclusions
Full Text
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