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Local classical solutions of a kinetic equation for three waves interactions in presence of a Dirac measure at the origin

Miguel Escobedo

TL;DR

The paper proves the local-in-time existence of classical solutions for a coupled kinetic system describing wave turbulence fluctuations around an equilibrium of the 3-d cubic Schrödinger equation in the presence of a condensate. The authors develop a robust functional-analytic framework based on weighted spaces $X_{ heta, ho}$, establish regularizing semigroups for the linear operator $ ext{L}$, and carefully estimate the nonlinear terms $Q_N$ to enable a fixed-point construction. A key feature is the singular behavior of the wave density near the origin, modeled by a Rayleigh–Jeans-type profile, which induces a time-ascending condensate density $n( au)$ via a nonlinear flux mechanism; this is captured by an explicit relation $n( au)=n(0) ext{exp}ig( rac{ ext{pi}^2}{3} ext{∫} olimits_0^ au ar{ ext{λ}}^2(s) ext{d}sig)$. The results provide a rigorous foundation for the dynamics of condensates coupled to wave turbulence and establish a methodology for handling singular kernels in kinetic equations through Mellin-transform techniques and semigroup theory. The work yields local existence, conservation-type identities, and a detailed description of the small-$X$ behavior that is central to the condensate flux, with potential implications for boson gases and related kinetic models.

Abstract

The existence of local, classical solutions is proved, for a system of two coupled equations that describe, in the framework of the wave turbulence theory, the fluctuations around an equilibrium, of a system of nonlinear waves satisfying the 3-d cubic Schrödinger equation, weakly interacting in presence of a condensate. The function that describes the density of waves behaves like a singular Rayleigh Jeans equilibria near the origin, and induces a strictly increasing behavior in time of the function describing the condensate's density.

Local classical solutions of a kinetic equation for three waves interactions in presence of a Dirac measure at the origin

TL;DR

The paper proves the local-in-time existence of classical solutions for a coupled kinetic system describing wave turbulence fluctuations around an equilibrium of the 3-d cubic Schrödinger equation in the presence of a condensate. The authors develop a robust functional-analytic framework based on weighted spaces , establish regularizing semigroups for the linear operator , and carefully estimate the nonlinear terms to enable a fixed-point construction. A key feature is the singular behavior of the wave density near the origin, modeled by a Rayleigh–Jeans-type profile, which induces a time-ascending condensate density via a nonlinear flux mechanism; this is captured by an explicit relation . The results provide a rigorous foundation for the dynamics of condensates coupled to wave turbulence and establish a methodology for handling singular kernels in kinetic equations through Mellin-transform techniques and semigroup theory. The work yields local existence, conservation-type identities, and a detailed description of the small- behavior that is central to the condensate flux, with potential implications for boson gases and related kinetic models.

Abstract

The existence of local, classical solutions is proved, for a system of two coupled equations that describe, in the framework of the wave turbulence theory, the fluctuations around an equilibrium, of a system of nonlinear waves satisfying the 3-d cubic Schrödinger equation, weakly interacting in presence of a condensate. The function that describes the density of waves behaves like a singular Rayleigh Jeans equilibria near the origin, and induces a strictly increasing behavior in time of the function describing the condensate's density.
Paper Structure (29 sections, 29 theorems, 466 equations)

This paper contains 29 sections, 29 theorems, 466 equations.

Key Result

Theorem 1.1

For all $r\in [0, \frac{1}{2}), q\in [0, 3)$, there exists $R>0$, $T>0$, and two functions $(F, \lambda)$ satisfying $F\in C((0, T\times (0, \infty)$, $\lambda \in C([0, T))$, and such that $F$, together with the function $n$ defined as satisfy equation (S1E00) in $L _{ \text{loc} }^\infty([0, T); L^1 _{ \text{loc} }([0, \infty); XdX)$ and equation (S1E021) pointwise, for all $\tau \in (0, T)$.

Theorems & Definitions (53)

  • Theorem 1.1
  • Theorem 1.2
  • Remark 1.3: On the initial data
  • Remark 1.4: On regularity
  • Remark 1.5
  • Proposition 2.1
  • Proposition 2.2
  • Lemma 2.3
  • proof : Proof of Lemma \ref{['blabla']}
  • Proposition 2.4
  • ...and 43 more