2019
DOI: 10.48550/arxiv.1907.02279
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Formal expansions in stochastic model for wave turbulence 2: method of diagram decomposition (complete version)

Abstract: We continue the study of small amplitude solutions of the damped/driven cubic NLS equation, written as formal series in the amplitude, initiated in our previous work [2]. As in [2], we are interested in behaviour of the formal series under the wave turbulence limit "the amplitude goes to zero, while the space-period goes to infinity".

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Cited by 15 publications
(45 citation statements)
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References 9 publications
(30 reference statements)
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“…The proof of Theorems 1.2, 1.3 and 1.4 are based on the framework introduced in [9] to prove Theorem 1.1. The latter work came as a culmination of an extensive research effort over the past years to provide a rigorous justification of the wave kinetic equation starting from the corresponding nonlinear dispersive PDE as a first principle [21,3,14,11,12,13,8,6,7]. This is Hilbert's sixth problem for waves; its particle analog is the rigorous derivation of the Boltzmann equation from Newtonian mechanics (see [17,20,15] and references therein).…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…The proof of Theorems 1.2, 1.3 and 1.4 are based on the framework introduced in [9] to prove Theorem 1.1. The latter work came as a culmination of an extensive research effort over the past years to provide a rigorous justification of the wave kinetic equation starting from the corresponding nonlinear dispersive PDE as a first principle [21,3,14,11,12,13,8,6,7]. This is Hilbert's sixth problem for waves; its particle analog is the rigorous derivation of the Boltzmann equation from Newtonian mechanics (see [17,20,15] and references therein).…”
mentioning
confidence: 99%
“…Note that the works [3,6,7,8,9,11,12,13,21] concern cubic nonlinearities or 4-wave interactions, while the works [1,14,26] concern quadratic nonlinearities or 3-wave interactions. Both models represent a lot of important physical scenarios.…”
mentioning
confidence: 99%
“…T d ds |s − x| d+2α−2 (∆ s g)(t, x, s, r, v, r, ṽ) = c β,d g(t, x, r, v) dr dṽ (r − r)(−∆ x ) α g(t, x, r, ṽ) =: −1 d,α Σ g (t, x, r) g(t, x, r, v) , and deduce from (39) the Vlasov-type equation ∂ t g(t, x, r, v) + v∂ r g(t, x, r, v) + C 1 [g, g](t, x, r, v) = 0, (…”
Section: Collective Behavior Kinetic Models Of Discrete Non-local Wav...mentioning
confidence: 84%
“…During the last few years, there has been a growing interests in rigorously understanding those kinetic equations. Starting with the pioneering work of Lukkarinen and Spohn [63], there have been a lot of recent works in in rigorously deriving WK equations (see, for instance [5,18,19,25,26,34,35,38,39,40,41,79] and the references therein). The analysis of WK and QK equations is also a topic of current interest.…”
Section: Introductionmentioning
confidence: 99%
“…In addition, to tackle the long standing open conjecture about the long time behavior of high Sobolev norms H s ps ą 1q of solutions of dispersive equations on the torus, discussed in the works of Bourgain [1] and Colliander, Staffilani, Keel, Takaoka, Tao [8], the rigorous justification of wave turbulence theory has been revisited during the last few years in [2,6,7,9,10,15,16,17,18,19,20,22,26,27,48].…”
Section: Introductionmentioning
confidence: 99%