A Macroscopic Multifractal Analysis of Parabolic Stochastic PDEs

It is generally argued that the solution to a stochastic PDE with multiplicative noise—such as u ˙ = 1 2 u ′ ′ + u ξ , where ξ denotes space-time white noise—routinely produces exceptionally-large peaks that are “macroscopically multifractal.” See, for example, Gibbon and Doering (Arch Ration Mech A...

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Veröffentlicht in:Communications in mathematical physics 2018-05, Vol.360 (1), p.307-346
Hauptverfasser: Khoshnevisan, Davar, Kim, Kunwoo, Xiao, Yimin
Format: Artikel
Sprache:eng
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Zusammenfassung:It is generally argued that the solution to a stochastic PDE with multiplicative noise—such as u ˙ = 1 2 u ′ ′ + u ξ , where ξ denotes space-time white noise—routinely produces exceptionally-large peaks that are “macroscopically multifractal.” See, for example, Gibbon and Doering (Arch Ration Mech Anal 177:115–150, 2005 ), Gibbon and Titi (Proc R Soc A 461:3089–3097, 2005 ), and Zimmermann et al. (Phys Rev Lett 85(17):3612–3615, 2000 ). A few years ago, we proved that the spatial peaks of the solution to the mentioned stochastic PDE indeed form a random multifractal in the macroscopic sense of Barlow and Taylor (J Phys A 22(13):2621–2626, 1989 ; Proc Lond Math Soc (3) 64:125–152, 1992 ). The main result of the present paper is a proof of a rigorous formulation of the assertion that the spatio-temporal peaks of the solution form infinitely-many different multifractals on infinitely-many different scales, which we sometimes refer to as “stretch factors.” A simpler, though still complex, such structure is shown to also exist for the constant-coefficient version of the said stochastic PDE.
ISSN:0010-3616
1432-0916
DOI:10.1007/s00220-018-3136-6