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 |
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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. |
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ISSN: | 0010-3616 1432-0916 |
DOI: | 10.1007/s00220-018-3136-6 |