2005
DOI: 10.4310/dpde.2005.v2.n1.a1
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Existence of KPP fronts in spatially-temporally periodic advection and variational principle for propagation speeds

Abstract: We prove the existence of Kolmogorov-Petrovsky-Piskunov (KPP) type traveling fronts in space-time periodic and mean zero incompressible advection, and establish a variational (minimization) formula for the minimal speeds. We approach the existence by considering limit of a sequence of front solutions to a regularized traveling front equation where the nonlinearity is combustion type with ignition cut-off. The limiting front equation is degenerate parabolic and does not permit strong solutions, however, the nec… Show more

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Cited by 94 publications
(109 citation statements)
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“…If the initial data for u is nonnegative and compactly supported, the large time behavior of u is an outward propagating front, with speed c * = c * ( e) in the direction e = 1, 0 . The variational principle of c * is [18]:…”
Section: Introductionmentioning
confidence: 99%
“…If the initial data for u is nonnegative and compactly supported, the large time behavior of u is an outward propagating front, with speed c * = c * ( e) in the direction e = 1, 0 . The variational principle of c * is [18]:…”
Section: Introductionmentioning
confidence: 99%
“…We refer to (Aronson & Weinberger, 1957;Aronson & Weinberger, 1978;Berestycki, Hamel, & Nadirashvili, 2010;Kametaka, 1976;Liang & Zhao, 2007;Liang, Yi, & Zhao, 2006;Sattinger, 1976;Uchiyama, 1978;Weinberger, 1982;etc). for the study of (1.2) in the case that f (x, u) is independent of x and refer to (Berestycki, Hamel, & Nadirashvili, 2005;Berestycki, Hamel, & Roques, 2005;Freidlin & Gärtner, 1979;Hamel, 2008;Hudson & Zinner, 1995;Nadin, 2009;Nolen, Rudd, & Xin, 2005;Weinberger, 2002;etc). for the study of (1.2) in the case that f (x, u) is periodic in x; refer to (Coville & Dupaigne, 2005;Coville, Dávila, & Martínez, 2008;Li, Sun, & Wang, 2010;etc).…”
Section: U(t Y)dy − U(t X) + U(t X) Fmentioning
confidence: 99%
“…Our proofs are built on his, with additional ingredients to handle both the time-dependence and the stochastic nature of the field B. For example, in the periodic case, µ(λ) is the principal eigenvalue of a periodic-parabolic operator [28,26], and perturbation theory [17] implies that µ(λ) is differentiable in λ. It then follows from Theorem 7.1.1 and Theorem 7.1.2 of [14] that the random variables η t z (t) satisfy a large deviation principle with convex rate function S(c) given by (4.3).…”
Section: A4mentioning
confidence: 99%
“…For compactly supported initial data bounded between 0 and 1, solutions of (1.1) develop into propagating fronts separating the cylindrical domain into a region where u ≈ 1 and the rest where u ≈ 0, which correspond to burned (hot) and unburned (cold) states in combustion. In case B is periodic in z and t, KPP type front dynamics and speeds have been recently studied for both shear and more general incompressible flows [20,22,23,27,28,26]. Exact traveling front solutions exist [27,28,26], extending those in spatially periodic media, [4,5,36,35], see also [3] and [37] for reviews.…”
Section: Introductionmentioning
confidence: 99%