2017
DOI: 10.1016/j.jmaa.2016.10.037
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Large time behavior of solutions for degenerate p-degree Fisher equation with algebraic decaying initial data

Abstract: This paper is concerned with the large time behavior of solutions to the onedimensional degenerate p-degree Fisher equation, where the initial data are assumed to be asymptotically front-like and to decay to zero non-exponentially at one end. By applying sub-super solution method we first prove the Lyapunov stability of all the wave fronts with noncritical speeds in some polynomially weighted space. Further, by using semigroup estimates, sub-super solution method and the nonlinear stability of the traveling wa… Show more

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Cited by 13 publications
(3 citation statements)
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“…By (1.8), the explicit upper and lower bounds locating Eω(t)$E_\omega (t)$ were obtained in [18] for different forms of u0$u_0$, for example, if u0(x)=Cxp$u_0(x)=C x^{-p}$ for large x$x$ with p,C>0$p,C>0$, then ln(minEωfalse(tfalse))ln(maxEωfalse(tfalse))ap1t3.33333ptas3.33333ptt+$\ln (\min E_\omega (t))\sim \ln (\max E_\omega (t))\sim ap^{-1}t\nobreakspace \text{as}\nobreakspace t\rightarrow +\infty$. We refer to [3, 19, 20] for the acceleration propagation results recently developed for more general reaction–diffusion equations. We also refer to [9, 11, 13] for the acceleration propagation of fractional diffusion equations and [4, 14, 15] for non‐local dispersal equations.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…By (1.8), the explicit upper and lower bounds locating Eω(t)$E_\omega (t)$ were obtained in [18] for different forms of u0$u_0$, for example, if u0(x)=Cxp$u_0(x)=C x^{-p}$ for large x$x$ with p,C>0$p,C>0$, then ln(minEωfalse(tfalse))ln(maxEωfalse(tfalse))ap1t3.33333ptas3.33333ptt+$\ln (\min E_\omega (t))\sim \ln (\max E_\omega (t))\sim ap^{-1}t\nobreakspace \text{as}\nobreakspace t\rightarrow +\infty$. We refer to [3, 19, 20] for the acceleration propagation results recently developed for more general reaction–diffusion equations. We also refer to [9, 11, 13] for the acceleration propagation of fractional diffusion equations and [4, 14, 15] for non‐local dispersal equations.…”
Section: Introductionmentioning
confidence: 99%
“…By (1.8), the explicit upper and lower bounds locating 𝐸 𝜔 (𝑡) were obtained in [18] for different forms of 𝑢 0 , for example, if 𝑢 0 (𝑥) = 𝐶𝑥 −𝑝 for large 𝑥 with 𝑝, 𝐶 > 0, then ln(min 𝐸 𝜔 (𝑡)) ∼ ln(max 𝐸 𝜔 (𝑡)) ∼ 𝑎𝑝 −1 𝑡 as 𝑡 → +∞. We refer to [3,19,20] for the acceleration propagation results recently developed for more general reaction-diffusion equations. We also refer to [9,11,13] for the acceleration propagation of fractional diffusion equations and [4,14,15] for non-local dispersal equations.…”
mentioning
confidence: 99%
“…where u −1 0 {A} = {x ∈ R, u 0 (x) ∈ A} denotes the inverse image of u 0 from the set A. We refer to [3,19,20] for the acceleration propagation results recently developed for more general reaction-diffusion equations. We also refer to [9,11,13] for the acceleration propagation in fractional diffusion equations and [4,14,15] for nonlocal dispersal equations.…”
Section: Introductionmentioning
confidence: 99%