activity
20182020
most citedPopulation dynamics in river networks

59 citations · 59 across the 2 of their papers we have counts for

collaborators

8 papers

math.AP2020

Propagation dynamics of a reaction-diffusion equation in a time-periodic shifting environment

Jian Fang, Rui Peng, Xiao-Qiang Zhao

This paper concerns the nonautonomous reaction-diffusion equation \[ u_t=u_{xx}+ug(t,x-ct,u), \quad t>0,x\in\mathbb{R}, \] where is the shifting speed, and the tim…

math.AP2020

Asymptotics of the principal eigenvalue for a linear time-periodic parabolic operator II: Small diffusion

Shuang Liu, Yuan Lou, Rui Peng +1

We investigate the effect of small diffusion on the principal eigenvalues of linear time-periodic parabolic operators with zero Neumann boundary conditions in one dimensional space…

math.AP2019

Sharp estimates for the spreading speed of the Lotka-Volterra diffusion system with strong competition

Rui Peng, Chang-Hong Wu, Maolin Zhou

This paper is concerned with the classical two-species Lotka-Volterra diffusion system with strong competition. The sharp dynamical behavior of the solution is established in two d…

math.AP201959 cited

Population dynamics in river networks

Yu Jin, Rui Peng, Junping Shi

Natural rivers connect to each other to form networks. The geometric structure of a river network can significantly influence spatial dynamics of populations in the system. We cons…

math.AP2019

Monotonicity of the principal eigenvalue for a linear time-periodic parabolic operator

Shuang Liu, Yuan Lou, Rui Peng +1

We investigate the effect of frequency on the principal eigenvalue of a time-periodic parabolic operator with Dirichlet, Robin or Neumann boundary conditions. The monotonicity and…

math.AP2018

Asymptotic behavior of the principal eigenvalue of a linear second order elliptic operator with small/large diffusion coefficient and its application

Rui Peng, Guanghui Zhang, Maolin Zhou

In this article, we are concerned with the following eigenvalue problem of a linear second order elliptic operator: \begin{equation} \nonumber -DΔϕ-2α\nabla m(x)\cdot \nablaϕ+V(x)ϕ…