2020
DOI: 10.1016/j.jde.2020.04.040
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Persistence and spreading speeds of parabolic-elliptic Keller-Segel models in shifting environments

Abstract: The current paper is concerned with the forced waves of Keller-Segel chemoattraction systems in shifting environments of the form, u t = u xx − χ(uv x) x + u(r(x − ct) − bu), x ∈ R 0 = v xx − νv + µu, x ∈ R, (0.1) where χ, b, ν, and µ are positive constants, c ∈ R, the resource function r(x) is globally Hölder continuous, bounded, r * = sup x∈R r(x) > 0, r(±∞) := lim x→±∞ r(x) exist, and either r(−∞) < 0 < r(∞), or r(±∞) < 0. Assume that b > 2χµ. In the case that r(−∞) < 0 < r(∞), it is shown that (0.1) has a … Show more

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Cited by 6 publications
(3 citation statements)
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“…Shen and Xue [88,89] incorporated the shifted feature into the parabolic-elliptic Keller-Segel models as follows…”
Section: Systems With Shifting Habitatsmentioning
confidence: 99%
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“…Shen and Xue [88,89] incorporated the shifted feature into the parabolic-elliptic Keller-Segel models as follows…”
Section: Systems With Shifting Habitatsmentioning
confidence: 99%
“…Theorem 3.4. [88,89] The persistence and spreading speeds as well as the forced waves of model (28) read that (i) For the case that r(−∞) < 0 < r(∞), the species becomes extinct in the habitat if the moving speed c > ĉ * := 2 √ r * ; and will persist and spread along the shifting habitat at the asymptotic spreading speed ĉ * if −ĉ * ≤ c < ĉ * ; and will spread in the both directions at the asymptotic spreading speed ĉ * if c < −ĉ * . Further, system (28) admits a forced wave solution connecting b−χµ .…”
Section: Systems With Shifting Habitatsmentioning
confidence: 99%
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