2019
DOI: 10.1016/j.nonrwa.2018.07.004
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An integro-PDE model with variable motility

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Cited by 21 publications
(11 citation statements)
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“…Actually, although p ≥ 1 + 4/ N can yield blowup result for the classical Schrödinger equation i∂ t ψ + △ ψ + | ψ | p − 1 ψ = 0, our discussion in this paper only turns out the condensation effect can cover the Yukawa interaction as p > 3, N ≥ 2. One can also refer to other works() for similar case. The problem is we cannot point out whether this is a sharp threshold for collapse or not.…”
Section: Blowup In Finite Timementioning
confidence: 99%
“…Actually, although p ≥ 1 + 4/ N can yield blowup result for the classical Schrödinger equation i∂ t ψ + △ ψ + | ψ | p − 1 ψ = 0, our discussion in this paper only turns out the condensation effect can cover the Yukawa interaction as p > 3, N ≥ 2. One can also refer to other works() for similar case. The problem is we cannot point out whether this is a sharp threshold for collapse or not.…”
Section: Blowup In Finite Timementioning
confidence: 99%
“…It should be emphasized that the work of Berestycki et al [3] did not require that the nonlocality is weak( that is, the nonlocal delay is small). After that, many important results about traveling wave solution and the spreading speed of equation (7) have been obtained, see [1,2,11,8,7,20,16,17,18,19,39] and the references therein. In addition, traveling wave soltuions of delayed Fisher-KPP equation was also studied deeply, see [4,11,21,30] and the references therein.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, a standard calculation shows its second order derivative J ′′ (t) in time has not definite sign, even for the system with negative energy. 15,16 In this paper, we eventually introduce a new modification…”
Section: Introductionmentioning
confidence: 99%