Stationary peaks in a multivariable reaction-diffusion system: foliated snaking due to subcritical Turing instability
被引:5
作者:
Knobloch, Edgar
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Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USAUniv Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
Knobloch, Edgar
[1
]
Yochelis, Arik
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Ben Gurion Univ Negev, Dept Solar Energy & Environm Phys, Swiss Inst Dryland Environm & Energy Res, Blaustein Inst Desert Res, Sede Boqer Campus, IL-8499000 Midreshet Ben Gurion, Israel
Ben Gurion Univ Negev, Dept Phys, IL-8410501 Beer Sheva, IsraelUniv Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
Yochelis, Arik
[2
,3
]
机构:
[1] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[2] Ben Gurion Univ Negev, Dept Solar Energy & Environm Phys, Swiss Inst Dryland Environm & Energy Res, Blaustein Inst Desert Res, Sede Boqer Campus, IL-8499000 Midreshet Ben Gurion, Israel
[3] Ben Gurion Univ Negev, Dept Phys, IL-8410501 Beer Sheva, Israel
An activator-inhibitor-substrate model of side branching used in the context of pulmonary vascular and lung development is considered on the supposition that spatially localized concentrations of the activator trigger local side branching. The model consists of four coupled reaction-diffusion equations, and its steady localized solutions therefore obey an eight-dimensional spatial dynamical system in one spatial dimension (1D). Stationary localized structures within the model are found to be associated with a subcritical Turing instability and organized within a distinct type of foliated snaking bifurcation structure. This behavior is in turn associated with the presence of an exchange point in parameter space at which the complex leading spatial eigenvalues of the uniform concentration state are overtaken by a pair of real eigenvalues; this point plays the role of a Belyakov-Devaney point in this system. The primary foliated snaking structure consists of periodic spike or peak trains with N identical equidistant peaks, N=1,2, ..., together with cross-links consisting of nonidentical, nonequidistant peaks. The structure is complicated by a multitude of multipulse states, some of which are also computed, and spans the parameter range from the primary Turing bifurcation all the way to the fold of the N=1 state. These states form a complex template from which localized physical structures develop in the transverse direction in 2D.