Stationary peaks in a multivariable reaction-diffusion system: foliated snaking due to subcritical Turing instability

被引:5
作者
Knobloch, Edgar [1 ]
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
基金
美国国家科学基金会;
关键词
localized states; homoclinic snaking; wavenumber selection; reaction-diffusion systems; MATRIX GLA PROTEIN; PATTERN-FORMATION; LOCALIZED STATES; HOMOCLINIC ORBITS; MECHANISM; DYNAMICS; MODEL; OSCILLATIONS; TRANSITION;
D O I
10.1093/imamat/hxab029
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
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.
引用
收藏
页码:1066 / 1093
页数:28
相关论文
共 88 条
  • [1] Localized Patterns in Periodically Forced Systems
    Alnahdi, A. S.
    Niesen, J.
    Rucklidge, A. M.
    [J]. SIAM JOURNAL ON APPLIED DYNAMICAL SYSTEMS, 2014, 13 (03): : 1311 - 1327
  • [2] [Anonymous], 2009, DISCRETE CONTINUOUS
  • [3] Solidification in soft-core fluids: Disordered solids from fast solidification fronts
    Archer, A. J.
    Walters, M. C.
    Thiele, U.
    Knobloch, E.
    [J]. PHYSICAL REVIEW E, 2014, 90 (04):
  • [4] Pattern formation and competition in nonlinear optics
    Arecchi, FT
    Boccaletti, S
    Ramazza, P
    [J]. PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 1999, 318 (1-2): : 1 - 83
  • [5] Spatially localized binary-fluid convection
    Batiste, Oriol
    Knobloch, Edgar
    Alonso, Arantxa
    Mercader, Isabel
    [J]. JOURNAL OF FLUID MECHANICS, 2006, 560 : 149 - 158
  • [6] Convectons and secondary snaking in three-dimensional natural doubly diffusive convection
    Beaume, Cedric
    Bergeon, Alain
    Knobloch, Edgar
    [J]. PHYSICS OF FLUIDS, 2013, 25 (02)
  • [7] Eckhaus instability and homoclinic snaking
    Bergeon, A.
    Burke, J.
    Knobloch, E.
    Mercader, I.
    [J]. PHYSICAL REVIEW E, 2008, 78 (04):
  • [8] Mathematical Modeling of Plant Root Hair Initiation: Dynamics of Localized Patches
    Brena-Medina, V.
    Champneys, A. R.
    Grierson, C.
    Ward, M. J.
    [J]. SIAM JOURNAL ON APPLIED DYNAMICAL SYSTEMS, 2014, 13 (01): : 210 - 248
  • [9] Subcritical Turing bifurcation and the morphogenesis of localized patterns
    Brena-Medina, Victor
    Champneys, Alan
    [J]. PHYSICAL REVIEW E, 2014, 90 (03):
  • [10] Classification of Spatially Localized Oscillations in Periodically Forced Dissipative Systems
    Burke, J.
    Yochelis, A.
    Knobloch, E.
    [J]. SIAM JOURNAL ON APPLIED DYNAMICAL SYSTEMS, 2008, 7 (03) : 651 - 711