2017
DOI: 10.1137/16m1087655
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Resonance Phenomena in a Scalar Delay Differential Equation with Two State-Dependent Delays

Abstract: Abstract. We study a scalar DDE with two delayed feedback terms that depend linearly on the state. The associated constant-delay DDE, obtained by freezing the state dependence, is linear and without recurrent dynamics. With state dependent delay terms, on the other hand, the DDE shows very complicated dynamics. To investigate this, we perform a bifurcation analysis of the system and present its bifurcation diagram in the plane of the two feedback strengths. It is organized by Hopf-Hopf bifurcation points that … Show more

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Cited by 38 publications
(49 citation statements)
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References 68 publications
(171 reference statements)
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“…In the context of the DDE (1) the trivial steady state Q = 0 is unstable when Q * > 0 51 . For the stability of Q * , from (7) and (12) we have a + b = (A − 1)Q * β (Q * ), and hence using (2) and (8) we find that −sκ < −sκ(1 − κ/[f (A − 1)]) = a + b < 0. Thus when Q * > 0 we have a + b < 0, and Q * can only lose stability if (a, b) crosses the curve C 0 as parameters are varied.…”
Section: A Stability Boundarymentioning
confidence: 95%
See 1 more Smart Citation
“…In the context of the DDE (1) the trivial steady state Q = 0 is unstable when Q * > 0 51 . For the stability of Q * , from (7) and (12) we have a + b = (A − 1)Q * β (Q * ), and hence using (2) and (8) we find that −sκ < −sκ(1 − κ/[f (A − 1)]) = a + b < 0. Thus when Q * > 0 we have a + b < 0, and Q * can only lose stability if (a, b) crosses the curve C 0 as parameters are varied.…”
Section: A Stability Boundarymentioning
confidence: 95%
“…The parameter regions for which the steady state of equation (10) is stable (white) and unstable (shaded). Also shown (red) is the locus in (a, b) of the parameters defined by (12) as τ is varied with the other parameters all at their values from Table I. The values of τ from (16) are indicated on this curve.…”
Section: A Stability Boundarymentioning
confidence: 99%
“…More specifically, we compute periodic solutions and tori and present them in different ways: in projection onto the (h(t), h(t − τ n ))-plane and as stroboscopic trace in the (h(t), h(t − τ n ))-plane, where triangles, crosses and squares represent stable, 1-saddle and 2-saddle periodic solutions, respectively. An enlargement of the stroboscopic trace also shows the one- dimensional trace of the unstable manifolds of the 1-saddle periodic solutions; as in [9] these curves were calculated via integration of initial conditions very close to the 1-saddle periodic solutions along their unstable eigendirections -technically, within a region referred to as a fundamental domain [31]. Throughout, light and dark shades of the same colours distinguish between the two symmetry-related periodic solutions (whose existence was discussed in section 1); see [29] for more details.…”
Section: Criticality Of the Curve Tmentioning
confidence: 98%
“…where [2,3]  [3,4]  [4,5]  [5,6]  [6,7]  [7,8]  [8,9]  [9,10] (2.16). Also shown in colour are the ten stages of the parametrisation of (t(µ i (η), u(µ i (η)) from the proof of Theorem 2.3 for i = 0, 1, 2 and j = 0.…”
Section: Singular Solutionsmentioning
confidence: 99%
“…For θ ∈ (0, 1), T = T 1 + T 2 where T i > 0, the Type I and Type II bimodal periodic admissible singular solution profiles are defined by We see from the (2.16) and (2.17) that both solutions have global minima with u = (−a 1 + nT )/c. If the phase of the periodic solution is chosen so that these minima occur when t = jT , for integer j, then for type I bimodal solutions the first local maximum which [3,4]  [4,5]  [5,6]  [6,7]  [7,8]  [8,9]  [9,10]…”
Section: Singular Solutionsmentioning
confidence: 99%