2005
DOI: 10.1090/s0002-9939-05-07851-2
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On the solitary wave pulse in a chain of beads

Abstract: Abstract. We study the shape of solitary wave pulses that propagate in an infinite chain of beads initially in contact with no compression. For this system, the repulsive force between two adjacent beads is proportional to the p th power of the distance of approach of their centers with p = 3 2 . It is known that solitary wave solutions exist for such a system when p > 1. We prove extremely fast, double-exponential, asymptotic decay for these wave pulses. An iterative method of solution is also proposed and is… Show more

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Cited by 70 publications
(88 citation statements)
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“…In this case, too, as identified via the methods of Refs. [6][7][8]22] (see Appendix B for details on numerical simulations) and shown in Fig. 1, the family of STWs numerically features H (c) > 0, in full agreement with their identification as stable.…”
Section: Numerical Corroborationsupporting
confidence: 73%
See 1 more Smart Citation
“…In this case, too, as identified via the methods of Refs. [6][7][8]22] (see Appendix B for details on numerical simulations) and shown in Fig. 1, the family of STWs numerically features H (c) > 0, in full agreement with their identification as stable.…”
Section: Numerical Corroborationsupporting
confidence: 73%
“…(9) of the FPU case but add long-range interactions with the kernel in Eq. (8). Figure 2 showcases the power of the stability criterion and illustrates the complementary nature of the cotraveling steady state and the periodic orbit FM calculation approaches.…”
Section: Numerical Corroborationmentioning
confidence: 99%
“…Note that these (Gaussian) homoclinic solutions decay super-exponentially, but do not decay doubly exponentially unlike the solitary wave solutions of the differential advance-delay equation (2.4) [30,31]. Homoclinic solution (3.16) yields an approximate Gaussian solitary wave solution of FPU lattice (1.8) with velocity equal to unity Ahnert & Pikovsky [28], based on a reformulation of (2.4) as a nonlinear integral equation and the method of successive approximations (see also [9,31] for variants of this method).…”
Section: (B) Stationary Solutionsmentioning
confidence: 99%
“…We will seek them directly as traveling waves in real space, by attempting to identify fixed points of a discretization of the co-traveling frame nonlinear problem in our direct method. We will also follow the approach of [43], rewriting the problem in Fourier space (upon a Fourier transform) and seeking fixed points of that variant upon inverse Fourier transform, similarly to [39,43]. This will recover a convolution based reformulation of the problem in real space.…”
Section: Introductionmentioning
confidence: 99%