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Volumn 57, Issue 4, 1998, Pages 4739-4742

Switching between bistable states in a discrete nonlinear model with long-range dispersion

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EID: 0004575138     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.57.4739     Document Type: Article
Times cited : (26)

References (20)
  • 11
    • 85035228775 scopus 로고    scopus 로고
    • J. L. Marín, S. Aubry, and L. M. Floría, ibid. (to be published);
    • J. L. Marín, S. Aubry, and L. M. Floría, ibid. (to be published);
  • 12
    • 85035234497 scopus 로고    scopus 로고
    • 0L. Proville and S. Aubry ibid. (to be published).
    • 0L. Proville and S. Aubry ibid. (to be published).
  • 15
    • 85035211764 scopus 로고    scopus 로고
    • We remark that since [formula presented], [formula presented] are time independent, the approach used here is equivalent to the standard Floquet analysis that was used, e.g., in 7, 8, 11. Namely, if μ is an eigenvalue of M, then [formula presented] where [formula presented] is an eigenvalue of the Floquet matrix for the same eigenvector.
    • We remark that since H+ and H- are time independent, the approach used here is equivalent to the standard Floquet analysis that was used, e.g., in 7811. Namely, if μ is an eigenvalue of M, then λ=eμT, where T=2π/Λ is an eigenvalue of the Floquet matrix for the same eigenvector.
  • 16
  • 17
    • 33646974037 scopus 로고
    • Izv. Vyssh. Uchebn. Zaved. Radiofiz. 16, 1020 (1973) [ SORPAK
    • M. G. Vakhitov and A. A. Kolokolov, Izv. Vyssh. Uchebn. Zaved. Radiofiz. 16, 1020 (1973) [Sov. Radiophys. 16, 783 (1973)];
    • (1973) Sov. Radiophys. , vol.16 , pp. 783
    • Vakhitov, M.G.1    Kolokolov, A.A.2
  • 19
    • 85035213967 scopus 로고    scopus 로고
    • Yu. B. Gaididei et al. (unpublished).
    • Yu. B. Gaididei et al. (unpublished).
  • 20
    • 85035218141 scopus 로고    scopus 로고
    • We remark that a state close to the instability regime in general has a larger value of the Hamiltonian than its bistable counterpart. Thus, when [formula presented] is small the switching can be viewed as a transition from a metastable state to a ground state.
    • We remark that a state close to the instability regime in general has a larger value of the Hamiltonian than its bistable counterpart. Thus, when|αth|is small the switching can be viewed as a transition from a metastable state to a ground state.


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