-
6
-
-
0031139885
-
-
PLEEE8
-
Yu. B. Gaididei, S. F. Mingaleev, P. L. Christiansen, and K. Ø. Rasmussen, Phys. Rev. E 55, 6141 (1997).PLEEE8
-
(1997)
Phys. Rev. E
, vol.55
, pp. 6141
-
-
Gaididei, Y.B.1
Mingaleev, S.F.2
Christiansen, P.L.3
Ø. Rasmussen, K.4
-
7
-
-
51249161338
-
-
G. Gaeta, C. Reiss, M. Peyrard, and T. Dauxois, Riv. Nuovo Cimento 17, 1 (1994);
-
(1994)
Riv. Nuovo Cimento
, vol.17
, pp. 1
-
-
Gaeta, G.1
Reiss, C.2
Peyrard, M.3
Dauxois, T.4
-
11
-
-
85035228775
-
-
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
-
-
0L. Proville and S. Aubry ibid. (to be published).
-
0L. Proville and S. Aubry ibid. (to be published).
-
-
-
-
15
-
-
85035211764
-
-
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
-
-
22244486688
-
-
S. Aubry, Physica D 103, 201 (1997).
-
(1997)
Physica D
, vol.103
, pp. 201
-
-
Aubry, S.1
-
17
-
-
33646974037
-
-
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
-
-
Yu. B. Gaididei et al. (unpublished).
-
Yu. B. Gaididei et al. (unpublished).
-
-
-
-
20
-
-
85035218141
-
-
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.
-
-
-
|