Abstract

We study bifurcations of localized stationary solutions of the externally driven, damped nonlinear Schrodinger equation iC t1Cxx12uCuC52igC2he in the region of large g (g.1/2). For each pair of h and g , there are two coexisting solitons C1 and C2 . As the driver’s strength h increases for the fixed g , the C1 soliton merges with the flat background while the C2 forms a stationary collective state with two ‘‘C pluses’’: C2→C (121) . We obtain other stationary solutions and identify them as multisoliton complexes C (11) ,C (22) ,C (21) ,C (222) ,C (212) , etc. @S1063-651X~98!06002-4#

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