2009
DOI: 10.1016/j.matcom.2009.06.019
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Identification of solitary-wave solutions as an inverse problem: Application to shapes with oscillatory tails

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Cited by 12 publications
(11 citation statements)
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“…Table 2 Best fit curve formulas for spectral coefficients of initial condition of 4BTE. For the 4BTE there is no exact solution available and the comparison is done with the computational solutions obtained in [3]. In [3] the stationary shapes of the 4BTE (21) are computed using the method of variational imbedding (MVI).…”
Section: Methods Validationmentioning
confidence: 99%
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“…Table 2 Best fit curve formulas for spectral coefficients of initial condition of 4BTE. For the 4BTE there is no exact solution available and the comparison is done with the computational solutions obtained in [3]. In [3] the stationary shapes of the 4BTE (21) are computed using the method of variational imbedding (MVI).…”
Section: Methods Validationmentioning
confidence: 99%
“…For the 4BTE there is no exact solution available and the comparison is done with the computational solutions obtained in [3]. In [3] the stationary shapes of the 4BTE (21) are computed using the method of variational imbedding (MVI). The latter was introduced in [23] and applied to finding the homoclinic solution of the Lorentz equations.…”
Section: Methods Validationmentioning
confidence: 99%
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“…Due to the nature of asymptotic boundary conditions for decay of the amplitude of the wave at infinity,the system under consideration always possesses a trivial solution. The above outline ddifficulties are much harder when the solutions have nonmomotone tails and when the intervals where they are well separated from zero, are large (see [3]). In many instances,the problem of finding the nontrivial amplitude of the bifurcating solution is akin to the problem of coefficient identification.…”
Section: Introductionmentioning
confidence: 97%