Combination of the successive perturbation method with other common methods

1987 ◽  
Vol 65 (5) ◽  
pp. 462-463 ◽  
Author(s):  
V. A. Popescu ◽  
I. M. Popescu

For the hydrogen atom in the fundamental state perturbed by βr−1, it is shown how the successive perturbation method can be combined with the method in which some fraction of a nonperturbed term (in the Hamiltonian) is included in the perturbation. Thus, the radius of convergence of the perturbation series is increased.

1966 ◽  
Vol 7 (11) ◽  
pp. 1900-1902 ◽  
Author(s):  
George A. Baker ◽  
Roy Chisholm

2009 ◽  
Vol 23 (30) ◽  
pp. 3667-3675 ◽  
Author(s):  
AHMET YILDIRIM

We implemented homotopy perturbation method for approximating the solution to the nonlinear dispersive K(m,n,1) type equations. By using this scheme, the explicit exact solution is calculated in the form of a quickly convergent series with easily computable components. To illustrate the application of this method, numerical results are derived by using the calculated components of the homotopy perturbation series.


1983 ◽  
Vol 102 (4) ◽  
pp. 344-353 ◽  
Author(s):  
Gustavo A. Arteca ◽  
Francisco M. Fernandez ◽  
Eduardo A. Castro

1976 ◽  
Vol 31 (6) ◽  
pp. 517-523 ◽  
Author(s):  
H. G. Becker ◽  
K. Bleuler

Using the advantages of the O (4)-symmetry the second order Stark-effect of the hydrogen atom is calculated by the Dalgarno-Lewis perturbation method in a purely algebraic manner. The Starkeffect provides the first quantum mechanical example in which the Dalgarno-Lewis equation relevant for second and third order perturbation theory of the whole spectrum can be exactly solved


1990 ◽  
Vol 68 (12) ◽  
pp. 1476-1478
Author(s):  
V. A. Popescu ◽  
I. M. Popescu ◽  
M. Jitaru

We consider the case where the radius of convergence of the perturbation expansion can be related to a "crossing" of two energy levels in the complex plane of the interaction parameter. This case is suitable for the comparison of the performance of the successive perturbation method with those of the Padé, Borel–Padé, and the variational functional methods.


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