Abstract:The use of Bateman method for solving the two-variable version of the twobody Lippmann-Schwinger equation without recourse to partial-wave decomposition is investigated. Bateman method is based on a special kind of interpolation of the momentum representation of the potential on a multi-variate grid. A suitable scheme for the generation of a multi-variate Cartesian grid is described. The method is tested on the Hartree potential for electron-hydrogen scattering in the static no-exchange approximation. Our resu… Show more
“…Towards this end, multivariable methods has been investigated for the solution of the multi-variable LS equation in the momentum space [3][4][5][6][7][8][9][10][11][12][13]. For example in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…For example in Refs. [11,12] , we have considered multivariable implementations of Schwinger variational and Bateman methods for two-body LS equation in momentum space. Significant progress has also been reported on the formal and computational aspects of solving the three-particle momentum-space Faddeev equations directly as 5-variable problems without invoking angular momentum decomposition [2,14,15].…”
Section: Introductionmentioning
confidence: 99%
“…Calculational schemes based on momentum-space LS equations dominate the literature for two-body scattering computations, as exemplified in [3,[5][6][7][8][9][10][11][12][13]. Coordinate-space version of the LS equation have received relatively less attention as a computational vehicle, although the coordinate-space partial-wave LS equation has been employed in connection with various types of Schwinger variational methods [16][17].…”
Direct numerical solution of the coordinate-space integral-equation version of the two-particle Lippmann Schwinger (LS) equation is considered as a means of avoiding the shortcomings of partial-wave expansion at high energies and in the context of few-body problems. Upon the regularization of the singular kernel of the three-dimensional LS equation by a subtraction technique, a three-variate quadrature rule is used to solve the resulting nonsingular integral equation. To avoid the computational burden of discretizing three variables, advantage is taken of the fact that, for central potentials, azimuthal angle can be integrated out leaving a two-variable reduced integral equation. Although the singularity in the the kernel of the two-variable integral equation is weaker than that of the three-dimensional equation, it nevertheless requires careful handling for quadrature discretization to be applicable. A regularization method for the kernel of the two-variable integral equation is derived from the treatment of the singularity in the three-dimensional equation. A quadrature rule constructed as the direct-product of single-variable quadrature rules for radial distance and polar angle is used to discretize the two-variable integral equation. These twoand three-variable methods are tested on a model nucleon-nucleon potential. The results show that Nystrom method for the coordinate-space LS equation compares favorably in terms of its ease of implementation and effectiveness with the Nystrom method for the momentum-space version of the LS equation .
“…Towards this end, multivariable methods has been investigated for the solution of the multi-variable LS equation in the momentum space [3][4][5][6][7][8][9][10][11][12][13]. For example in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…For example in Refs. [11,12] , we have considered multivariable implementations of Schwinger variational and Bateman methods for two-body LS equation in momentum space. Significant progress has also been reported on the formal and computational aspects of solving the three-particle momentum-space Faddeev equations directly as 5-variable problems without invoking angular momentum decomposition [2,14,15].…”
Section: Introductionmentioning
confidence: 99%
“…Calculational schemes based on momentum-space LS equations dominate the literature for two-body scattering computations, as exemplified in [3,[5][6][7][8][9][10][11][12][13]. Coordinate-space version of the LS equation have received relatively less attention as a computational vehicle, although the coordinate-space partial-wave LS equation has been employed in connection with various types of Schwinger variational methods [16][17].…”
Direct numerical solution of the coordinate-space integral-equation version of the two-particle Lippmann Schwinger (LS) equation is considered as a means of avoiding the shortcomings of partial-wave expansion at high energies and in the context of few-body problems. Upon the regularization of the singular kernel of the three-dimensional LS equation by a subtraction technique, a three-variate quadrature rule is used to solve the resulting nonsingular integral equation. To avoid the computational burden of discretizing three variables, advantage is taken of the fact that, for central potentials, azimuthal angle can be integrated out leaving a two-variable reduced integral equation. Although the singularity in the the kernel of the two-variable integral equation is weaker than that of the three-dimensional equation, it nevertheless requires careful handling for quadrature discretization to be applicable. A regularization method for the kernel of the two-variable integral equation is derived from the treatment of the singularity in the three-dimensional equation. A quadrature rule constructed as the direct-product of single-variable quadrature rules for radial distance and polar angle is used to discretize the two-variable integral equation. These twoand three-variable methods are tested on a model nucleon-nucleon potential. The results show that Nystrom method for the coordinate-space LS equation compares favorably in terms of its ease of implementation and effectiveness with the Nystrom method for the momentum-space version of the LS equation .
“…Certain drawbacks of this strategy have been noted in recent years, especially for high-energy collisions and within the context of few-body problems. As a result, computational methods that avoid the traditional decomposition of wave functions and scattering amplitudes into partial waves have been explored recently by a number of groups [1][2][3][4][5][6][7][8][9][10][11][12]. Various direct multivariable methods have been investigated for the solution of two-body Lippmann Schwinger (LS) equation.…”
Section: Introductionmentioning
confidence: 99%
“…Among these, multivariable version of the Schwinger variational method (with local interpolation polynomials as the expansion basis) and some of its variants have been shown to be quite effective [11]. In a similar vein, a multivariate Bateman interpolation of the momentum-space kernel of the potential have proved to be a relatively simple and effective method [12]. It is interesting to note that both these methods can also be viewed as the result of certain finite-rank separable approximations of the interaction potential [11,14].…”
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