Abstract:Recently there has been a growing interest in computational methods for quantum scattering equations that avoid the traditional decomposition of wave functions and scattering amplitudes into partial waves. The aim of the present work is to show that the
“…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 .
“…Therefore, there is considerable interest in multi-variable methods that could produce the three-dimensional off-shell T-matrix in more economical manner than the Nystrom method. Galerkin [2,4], collocation [10], and Schwinger variational methods [10] have been investigated with various choices of multi-variable bases. These methods can effectively be viewed as contractions of the linear system of equations that the Nystrom approach gives rise to.…”
mentioning
confidence: 99%
“…These methods can effectively be viewed as contractions of the linear system of equations that the Nystrom approach gives rise to. In other words, the (large) equation system of the Nystrom method is replaced by a smaller set of approximate equations, by demanding that a residual vanishes on a chosen test space [10].…”
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 results show that the Bateman method is capable of producing quite accurate solutions with relatively small number of grid points.Keywords Quantum scattering theory · Lippmann-Schwinger equation · Few-body collisions · Multi-variate interpolation and approximation · Bateman interpolation · Degenerate-kernel methods for integral equations · Nystrom method · Faddeev equations
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