Scheme for an accurate solution of Faddeev integral equations in configuration space

Faddeev equations in configuration space for three-atom scattering processes are formulated in integral form allowing for additive and nonadditive forces. The object of the equations are T–functions, that are the product of wave functions times potentials, that decay to zero in all directions. The d...

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Published in:Nuclear physics. A Vol. 790; no. 1; pp. 282c - 285c
Main Authors: Glöckle, W., Rawitscher, G.
Format: Journal Article
Language:English
Published: Elsevier B.V 15-06-2007
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Abstract Faddeev equations in configuration space for three-atom scattering processes are formulated in integral form allowing for additive and nonadditive forces. The object of the equations are T–functions, that are the product of wave functions times potentials, that decay to zero in all directions. The driving and coupling terms are based on the two-body t–matrices, which describe the two-body correlations in each arrangement. However, three-atom forces are also included in the formalism. The solution is based on an accurate numerical spectral expansion method, and steps for a practical implementation are described for a simplified “toy” model, although numerical results are not yet available. This formulation appears to be a valuable alternative to current approaches.
AbstractList Faddeev equations in configuration space for three-atom scattering processes are formulated in integral form allowing for additive and nonadditive forces. The object of the equations are T–functions, that are the product of wave functions times potentials, that decay to zero in all directions. The driving and coupling terms are based on the two-body t–matrices, which describe the two-body correlations in each arrangement. However, three-atom forces are also included in the formalism. The solution is based on an accurate numerical spectral expansion method, and steps for a practical implementation are described for a simplified “toy” model, although numerical results are not yet available. This formulation appears to be a valuable alternative to current approaches.
Author Rawitscher, G.
Glöckle, W.
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  organization: Physics Department, University of Connecticut, Storrs, CT 06268
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CitedBy_id crossref_primary_10_1007_s00601_008_0301_z
crossref_primary_10_1007_s00601_010_0146_0
crossref_primary_10_1103_PhysRevA_77_012707
crossref_primary_10_1103_PhysRevE_85_026701
crossref_primary_10_1103_PhysRevC_86_034004
crossref_primary_10_1119_1_3534837
Cites_doi 10.1016/0003-4916(80)90344-9
10.1103/PhysRevA.65.032725
10.1088/0143-0807/27/5/017
10.1016/0370-1573(95)00085-2
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