BB intermeson potentials in the quark model

Physical Review C - Nuclear Physics

Volumn 60, Issue 4, 1999, Pages 452021-4520212

  Barnes, T ^a,b   Black, N ^b   Dean, D J ^a,b   Swanson, E S ^c  

^a OAK RIDGE NATIONAL LABORATORY   (United States)

^b UNIVERSITY OF TENNESSEE   (United States)

^c NORTH CAROLINA STATE UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 17144470017     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.60.045202     Document Type: Article

References (26)

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8. T. Barnes and E.S. Swanson, Phys. Rev. D 46, 131 (1992); see also G.-Q. Zhao, X.G. Jing, and J.-C. Su, ibid. 58, 117503 (1998) (Π Π scattering); D. Blaschke and G. Röpke, Phys. Lett. B 299, 332 (1993); K. Martins, D. Blaschke, and E. Quack, Phys. Rev. C 51, 2723 (1995) (cc̄ propagation in media).
9. T. Barnes and E.S. Swanson, Phys. Rev. D 46, 131 (1992); see also G.-Q. Zhao, X.G. Jing, and J.-C. Su, ibid. 58, 117503 (1998) (Π Π scattering); D. Blaschke and G. Röpke, Phys. Lett. B 299, 332 (1993); K. Martins, D. Blaschke, and E. Quack, Phys. Rev. C 51, 2723 (1995) (cc̄ propagation in media).
10. T. Barnes and E.S. Swanson, Phys. Rev. D 46, 131 (1992); see also G.-Q. Zhao, X.G. Jing, and J.-C. Su, ibid. 58, 117503 (1998) (Π Π scattering); D. Blaschke and G. Röpke, Phys. Lett. B 299, 332 (1993); K. Martins, D. Blaschke, and E. Quack, Phys. Rev. C 51, 2723 (1995) (cc̄ propagation in media).
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14. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
15. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
16. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
17. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
18. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
19. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
20. There is an extensive literature on quark model calculations of the NN force, beginning with D.A. Liberman, Phys. Rev. D 16, 1542 (1977). More recent studies have employed resonating group methods [see for example C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); M. Oka and K. Yazaki, Phys. Lett. 90B, 41 (1980); C.S. Warke and R. Shanker, Phys. Rev. C 21, 2643 (1980); J.E.T. Ribeiro, Z. Phys. C 5, 27 (1980)] and variational methods [for example, K. Maltman and N. Isgur, Phys. Rev. D 29, 952 (1984)]. A more extensive set of references and the Born-order OGE NN results analogous to the present paper are given in T. Barnes, S. Capstick, M.D. Kovarik, and E.S. Swanson, Phys. Rev. C 48, 539 (1993).
21. T. Barnes and G.I. Ghandour, Phys. Lett. 118B, 411 (1982), give a systematic procedure for converting a general T-matrix into an equivalent potential operator.
22. D. Scora and N. Isgur, Phys. Rev. D 52, 2783 (1995); see especially Appendix A.
23. s/3r. The spectator light antiquarks should not significantly modify this conclusion.
24. N.A. Törnqvist, Phys. Rev. Lett. 67, 556 (1991).
25. T.E.O. Ericson and G. Karl, Phys. Lett. B 309, 426 (1993).
26. G. Karl (private communication).