Consistently computing the K → π long distance weak transition

Modern Physics Letters A

Volumn 17, Issue 38, 2002, Pages 2497-2512

  Lowe, J ^a   Scadron, M D ^b  

^a UNIVERSITY OF NEW MEXICO   (United States)

^b The University of Arizona   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ACCELERATION; ARTICLE; CALCULATION; ELECTROMAGNETIC RADIATION; ELEMENTARY PARTICLE; ENERGY; MASS; MATHEMATICAL ANALYSIS; MATHEMATICS; QUANTUM MECHANICS; SPACE;

EID: 0037079487     PISSN: 02177323     EISSN: None     Source Type: Journal    
DOI: 10.1142/S0217732302008976     Document Type: Article

References (42)

1. R. E. Karlsen and M. D. Scadron, Phys. Rev. D45, 4108 (1992).
2. us = (0.9750 ± 0.0008) × (0.2225 ± 0.0035) = 0.217 ± 0.003.
3. N. Cabibbo, Phys. Rev. Lett. 12, 62 (1964); M. Gell-Mann, ibid. 12, 155 (1964).
4. N. Cabibbo, Phys. Rev. Lett. 12, 62 (1964); M. Gell-Mann, ibid. 12, 155 (1964).
5. G. Grayer et al., Nucl. Phys. B75, 189 (1974); N. Durusoy et al., Phys. Lett. B45, 517 (1973). For a more recent summary of experimental ππ phase shifts, see J. Gasser and U.-G. Meissner, Phys. Lett. B258, 219 (1991).
6. G. Grayer et al., Nucl. Phys. B75, 189 (1974); N. Durusoy et al., Phys. Lett. B45, 517 (1973). For a more recent summary of experimental ππ phase shifts, see J. Gasser and U.-G. Meissner, Phys. Lett. B258, 219 (1991).
7. G. Grayer et al., Nucl. Phys. B75, 189 (1974); N. Durusoy et al., Phys. Lett. B45, 517 (1973). For a more recent summary of experimental ππ phase shifts, see J. Gasser and U.-G. Meissner, Phys. Lett. B258, 219 (1991).
8. Footprints of a broad σ(500-600) in weak interaction processes, A. D. Polosa, N. A. Tornquist, M. D. Scadron and V. Elias, hep-ph/0005106; Mod. Phys. Lett. A17, 569 (2002).
9. Footprints of a broad σ(500-600) in weak interaction processes, A. D. Polosa, N. A. Tornquist, M. D. Scadron and V. Elias, hep-ph/0005106; Mod. Phys. Lett. A17, 569 (2002).
10. R. Appel et al., E865 collab., Phys. Rev. Lett. 83, 4482 (1999).
11. H. Burkhardt et al., Phys. Lett. B512, 317 (2001); also see G. Eilam and M. D. Scadron, Phys. Rev. D31, 2263 (1985).
12. H. Burkhardt et al., Phys. Lett. B512, 317 (2001); also see G. Eilam and M. D. Scadron, Phys. Rev. D31, 2263 (1985).
13. φ = 1.0017, very close to unity as demanded.
14. C. O. Dib, I. Dunietz and F. J. Gilman, Phys. Rev. D39, 2639 (1989).
15. H. Ma et al., hep-ex/9910047; Phys. Rev. Lett. 84, 2580 (2000).
16. H. Ma et al., hep-ex/9910047; Phys. Rev. Lett. 84, 2580 (2000).
17. R. E. Karlsen and M. D. Scadron, Mod. Phys. Lett. A6, 543 (1991).
18. R. Delbourgo and M. D. Scadron, Nuovo Cimento Lett. 44, 193 (1985).
19. R. Delbourgo and D. Liu, Aust. J. Phys. 53, 737 (2000); hep-ph/0010155.
20. For light plane-damped wave functions see N. H. Fuchs and M. D. Scadron, Nuovo Cimento A93, 205 (1986); C. Michael and C. Payne, Nucl. Phys. B148, 102 (1979); Phys. Lett. B91, 41 (1980). We drop the factor of 0.97 from these papers.
21. For light plane-damped wave functions see N. H. Fuchs and M. D. Scadron, Nuovo Cimento A93, 205 (1986); C. Michael and C. Payne, Nucl. Phys. B148, 102 (1979); Phys. Lett. B91, 41 (1980). We drop the factor of 0.97 from these papers.
22. For light plane-damped wave functions see N. H. Fuchs and M. D. Scadron, Nuovo Cimento A93, 205 (1986); C. Michael and C. Payne, Nucl. Phys. B148, 102 (1979); Phys. Lett. B91, 41 (1980). We drop the factor of 0.97 from these papers.
23. W, our present notation).
24. See e.g. R. Marshak, Riazuddin and C. Ryan, Theory of Weak-Interaction Particle Physics (Wiley, 1969), p. 641.
25. M. Gell-Mann and M. Levy, Nuovo Cimento 16, 705 (1960); R. Delbourgo and M. D. Scadron, Mod. Phys. Lett. A10, 251 (1995).
26. M. Gell-Mann and M. Levy, Nuovo Cimento 16, 705 (1960); R. Delbourgo and M. D. Scadron, Mod. Phys. Lett. A10, 251 (1995).
27. V. Elias and M. D. Scadron, Mod. Phys. Lett. A10, 1159 (1995); S. R. Choudhury and M. D. Scadron, Phys. Rev. D53, 2421 (1996).
28. V. Elias and M. D. Scadron, Mod. Phys. Lett. A10, 1159 (1995); S. R. Choudhury and M. D. Scadron, Phys. Rev. D53, 2421 (1996).
29. T. Uppal et al., J. Phys. G21, 621 (1995); S. R. Choudhury and M. D. Scadron, Phys. Rev. D53, 2421 (1996).
30. T. Uppal et al., J. Phys. G21, 621 (1995); S. R. Choudhury and M. D. Scadron, Phys. Rev. D53, 2421 (1996).
31. M. D. Scadron and L. R. Thebaud, Phys. Rev. D8, 2190 (1973); M. D. Scadron and D. Tadic, J. Phys. G27, 163 (2001).
32. M. D. Scadron and L. R. Thebaud, Phys. Rev. D8, 2190 (1973); M. D. Scadron and D. Tadic, J. Phys. G27, 163 (2001).
33. M. D. Scadron and M. Visinescu, Phys. Rev. D28, 1117 (1983); M. P. Khanna et al., J. Phys. G12, 1323 (1986).
34. M. D. Scadron and M. Visinescu, Phys. Rev. D28, 1117 (1983); M. P. Khanna et al., J. Phys. G12, 1323 (1986).
35. See e.g. S. Drell, Nuovo Cimento 11, 692 (1959); M. Berman and D. Geffen, ibid. 18, 1192 (1960); L. Sehgal, ibid. 45, 785 (1966).
36. See e.g. S. Drell, Nuovo Cimento 11, 692 (1959); M. Berman and D. Geffen, ibid. 18, 1192 (1960); L. Sehgal, ibid. 45, 785 (1966).
37. See e.g. S. Drell, Nuovo Cimento 11, 692 (1959); M. Berman and D. Geffen, ibid. 18, 1192 (1960); L. Sehgal, ibid. 45, 785 (1966).
38. M. D. Scadron and M. Visinescu, Phys. Rev. D29, 911 (1984).
39. F. Inami and C. Lim, Prog. Theor. Phys. 65, 297 (1981).
40. J. M. Boglione and M. Pennington, Euro. Phys. J. C9, 11 (1999).
41. E. Aitala et al., E791 collab., Phys. Rev. Lett. 86, 770 (2001).
42. R. E. Karlsen and M. D. Scadron, Nuovo Cimento A106, 113 (1993).