Weak [Formula Presented] interaction

Physical Review C - Nuclear Physics

Volumn 57, Issue 3, 1998, Pages 1478-1484

  Savage, Martin J ^a   Springer, Roxanne P ^b  

^a UNIVERSITY OF WASHINGTON   (United States)

^b DUKE UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0039984803     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.57.1478     Document Type: Article

References (16)

1. M. Danysz, et al., Phys. Rev. Lett. 11, 29 (1993)
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5. E. Jenkins, Nucl. Phys. B375, 561 (1992).
6. M. J. Savage and R. P. Springer, Phys. Rev. C 53, 441 (1996).
7. A. Parreno, A. Ramos, and C. Bennhold, Phys. Rev. C 56, 339 (1997).
8. C. Carone and H. Georgi, Nucl. Phys. B375, 243 (1992).
9. The formalism of heavy baryon chiral perturbation theory is introduced by E. Jenkins and A. V. Manohar, in Proceedings of Effective Field Theories of the Standard Model, Dobogokoe, 1991 (unpublished), pp. 113–137.
10. E. Jenkins and A. Manohar, Phys. Lett. B 255, 558 (1991)
11. Phys. Lett. BE. JenkinsA. Manohar259, 353 (1991).
12. M. N. Butler, M. J. Savage, and R. P. Springer, Nucl. Phys. B399, 69 (1993).
13. R. P. Springer, Report No. DUKE-TH-97-152.
14. M. J. Savage and J. Walden, Phys. Rev. D 55, 5376 (1997).
15. M. A. Luty and M. White, Phys. Lett. B 319, 261 (1993).
16. J. F. Dubach, G. B. Feldman, B. R. Holstein, and L. de la Torre, Ann. Phys. (N.Y.) 249, 146 (1996). Note that our amplitudes cannot be directly compared with the amplitudes found in this reference because of different conventions (which can be extracted from the experimental amplitudes given).