Abstract
Available phase space suppresses the decay\(\Lambda _c^ + \to p\overline {K^0 } \pi ^ + \pi ^ - \) in comparison with the decay\(\Lambda _c^ + \to p\overline {K^0 } \). However, their comparable decay rates, as found experimentally, can be explained by the strong interaction induced tree diagrams in which pions are emitted along the final baryon leg.
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References
Particle Data Group: Phys. Rev. D45 (1992) Part 2
E.D. Commins, P.H. Bucksbaum: Weak interactions of leptons and quarks. Cambridge: Cambridge Univ. Press 1983, and references therein
B. Guberina, D. Tadić, J. Trampetić: Z. Phys. C13 (1982) 251
F. Hussain, M.D. Scadron: Nuovo Cimento 79A (1984) 248; F. Hussain, K. Khan:ibid. Nuovo Cimento 88A (1985) 213
D. Ebert, W. Kallies; Phys. Lett. 131B (1983) 183; 148B, (1984) 502(E); Yad. Fiz. 40 (1984) 1250 [Sov. J. Nucl. Phys. 40 (1984) 794; Z. Phys. C29 (1985) 643
H.Y. Cheng: Z. Phys. C29 (1985) 453; H.Y. Cheng, B. Tseng: Phys. Rev. D46 (1992) 1042
Yu.L. Kalinovsky, V.N. Pervushin, N.A. Sarikov: Phys. Lett. B 180 (1986) 141; Yu.L. Kalinovsky et al.: Fiz. Elem. Chastits At. Yadra 14 (1988) 77 [Sov. J. Part. Nucl. 14 (1988) 47]
S. Pakvasa, S.F. Tuan, S.P. Rosen: Phys. Rev. D42 (1990) 3746
G. Kaur, M.P. Khanna: Phys. Rev. D44 (1992) 182;ibid. G. Kaur: Phys. Rev. D45 (1992) R3024
S.M. Sheikoleslami, M.P. Khanna, R.C. Verma: Phys. Rev. D43 (1991) 170
G. Turan, J.O. Eeg: Z. Phys. C51 (1991) 599
J. Körner, M. Kramer: Z. Phys. C 55 (1992) 659
Acoording to [1]Λ + c is more likely to decay inpK - π + than in\(p\overline {K^0 } \)
G. Burdman, J. Donoghue: Phys. Lett. B280 (1992) 287
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Fajfer, S., Ilakovac, A., Tadic, D. et al. \(\Lambda _c \to p\bar K^0 \pi \pi \) and\(\Lambda _c \to p\bar K^0 \) decay rates. Z. Phys. C - Particles and Fields 62, 421–423 (1994). https://doi.org/10.1007/BF01555901
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DOI: https://doi.org/10.1007/BF01555901