-nucleon interactions and y*1-resonance

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IL NUOVO CIMENT0 VOL. XXXV, N. 1 lO Gennaio 1965 K-Nucleon Interactions and Y~-Resonance. I~AMESH CHAND Department o] Physics, Syracuse U~iversity - Siracuse, N. Y. (Nuovo Cimento, 30, 1443 (1963)) Equation (7.2) on p. 1448 should read 2 5 (7.2) F = --~Krb(Ke)/lz. K-Nucleon Interactions. RAM]~SH CHAND Department o] Physics, Syracuse University - Syracuse, N. Y. (Nuovo Cimento, 32, 1234 (1964)) Equation (4b) on p. 1236 should read 2 5 b (4b) F=--~K r (Kr)/#. This means that the analysis on ~', ~Y coupled systems in an I= 1, pcstate and discussed in these two papers is correct only for the width of the 1385 MeV Y* resonance to be F=50/3MeV and not for F=50MeV. The analysis for F=50 MeV will soon be sent lor publication.

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IL NUOVO CIMENT0 VOL. XXXV, N. 1 lO Gennaio 1965

K-Nucleon Interactions and Y~-Resonance.

I~AMESH CHAND

Department o] Physics, Syracuse U~iversity - Siracuse, N. Y.

(Nuovo Cimento, 30, 1443 (1963))

Equation (7.2) on p. 1448 should read

2 5 (7.2) F = --~Krb(Ke)/lz.

K-Nucleon Interactions.

RAM]~SH CHAND

Department o] Physics, Syracuse University - Syracuse, N. Y.

(Nuovo Cimento, 32, 1234 (1964))

Equation (4b) on p. 1236 should read

2 5 b (4b) F = - - ~ K r (Kr)/#.

This means that the analysis on ~ ' , ~Y coupled systems in an I = 1, pcs ta te and discussed in these two papers is correct only for the width of the 1385 MeV Y* resonance to be F = 5 0 / 3 M e V and not for F = 5 0 M e V . The analysis for F = 5 0 MeV will soon be sent lor publication.