scholarly journals A Cloudy Quark Bag Model of S, P, and D wave interactions for the coupled channel antikaon-nucleon system

1992 ◽  
Author(s):  
Guangliang. He
1995 ◽  
Vol 585 (1-2) ◽  
pp. 379-380 ◽  
Author(s):  
Guangliang He ◽  
Rubin H. Landau
Keyword(s):  

1974 ◽  
Vol 9 (1) ◽  
pp. 56-68 ◽  
Author(s):  
F. S. Chwieroth ◽  
Y. C. Tang ◽  
D. R. Thompson

2014 ◽  
Vol 26 ◽  
pp. 1460061
Author(s):  
E. J. GARZON ◽  
JUJUN XIE ◽  
E. OSET

Using an interaction extracted from the local hidden gauge Lagrangians and the coupled channels ρN (s-wave), πN (d-wave), πΔ (s-wave) and πΔ (d-wave), we look in the region of [Formula: see text] and we find two resonances dynamically generated which are naturally associated to the N*(1520)(3/2-) and N*(1700)(3/2-). The N*(1700)(3/2-) appears neatly as a pole in the complex plane. The free parameters of the theory are chosen to fit the πN (d-wave) data. The unitary coupled channel approach followed here, in connection with the experimental data, leads automatically to a pole in the 1700 MeV region and makes this second 3/2- resonance unavoidable.


2009 ◽  
Vol 24 (11n13) ◽  
pp. 785-790 ◽  
Author(s):  
A. DELTUVA ◽  
A. C. FONSECA ◽  
P. U. SAUER

The four-nucleon bound state and scattering below three-body breakup threshold are described. The description is based on a realistic coupled-channel potential which allows the excitation of a single nucleon to a Δ isobar. In the four-nucleon system the Δ isobar mediates effective two-, three- and four-nucleon forces. The effect of the four-nucleon force is found to be much smaller than the effect of the three-nucleon force.


2005 ◽  
Vol 20 (08n09) ◽  
pp. 1826-1829
Author(s):  
M. J. VICENTE VACAS ◽  
E. OSET ◽  
SOURAV SARKAR

The s-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons is studied in a unitarized coupled channel approach. We obtain a fair agreement for mass and width of several [Formula: see text] resonances. In particular, the Ξ(1820), the Λ(1520) and the Σ(1670) states are well reproduced. Other resonances are predicted and also the couplings of the observed resonances to the various channels are evaluated.


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