Nucleon form factors in an independent-quark model based on Dirac equation with power-law potential

1986 ◽  
Vol 33 (1) ◽  
pp. 172-178 ◽  
Author(s):  
N. Barik ◽  
M. Das
1973 ◽  
Vol 8 (1) ◽  
pp. 11-15 ◽  
Author(s):  
V. F. Dushenko ◽  
A. P. Kobushkin ◽  
Yu. M. Sinjukov

2002 ◽  
Vol 66 (5) ◽  
Author(s):  
V. E. Lyubovitskij ◽  
P. Wang ◽  
Th. Gutsche ◽  
Amand Faessler

2005 ◽  
Vol 20 (08n09) ◽  
pp. 1785-1790 ◽  
Author(s):  
D. O. RISKA

The chiral quark model posits that pions couple to the axial current of constituent quarks. This chiral pion coupling governs the pion decays of baryon resonances and also implies pion and multipion interactions between the quarks. The qualitative features of this model for the description of pionic decay widths and baryon spectra are outlined. When the covariant quark model wave function for the nucleon is chosen so as to describe the empirical nucleon form factors the pion decay widths of the positive parity resonances are underpredicted. This indicates the presence of significant multiquark components in these resonances.


1998 ◽  
Vol 1 (3) ◽  
pp. 307-315 ◽  
Author(s):  
E. Santopinto ◽  
F. Iachello ◽  
M.M. Giannini

1990 ◽  
Vol 41 (5) ◽  
pp. 1568-1577 ◽  
Author(s):  
N. Barik ◽  
S. N. Jena ◽  
D. P. Rath

1970 ◽  
Vol 23 (5) ◽  
pp. 615 ◽  
Author(s):  
GB Smith ◽  
LJ Tassie

From the sum rules for hadron scattering, the nucleon form factors, and the masses of the hadrons, the properties of quarks are estimated as: 2 Ge V Jc2 ;:; quark mass ;:; 30 Ge V Jc2, 0�1 fm ;:; range of the quark-quark interaction ;:; 0�25 fm. The hadrons are described by a relativistic independent quark model using the Dirac equation with a potential energy term for the effective interaction.


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