SU 6 Quark model, nucleon resonance electroproduction and spin-dependent electroproduction structure functions

1974 ◽  
Vol 23 (1) ◽  
pp. 103-125
Author(s):  
H. Osborn ◽  
G. Woo
1983 ◽  
Vol 27 (4) ◽  
pp. 1561-1571 ◽  
Author(s):  
L. S. Celenza ◽  
C. M. Shakin

1989 ◽  
Vol 39 (6) ◽  
pp. 2477-2477 ◽  
Author(s):  
L. S. Celenza ◽  
C. M. Shakin

2009 ◽  
Vol 831 (3-4) ◽  
pp. 243-262 ◽  
Author(s):  
M.M. Yazdanpanah ◽  
A. Mirjalili ◽  
S. Atashbar Tehrani ◽  
F. Taghavi-Shahri

1992 ◽  
Vol 01 (03) ◽  
pp. 505-524 ◽  
Author(s):  
ROBERT D. CARLITZ

These lectures discuss the substructure of the nucleon, first on the scale of 1 fermi and then at much shorter distances. We review relevant features of the quark model and introduce Quantum Chromodynamics and the idea of a running coupling. Recent data involving polarized protons is discussed in this framework, and an outlook is presented for future experiments relating to the spin substructure of the nucleon.


2010 ◽  
Vol 19 (08n10) ◽  
pp. 1697-1701 ◽  
Author(s):  
C. MÍREZ ◽  
L. TOMIO ◽  
L. A. TREVISAN ◽  
T. FREDERICO

The neutron-to-proton ratio of the structure functions, [Formula: see text], as well as the corresponding difference [Formula: see text] are obtained within a statistical quark model for the nucleon, where the quark energy levels are given by a central linear confining potential.


2014 ◽  
Vol 29 ◽  
pp. 1460235 ◽  
Author(s):  
Jun He

The Λ(1520) photoproduction from proton target is investigated within the effective Lagrangian method and well compared with the experimental data. The D13 state N(2120) plays the most important role among the nucleon resonances. Besides N(2120), a nucleon resonance [Formula: see text] predicted by the constituent quark model is found also important to reproduce the experimental data. Other nucleon resonances give negligible contributions in the channel considered in this work.


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