An Analytic Expression for Non-Singlet Component of Nucleon Structure Functions to the Next Order Effects

1983 ◽  
Vol 2 (2) ◽  
pp. 965-970
Author(s):  
Lu Jing-xian ◽  
Wu Chi-min ◽  
Zhao Pei-ying
1987 ◽  
Vol 193 (2-3) ◽  
pp. 368-372 ◽  
Author(s):  
P. Bordalo ◽  
Ph. Busson ◽  
L. Kluberg ◽  
A. Romana ◽  
R. Salmeron ◽  
...  

1994 ◽  
Vol 50 (7) ◽  
pp. 4718-4718 ◽  
Author(s):  
X. Song ◽  
J. S. McCarthy

1983 ◽  
Vol 123 (3-4) ◽  
pp. 275-278 ◽  
Author(s):  
J.J. Aubert ◽  
G. Bassompierre ◽  
K.H. Becks ◽  
C. Best ◽  
E. Böhm ◽  
...  

1995 ◽  
Vol 343 (1-4) ◽  
pp. 369-376 ◽  
Author(s):  
E Stein ◽  
P Górnicki ◽  
L Mankiewicz ◽  
A Schäfer ◽  
W Greiner

1983 ◽  
Vol 27 (4) ◽  
pp. 1561-1571 ◽  
Author(s):  
L. S. Celenza ◽  
C. M. Shakin

1992 ◽  
Vol 01 (04) ◽  
pp. 809-821 ◽  
Author(s):  
BO-QIANG MA

The off-shell behaviors of bound nucleons in deep inelastic lepton nucleus scattering are discussed in two scenarios with the basic constituents chosen to be baryon-mesons and quark-gluons respectively in light-cone formalism. It is found that when taking into account the effect due to internal quark structure of nucleons, the derived scaling variable for bound nucleons and the calculated nuclear structure functions are different from those in considering the baryon-mesons as the effective elementary constituents. This implies that the pure baryon-meson descriptions of nuclei give the inaccurate off-shell behavior of the bound nucleon structure function, thereby the quark-gluons seem to be the most appropriate degrees of freedom for nuclear descriptions.


2010 ◽  
Vol 19 (10) ◽  
pp. 1893-1921 ◽  
Author(s):  
J.-P. CHEN

Nucleon structure study is one of the most important research areas in modern physics and has challenged us for decades. Spin has played an essential role and often brought surprises and puzzles to the investigation of the nucleon structure and the strong interaction. New experimental data on nucleon spin structure at low to intermediate momentum transfers combined with existing high momentum transfer data offer a comprehensive picture in the strong region of the interaction and of the transition region from the strong to the asymptotic-free region. Insight into some aspects of the theory for the strong interaction, Quantum Chromodynamics (QCD), is gained by exploring lower moments of spin structure functions and their corresponding sum rules (i.e., the Bjorken, Burkhardt–Cottingham, Gerasimov–Drell–Hearn (GDH), and the generalized GDH). These moments are expressed in terms of an operator-product expansion using quark and gluon degrees of freedom at moderately large momentum transfers. The higher-twist contributions have been examined through the evolution of these moments as the momentum transfer varies from higher to lower values. Furthermore, QCD-inspired low-energy effective theories, which explicitly include chiral symmetry breaking, are tested at low momentum transfers. The validity of these theories is further examined as the momentum transfer increases to moderate values. It is found that chiral perturbation theory calculations agree reasonably well with the first moment of the spin structure function g1 at low momentum transfer of 0.05–0.1 GeV2 but fail to reproduce some of the higher moments, noticeably, the neutron data in the case of the generalized polarizability δLT. The Burkhardt–Cottingham sum rule has been verified with good accuracy in a wide range of Q2 assuming that no singular behavior of the structure functions is present at very high excitation energies.


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