scholarly journals Nucleon–meson coupling constants and form factors in the quark model

2006 ◽  
Vol 638 (5-6) ◽  
pp. 455-460 ◽  
Author(s):  
C. Downum ◽  
T. Barnes ◽  
J.R. Stone ◽  
E.S. Swanson
1967 ◽  
Vol 48 (2) ◽  
pp. 570-572 ◽  
Author(s):  
P. A. Cook

2012 ◽  
Vol 27 (05) ◽  
pp. 1250022
Author(s):  
N. GHAHRAMANY ◽  
R. KHOSRAVI ◽  
M. JANBAZI

The structure of the Ds1(2460) meson has not yet been exactly known in the quark model. Considering the Ds1 meson as a conventional [Formula: see text] meson, we investigate the strong form factors and coupling constants gDs1D*K and [Formula: see text] in the framework of the three point QCD sum rules. Any future experimental measurement on these form factors as well as coupling constants gDs1D*K and [Formula: see text] and their comparison with the obtained results in the present work can give considerable information about the structure of this meson.


1998 ◽  
Vol 07 (01) ◽  
pp. 69-88 ◽  
Author(s):  
S. N. Jena ◽  
M. R. Behera

Nucleon charge and magnetic form factors [Formula: see text] are computed in an independent-quark model with an equally mixed scalar and vector confining potential in square root form taking into account the corrections due to center-of-mass motion and pion-clound effects. The values obtained for the nucleon static properties such as the magnetic moment, charge radius and axial vector coupling constant in the neutron beta decay process agree reasonably with the corresponding experimental data. The pseudo-scalar and pseudo-vector pion-nucleon coupling constants are found to be gNNπ=13.43 and fNNπ=0.282, which are in excellent agreement with the experimental data.


1992 ◽  
Vol 07 (27) ◽  
pp. 6813-6831 ◽  
Author(s):  
N. BARIK ◽  
S.N. JENA ◽  
D.P. RATH

Incorporating corrections for the center-of-mass motion and pion-cloud effects the nucleon electromagnetic form factors [Formula: see text] are computed in an independent quark model based on the Dirac equation with a confining potential [Formula: see text] The static quantities like magnetic moment μN, charge radius [Formula: see text] and axial vector coupling constant (gA)n→peν of the nucleons computed in this model are in reasonable agreement with the experiment. The pseudoscalar and the pseudovector pion-nucleon coupling constants are obtained as gNNπ=13.52 and fNNπ=0.284, which are in excellent agreement with the experimental data.


2001 ◽  
Vol 511 (1) ◽  
pp. 33-39 ◽  
Author(s):  
R.F. Wagenbrunn ◽  
S. Boffi ◽  
W. Klink ◽  
W. Plessas ◽  
M. Radici

1973 ◽  
Vol 8 (1) ◽  
pp. 11-15 ◽  
Author(s):  
V. F. Dushenko ◽  
A. P. Kobushkin ◽  
Yu. M. Sinjukov

2001 ◽  
Vol 64 (11) ◽  
Author(s):  
C. Q. Geng ◽  
C. W. Hwang ◽  
C. C. Lih ◽  
W. M. Zhang

2007 ◽  
Vol 76 (6) ◽  
Author(s):  
M. De Sanctis ◽  
M. M. Giannini ◽  
E. Santopinto ◽  
A. Vassallo

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