Magnetic moments of octet baryons in a chiral potential model

Pramana ◽  
1986 ◽  
Vol 27 (6) ◽  
pp. 783-793 ◽  
Author(s):  
N Barik ◽  
M Das
1995 ◽  
Vol 359 (3-4) ◽  
pp. 288-294 ◽  
Author(s):  
Georg Wagner ◽  
Alfons J Buchmann ◽  
Amand Faessler

1994 ◽  
Vol 09 (03) ◽  
pp. 327-339 ◽  
Author(s):  
N. BARIK ◽  
S.N. JENA ◽  
D.P. RATH

The magnetic moments of the octet baryons are calculated in a chiral symmetric inde-pendent quark potential model of the form [Formula: see text] The residual interaction arising from the quark-pion coupling over and above the dominant confining one represented by this phenomenological potential, is treated as a low order perturbation. The correction due to center of mass motion is also taken into account appropriately. The results are in reasonable agreement with the experimental data.


2010 ◽  
Vol 81 (1) ◽  
Author(s):  
A. Bhattacharya ◽  
A. Sagari ◽  
B. Chakrabarti ◽  
S. Mani

1988 ◽  
Vol 205 (2-3) ◽  
pp. 128-134 ◽  
Author(s):  
Kazuo Tsushima ◽  
Tetsuya Yamaguchi ◽  
Makoto Takizawa ◽  
Y. Kohyama ◽  
K. Kubodera

1992 ◽  
Vol 07 (12) ◽  
pp. 2841-2861 ◽  
Author(s):  
S. N. JENA ◽  
S. PANDA

A simple independent-quark model based on the Dirac equation with an equally mixed scalar–vector linear confining potential model is used to obtain a fit for the electromagnetic properties — like the magnetic moments, charge radii and axial-vector coupling-constant ratios — of octet baryons, taking into account the appropriate center-of-mass corrections. This fit is extended to include the quark-core contributions to the nucleon electromagnetic form factors [Formula: see text], [Formula: see text], [Formula: see text] and the axial-vector form factor GA(q2). The respective root-mean-square radii associated with [Formula: see text] and GA(q2) come out as [Formula: see text] and [Formula: see text]. The possibility of restoring in this model the chiral symmetry in the usual way is discussed and the pion-nucleon coupling constant is found as gπ NN = 13.72 as compared to (gπ NN ) exp ≃ 13.


1993 ◽  
Vol 08 (25) ◽  
pp. 4563-4576 ◽  
Author(s):  
S.N. JENA ◽  
S. PANDA

Under the assumption that baryons are an assembly of independent quarks confined in a first approximation by an effective potential [Formula: see text], which presumably represents the nonperturbative gluon interactions, the magnetic moments of octet baryons have been calculated by considering perturbatively the contributions of the residual quark-pion coupling arising out of the requirement of chiral symmetry over and above the necessary center-of-mass correction. The results so obtained agree quite well with the corresponding experimental values.


Pramana ◽  
1995 ◽  
Vol 44 (2) ◽  
pp. 145-152 ◽  
Author(s):  
N Barik ◽  
P Das ◽  
A R Panda

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