C. P. Singh
Panjab University, Chandigarh
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Featured researches published by C. P. Singh.
Pramana | 1979
C. P. Singh; Ramesh C. Verma; M. P. Khanna
Assuming that the anomalous magnetic moment interaction has the formaT11 +bT22 +cT44 +sTαα in SU(4), which may arise due to symmetry breaking or some other dynamical effects, we have obtained the magnetic moments and the transition moments of the ordinary and charmed baryons.
Pramana | 1980
C. P. Singh; Satish Kanwar; M. P. Khanna
We use the quark model considerations of Federman, Rubinstein and Talmi and the relation (mψ/mϕ)≃(mϒ/mψ)≃(mϒ/mϒ) to compute the masses of beautiful and tasty vector mesons.
Pramana | 1981
C. P. Singh
We use broken SU(6) internal symmetry to derive the mass formulas amongst hadrons (1/2+, 3/2+, 0−, 1−) including second order mass contributions from symmetric 405 representation. Some hybrid mass relations are also obtained by relating second order parameters.
Pramana | 1981
C. P. Singh; Avinash Sharma; M. P. Khanna
Employing non-relativistic quasinuclear coloured quark model, which provides a unified description of mesons and baryons, masses of charmed andb-quark hadrons are studied. Various mass splittings are estimated, and mass relations among them are obtained.
Physical Review D | 1981
C. P. Singh; Avinash Sharma; M. P. Khanna
The phenomenology of a quantum-chromodynamics-based constituent-quark model is employed to estimate the electromagnetic mass differences of the b-quark hadrons. The sign of D/sup -//sub b/-D/sup 0//sub b/ is found to be negative.
Physical Review D | 1984
P. K. Chatley; C. P. Singh; M. P. Khanna
Physical Review D | 1982
C. P. Singh; Avinash Sharma
Physical Review D | 1981
C. P. Singh
Physical Review D | 1981
C. P. Singh; Satish Kanwar; M. P. Khanna
Physical Review D | 1980
C. P. Singh; Ramesh C. Verma; M. P. Khanna