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Unquenched quark model for baryons: Magnetic moments, spins, and orbital angular momenta

R. Bijker and E. Santopinto
Phys. Rev. C 80, 065210 – Published 31 December 2009

Abstract

We present an unquenched quark model for baryons in which the effects of the quark-antiquark pairs (uu¯, dd¯, and ss¯) are taken into account in an explicit form via a microscopic, QCD-inspired, quark-antiquark creation mechanism. In the present approach, the contribution of the quark-antiquark pairs can be studied for any inital baryon and for any flavor of the qq¯ pairs. It is shown that, while the inclusion of the qq¯ pairs does not affect the baryon magnetic moments, it leads to a sizable contribution of the orbital angular momentum to the spin of the proton and the Λ hyperon.

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  • Received 23 October 2009

DOI:https://doi.org/10.1103/PhysRevC.80.065210

©2009 American Physical Society

Authors & Affiliations

R. Bijker*

  • Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, A.P. 70-543, 04510 México, D. F., México

E. Santopinto

  • I. N. F. N., Sezione di Genova, via Dodecaneso 33, I-16146, Italy

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Issue

Vol. 80, Iss. 6 — December 2009

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Images

  • Figure 1
    Figure 1
    The helicity amplitudes as a function of Q2 for the D13(1520) resonance. Experimental data [10] are compared with theoretical predictions from the collective U(7) model [6] (dotted line) and the hypercentral model [7] (solid line). The dashed line corresponds to a fit to the experimental data.Reuse & Permissions
  • Figure 2
    Figure 2
    Quark line diagrams for ABC with qq¯=ss¯ and q1q2q3=uud.Reuse & Permissions
  • Figure 3
    Figure 3
    Magnetic moments of octet baryons: experimental values from the Particle Data Group [34] (circles), CQM (squares), and unquenched quark model (triangles).Reuse & Permissions
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