π and ρ mesons, and their diquark partners, from a contact interaction

被引:139
作者
Roberts, H. L. L. [1 ,2 ,3 ]
Bashir, A. [4 ,5 ]
Gutierrez-Guerrero, L. X. [4 ]
Roberts, C. D. [1 ,2 ,5 ,6 ,7 ]
Wilson, D. J. [1 ]
机构
[1] Argonne Natl Lab, Div Phys, Argonne, IL 60439 USA
[2] Forschungszentrum Julich, Inst Kernphys, D-52425 Julich, Germany
[3] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[4] Univ Michoacana, Inst Fis & Matemat, Morelia 58040, Michoacan, Mexico
[5] Kavli Inst Theoret Phys China, CAS, Beijing 100190, Peoples R China
[6] Peking Univ, Ctr High Energy Phys, Dept Phys, Beijing 100871, Peoples R China
[7] Peking Univ, State Key Lab Nucl Phys & Technol, Beijing 100871, Peoples R China
来源
PHYSICAL REVIEW C | 2011年 / 83卷 / 06期
关键词
ELECTROMAGNETIC FORM-FACTORS; DYSON-SCHWINGER EQUATIONS; CHIRAL-SYMMETRY BREAKING; ANOMALOUS GAMMA; BOUND-STATES; LIGHT; MODEL; QCD; NUCLEON; MASS;
D O I
10.1103/PhysRevC.83.065206
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
We present a unified Dyson-Schwinger equation treatment of static and electromagnetic properties of pseudoscalar and vector mesons, and scalar and axial-vector diquark correlations, based upon a vector-vector contact interaction. A basic motivation for this paper is the need to document a comparison between the electromagnetic form factors of mesons and those diquarks that play a material role in nucleon structure. A notable result, therefore, is the large degree of similarity between related meson and diquark form factors. The simplicity of the interaction enables computation of the form factors at arbitrarily large spacelike Q(2), which enables us to expose a zero in the rho-meson electric form factor at z(Q)(rho) approximate to root 6m(rho). Notably, r(rho)z(Q)(rho) approximate to r(D)z(Q)(D), where r(rho) and r(D) are, respectively, the electric radii of the rho-meson and deuteron.
引用
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页数:12
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