Static Three-Body Potential in Baryons
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Abstract
The first principle of quantum chromodynamics is used to calculate the static perturbative three-body potential between three valence quarks in baryons, which is gauge invariant and flavor-dependent, and of magnitude of the same order as the next non-leading static q-q potential. Its effect on an S-state baryon composed of three valence quarks of equal mass may be viewed as a slight increase of the constituent quark masses with respect to those in mesons.
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Cite this article:
LIU Jue-ping, WANG Ping. Static Three-Body Potential in Baryons[J]. Chin. Phys. Lett., 1998, 15(8): 555-557.
LIU Jue-ping, WANG Ping. Static Three-Body Potential in Baryons[J]. Chin. Phys. Lett., 1998, 15(8): 555-557.
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LIU Jue-ping, WANG Ping. Static Three-Body Potential in Baryons[J]. Chin. Phys. Lett., 1998, 15(8): 555-557.
LIU Jue-ping, WANG Ping. Static Three-Body Potential in Baryons[J]. Chin. Phys. Lett., 1998, 15(8): 555-557.
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