Abstract
By means of functional integral techniques, QCD is converted into a quantum hadrodynamics, an effective theory of interacting mesons and baryons. While mesons appear as composite quark antiquark fields baryons are buil up from diquark fields in the \(\bar 3_c\) representation plus a quark. In the large N c limit the diquark correlations disappear and the effective hadron theory becomes an effective meson theory where baryons appear as chiral solitons. Numerical results are presented for the s = 1/2 baryon octet.
supported by Deutsche Forschungsgemeinschaft under contract Re 856/2-1 and by COSY under contract 41170833
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© 1993 Springer Verlag
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Reinhardt, H. (1993). Hadronization of QCD. In: Goeke, K., Kroll, P., Petry, HR. (eds) Quark Cluster Dynamics. Lecture Notes in Physics, vol 417. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-56437-3_55
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DOI: https://doi.org/10.1007/3-540-56437-3_55
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