2024 Impact factor 4.8
Particles and Fields
Eur. Phys. J. C 7, 279-288
DOI 10.1007/s100529801019

Nonperturbative corrections of quark and gluon condensates to QCD inspired quark potentials

J.J. Yang1,2,3 - H.Q. Shen1 - G.L. Li2,3 - T. Huang2,3 - P.N. Shen2,3

1 Department of Physics, Nanjing Normal University, Nanjing 210097, China
2 China Center of Advanced Science and Technology (World Laboratory), P.O.Box 8730, Beijing 100080, China
3 Institute of High Energy Physics, Academia Sinica, P.O.Box 918(4), Beijing 100039, China

Received: 22 June 1998 / Revised version: 10 August 1998 / Published online: 29 October 1998

Abstract
We adopt the Lorentz gauge to derive the non-local two-gluon vacuum expectation value (VEV) with translational invariance. By means of the obtained non-local two-gluon VEV, the leading nonperturbative QCD corrections to one gluon exchange quark-quark, quark-antiquark and $q \bar{q}$ pair-excitation potentials are given by employing non-vanishing vacuum condensates of quarks and gluons to modify the free gluon propagator. The linear, cubic and Yukawa-type terms in quark-quark potential appear automatically. In the $q \bar{q}$ pair-excitation potential with $\omega_q=0$, the linear, square and cubic terms arise from the nonzero quark and gluon condensates.


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