Coulomb Confinement from the Yang-Mills Vacuum State in 2+1 Dimensions

Abstract

The Coulomb-gauge ghost propagator, and the color-Coulomb potential, are computed in an ensemble of configurations derived from our recently proposed Yang-Mills vacuum wavefunctional in 2+1 dimensions. The results are compared to the corresponding values obtained by standard Monte Carlo simulations in three Euclidean dimensions. The agreement is quite striking for the Coulomb-gauge ghost propagator. The color-Coulomb potential rises linearly at large distances, but its determination suffers from rather large statistical fluctuations, due to configurations with very low values of ${\mu }_0$, the lowest eigenvalue of the Coulomb-gauge Faddeev-Popov operator. However, if one imposes cuts on the data, effectively leaving out configurations with very low ${\mu }_0$, the agreement of the potential in both sets of configurations is again satisfactory, although the errorbars grow systematically as the cutoff is eliminated.

arXiv comment8 pages, 5 figures (10 EPS files), RevTeX4.1. V2: original figs. 4 and 5 compressed into a new fig. 5; a new fig. 4; sec. IV.B slightly modified to reflect the changes. Version to appear in Phys. Rev. D. V3: a reference corrected.

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• Testing the Yang-Mills vacuum wave functional Ansatz in 3+1 dimensions
• The Yang-Mills vacuum wave functional thirty-five years later
• In quest of the Yang-Mills vacuum wavefunctional
• Numerical study of the SU(2) Yang-Mills vacuum state: Much ado about nothing?
• The QCD vacuum wave functional and confinement in Coulomb gauge