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Analytic calculation of color-Coulomb potential and color confinement
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abstract
We develop a calculational scheme in Coulomb and temporal gauge that respects gauge invariance and is most easily applied to the infrared asymptotic region of QCD. It resembles the Dyson-Schwinger equations of Euclidean quantum field theory in Landau gauge, but is 3-dimensional. A simple calculation yields a color-Coulomb potential that behaves at large $R$ approximately like $V_{\rm coul}(R) \sim R^{[1-0.2(d-1)]}$ for spatial dimension $1 \leq d \leq 3$. This is a linearly rising potential plus a rather weak dependence on $d$.
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Cited by 1 Pith paper
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The Coulomb flux tube revisited
Lattice data at beta=2.5 and 2.7 favor a power-law transverse falloff of the Coulomb flux tube, with exponent near 2, instead of the exponential falloff reported at beta=2.5 by Chung and Greensite.
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