Summary
The three-dimensional representations (orographs) of the total chromomagneto-electric self-energy {\(W\left( {\mathfrak{M},V} \right)\) and of the chromomagnetic selfenergy\(U\left( \mathfrak{M} \right)\) of a\(q\bar q\) system model are explored as functions of the chromomagnetization density\(\mathfrak{M}\), the chromo-electric potentialV and the temperatureT with the purpose of achieving a deeper understanding of the mathematical features of\(W\left( {\mathfrak{M},V} \right)\) and\(U\left( \mathfrak{M} \right)\) and of some aspects of the physical content concealed into the\(V_{q\bar q} \left( r \right)\) potential, deduced in a preceding note.
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References
T. A. Minelli, A. Pascolini andC. Villi:Nuovo Cimento A,106, 133 (1993); hereafter this paper will be referred to as [I].
T. A. Minelli, A. Pascolini andC. Villi:Nuovo Cimento A,104, 1589 (1991); hereafter this paper will be referred to as [A].
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Minelli, T.A., Pascolini, A. & Villi, C. Temperature dependence of chromomagneto-electric orographs of the self-energies of a\(q\bar q\) systemsystem. Nuov Cim A 106, 561–570 (1993). https://doi.org/10.1007/BF02782708
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DOI: https://doi.org/10.1007/BF02782708