The Quenched limit of lattice QCD at nonzero baryon number

Engels J, Kaczmarek O, Karsch F, Laermann E (1999)
Nucl.Phys. B 558(1-2): 307-326.

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Abstract
We discuss the thermodynamics of gluons in the background of static quark sources. In order to do so we formulate the quenched limit of QCD at non-zero baryon number. A first numerical analysis of this system shows that it undergoes a smooth deconfining transition. We find evidence for a region of coexisting phases that becomes broader with increasing baryon number density. Although the action is in our formulation explicitly Z(3) symmetric the Polyakov loop expectation value becomes non-zero already in the low temperature phase. It indicates that the heavy quark potential stays finite at large distances, ie. the string between static quarks breaks at non-zero baryon number density already in the hadronic phase.
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Engels J, Kaczmarek O, Karsch F, Laermann E. The Quenched limit of lattice QCD at nonzero baryon number. Nucl.Phys. B. 1999;558(1-2):307-326.
Engels, J., Kaczmarek, O., Karsch, F., & Laermann, E. (1999). The Quenched limit of lattice QCD at nonzero baryon number. Nucl.Phys. B, 558(1-2), 307-326.
Engels, J., Kaczmarek, O., Karsch, F., and Laermann, E. (1999). The Quenched limit of lattice QCD at nonzero baryon number. Nucl.Phys. B 558, 307-326.
Engels, J., et al., 1999. The Quenched limit of lattice QCD at nonzero baryon number. Nucl.Phys. B, 558(1-2), p 307-326.
J. Engels, et al., “The Quenched limit of lattice QCD at nonzero baryon number”, Nucl.Phys. B, vol. 558, 1999, pp. 307-326.
Engels, J., Kaczmarek, O., Karsch, F., Laermann, E.: The Quenched limit of lattice QCD at nonzero baryon number. Nucl.Phys. B. 558, 307-326 (1999).
Engels, Jürgen, Kaczmarek, Olaf, Karsch, Frithjof, and Laermann, Edwin. “The Quenched limit of lattice QCD at nonzero baryon number”. Nucl.Phys. B 558.1-2 (1999): 307-326.
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