# The nonzero baryon number formulation of QCD

Engels J, Kaczmarek O, Karsch F, Laermann E (2000)
Nucl.Phys.Proc.Suppl. 83: 369-371.

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We discuss the non-zero baryon number formulation of QCD in the quenched limit at finite temperature. This describes the thermodynamics of gluons in the background of static quark sources. Although a sign problem remains in this theory, our simulation results show that it can be handled quite well numerically. The transition region gets shifted to smaller temperatures and the transition region broadens with increasing baryon number. 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 and the heavy quark potential gets screened at non-vanishing number density already this phase.
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Engels J, Kaczmarek O, Karsch F, Laermann E. The nonzero baryon number formulation of QCD. Nucl.Phys.Proc.Suppl. 2000;83:369-371.
Engels, J., Kaczmarek, O., Karsch, F., & Laermann, E. (2000). The nonzero baryon number formulation of QCD. Nucl.Phys.Proc.Suppl., 83, 369-371. doi:10.1016/S0920-5632(00)91676-1
Engels, J., Kaczmarek, O., Karsch, F., and Laermann, E. (2000). The nonzero baryon number formulation of QCD. Nucl.Phys.Proc.Suppl. 83, 369-371.
Engels, J., et al., 2000. The nonzero baryon number formulation of QCD. Nucl.Phys.Proc.Suppl., 83, p 369-371.
J. Engels, et al., “The nonzero baryon number formulation of QCD”, Nucl.Phys.Proc.Suppl., vol. 83, 2000, pp. 369-371.
Engels, J., Kaczmarek, O., Karsch, F., Laermann, E.: The nonzero baryon number formulation of QCD. Nucl.Phys.Proc.Suppl. 83, 369-371 (2000).
Engels, Jürgen, Kaczmarek, Olaf, Karsch, Frithjof, and Laermann, Edwin. “The nonzero baryon number formulation of QCD”. Nucl.Phys.Proc.Suppl. 83 (2000): 369-371.
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