# Polyakov loop in different representations of SU(3) at finite temperature

Gupta S, Hübner KA, Kaczmarek O (2007)
Nucl.Phys. 785(1-2): 278-281.

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Journal Article | Original Article | Published | English

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We investigate the Polyakov loop in different representations of SU(3) in pure gauge at finite $T$. We discuss Casimir scaling for the Polyakov loop in the deconfined phase and test and generalize the renormalization procedure for the Polyakov loop from (Kaczmarek:2002mc) to arbitrary representations. In the confined phase we extract the renormalized adjoint Polyakov loop, which is finite in the thermodynamic limit. For our numerical calculations we used the tree-level improved Symanzik action on $32^3\times 4,6,8$ lattices.
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Gupta S, Hübner KA, Kaczmarek O. Polyakov loop in different representations of SU(3) at finite temperature. Nucl.Phys. 2007;785(1-2):278-281.
Gupta, S., Hübner, K. A., & Kaczmarek, O. (2007). Polyakov loop in different representations of SU(3) at finite temperature. Nucl.Phys., 785(1-2), 278-281. doi:10.1016/j.nuclphysa.2006.11.160
Gupta, S., Hübner, K. A., and Kaczmarek, O. (2007). Polyakov loop in different representations of SU(3) at finite temperature. Nucl.Phys. 785, 278-281.
Gupta, S., Hübner, K.A., & Kaczmarek, O., 2007. Polyakov loop in different representations of SU(3) at finite temperature. Nucl.Phys., 785(1-2), p 278-281.
S. Gupta, K.A. Hübner, and O. Kaczmarek, “Polyakov loop in different representations of SU(3) at finite temperature”, Nucl.Phys., vol. 785, 2007, pp. 278-281.
Gupta, S., Hübner, K.A., Kaczmarek, O.: Polyakov loop in different representations of SU(3) at finite temperature. Nucl.Phys. 785, 278-281 (2007).
Gupta, Sourendu, Hübner, Kay A., and Kaczmarek, Olaf. “Polyakov loop in different representations of SU(3) at finite temperature”. Nucl.Phys. 785.1-2 (2007): 278-281.
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