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Polyakov loop information


In quantum field theory, the Polyakov loop is the thermal analogue of the Wilson loop, acting as an order parameter for confinement in pure gauge theories at nonzero temperatures. In particular, it is a Wilson loop that winds around the compactified Euclidean temporal direction of a thermal quantum field theory. It indicates confinement because its vacuum expectation value must vanish in the confined phase due to its non-invariance under center gauge transformations. This also follows from the fact that the expectation value is related to the free energy of individual quarks, which diverges in this phase. Introduced by Alexander M. Polyakov in 1975,[1] they can also be used to study the potential between pairs of quarks at nonzero temperatures.

  1. ^ Polyakov, A.M. (1978). "Compact gauge fields and the infrared catastrophe". Physics Letters B. 59 (1): 82–84. doi:10.1016/0370-2693(75)90162-8.

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Polyakov loop

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1103/PhysRevD.73.014019. Rößner, S.; Ratti, C.; Weise, W. (8 February 2007). "Polyakov loop, diquarks, and the two-flavor phase diagram". Physical Review D. 75...

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theory can be said to be defined by the path integral quantization of the Polyakov action: I 0 [ g , X ] = T 8 π ∫ M d 2 ξ g g m n ∂ m x μ ∂ n x ν G μ ν (...

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ISBN 0-521-63303-6. Vol. 2: Superstring theory and beyond. ISBN 0-521-63304-4. Polyakov, A.M. (1981). "Quantum geometry of bosonic strings". Physics Letters B...

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elaborated in articles by Steven Gubser, Igor Klebanov, and Alexander Markovich Polyakov, and by Edward Witten. By 2010, Maldacena's article had over 7000 citations...

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theory known as string theory. These theories are without supersymmetry. Polyakov action Nambu-Goto action Bosonic string theory Kondo model (s-d model)...

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≤ σ < 2 π {\displaystyle 0\leq \sigma <2\pi } . In order to define the Polyakov action, the world-sheet is equipped with a world-sheet metric g {\displaystyle...

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