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G. ’t Hooft, in Recent Developments in Gauge Theories, edited by G. ’t Hooft et al. (Plenum, New York, 1980).
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25
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85039024396
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For an attempt to define an order parameter in the presence of dynamical quarks, see Ref. 24
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For an attempt to define an order parameter in the presence of dynamical quarks, see Ref. 24.
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28
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85039032645
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J. Zinn-Justin, Quantum Field Theory and Critical Phenomena, 3rd ed. (Oxford University Press, Oxford, 1996)
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J. Zinn-Justin, Quantum Field Theory and Critical Phenomena, 3rd ed. (Oxford University Press, Oxford, 1996).
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29
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85039013968
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The state created by the operator (Formula presented) is often referred as a “gluelump” in distinction from a “glueball” 28. However, we expect that the difference vanishes near the critical point. Note that in practical lattice simulations the specific heat is measured from the integrated correlator of plaquettes which excite glueballs
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The state created by the operator (Formula presented) is often referred as a “gluelump” in distinction from a “glueball” 28. However, we expect that the difference vanishes near the critical point. Note that in practical lattice simulations the specific heat is measured from the integrated correlator of plaquettes which excite glueballs.
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35
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85038995622
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Due to the very small critical exponent (Formula presented) the correct singularity in the specific heat has not been confirmed on the lattice so far. See, however, Ref. 34
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Due to the very small critical exponent (Formula presented) the correct singularity in the specific heat has not been confirmed on the lattice so far. See, however, Ref. 34.
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