2019
DOI: 10.1103/physrevd.100.094037
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Spectral dimension as a tool for analyzing nonperturbative propagators

Abstract: We derive general properties of the scale-dependent effective spectral dimensions of nonperturbative gauge boson propagators as they appear as solutions from different methods in Yang-Mills theories. In the ultraviolet and for short timescales the anomalous dimensions of the propagators lead to a slight decrease of the spectral dimension as compared to the one of a free propagator. Lowering the momentum scale, the spectral dimension decreases further. The class of propagators which display a maximum at Euclide… Show more

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Cited by 13 publications
(8 citation statements)
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References 84 publications
(135 reference statements)
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“…The appearance of this maximum is inextricably connected with the presence of the unprotected logarithm originating from the ghost loop. In addition to confirming the known nonperturbative behavior of the ghost propagator in Euclidean space (i.e., absence of a "ghost mass"), it has a direct implication on the general analytic structure of the gluon propagator [48,93]. In particular, from the standard Källén-Lehmann representation [94,95]…”
Section: A Basic Concepts and Key Relationsmentioning
confidence: 80%
“…The appearance of this maximum is inextricably connected with the presence of the unprotected logarithm originating from the ghost loop. In addition to confirming the known nonperturbative behavior of the ghost propagator in Euclidean space (i.e., absence of a "ghost mass"), it has a direct implication on the general analytic structure of the gluon propagator [48,93]. In particular, from the standard Källén-Lehmann representation [94,95]…”
Section: A Basic Concepts and Key Relationsmentioning
confidence: 80%
“…In particular, the gluon propagator has a shallow/pronounced maximum from which it follows immediately that it violates positivity. Note that such a property also leads to a spectral dimension of one in the deep IR [83]. Correspondingly, if the maximum vanished, this would imply a qualitative change of the type of solution, and it is reassuring that we do not observe that.…”
Section: Resultsmentioning
confidence: 73%
“…This also explains why the maximum in the gluon propagator is difficult to observe in lattice results for four dimensions [64,67,69]. In general, however, there are additional arguments for the existence of a maximum from both continuum analyses, e.g., [99,113] and from three-dimensional lattice calculations, e.g., [96,114,115]. The observed maximum in the gluon propagator directly leads to a violation of positivity of the spectral function, see, e.g., [94,99,116,117].…”
Section: A Propagatorsmentioning
confidence: 97%
“…For the Higgs-type solutions, the maximum is at zero. The existence of a maximum at nonvanishing momenta does not only lead to positivity violation of the propagator [15], it also reduces the spectral dimension, viz., the dimension felt by the propagator [99], from four to one. The calculations in this work span solutions from scaling to the boundary of the Higgs-branch.…”
Section: Renormalizationmentioning
confidence: 99%
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