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Landau gauge gluon and ghost propagators at finite temperature from quenched lattice QCD
High Energy Physics - Lattice · Submitted 8 Aug 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Since the longitudinal component D_L(q) turns out to be most sensitive with respect to the phase transition we propose some combinations of D_L(q) signalling the transition much like "order parameters".
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The abstract, sentence by sentence
The behavior of the Landau gauge gluon and ghost propagators is studied in pure SU(3) gauge theory at non-zero temperature on the lattice. We concentrate on the momentum range [0.6, 2.0] GeV. For the longitudinal as well as for the transverse component of the gluon propagator we extract the continuum limit. We demonstrate the smallness of finite-size and Gribov-copy effects at temperatures close to the deconfinement phase transition at T=T_c and within the restricted range of momenta. Since the longitudinal component D_L(q) turns out to be most sensitive with respect to the phase transition we propose some combinations of D_L(q) signalling the transition much like "order parameters".
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The behavior of the Landau gauge gluon and ghost propagators is studied in pure SU(3) gauge theory at non-zero temperature on the lattice. | contribution 0.96 | 0.90 | 0.04 | asserted 0.93 |
| s1 | We concentrate on the momentum range [0.6, 2.0] GeV. | method 0.76 | 0.82 | 0.03 | asserted 0.85 |
| s2 | For the longitudinal as well as for the transverse component of the gluon propagator we extract the continuum limit. | method 0.58 | 0.95 | 0.10 | asserted 0.99 |
| s3 | We demonstrate the smallness of finite-size and Gribov-copy effects at temperatures close to the deconfinement phase transition at T=T_c and within the restricted range of momenta. | result 0.99 | 0.94 | 0.17 | asserted 1.00 |
| s4 | Since the longitudinal component D_L(q) turns out to be most sensitive with respect to the phase transition we propose some combinations of D_L(q) signalling the transition much like "order parameters". | interpretation 0.66 | 0.91 | 0.48 | asserted 0.48 |
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The paper
Original abstract
The behavior of the Landau gauge gluon and ghost propagators is studied in pure SU(3) gauge theory at non-zero temperature on the lattice. We concentrate on the momentum range [0.6, 2.0] GeV. For the longitudinal as well as for the transverse component of the gluon propagator we extract the continuum limit. We demonstrate the smallness of finite-size and Gribov-copy effects at temperatures close to the deconfinement phase transition at T=T_c and within the restricted range of momenta. Since the longitudinal component D_L(q) turns out to be most sensitive with respect to the phase transition we propose some combinations of D_L(q) signalling the transition much like "order parameters".
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References
How the literature uses it
34 arXiv papers cite this in 63 sentences
Papers citing it · 30 sentences without a confident label
Builds on it 1 paper
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Correspondingly we have started a lattice computation of gluon and ghost propagators at non-zero temperature, first in $SU(3)$ pure gauge theory [ref] and more recently for the full QCD case with two light flavor degrees of freedom [ref] .
Landau gauge gluon and ghost propagators from two-flavor lattice QCD at T > 0 · Introduction · 0.95
Uses its method or tool 6 papers
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As we see later, thanks to a nice parametrization of the propagators in Ref. [ref] , our practical strategy requires only minimal modifications in the model-study procedures.
Polyakov loop and QCD thermodynamics from the gluon and ghost propagators · Introduction · 0.80
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In order to suppress lattice effects we have applied momentum cuts as described in [ref] .
Lattice Landau gauge quark propagator at finite temperature · Results and Conclusions · 0.99
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At finite $T$, we project the Lorentz structure of the propagator $D^ab_μν(q̂)$ with two independent form factors, [equation] using transverse and longitudinal projectors in the Landau gauge [ref] , similar to magnetic and electric projectors respectively, [equation] [equation]
Gluon mass at finite temperature in Landau gauge · Gluon propagator at $T > 0$ · 0.97
Uses its data or values 3 papers
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In this work we use two sets of parameters at $T=0.86 T_c$ and $T=1.20 T_c$ taken from Ref. [ref] , which is listed in Tab. [ref].
Polyakov loop and QCD thermodynamics from the gluon and ghost propagators · Introduction · 1.00
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For the values reported in [ref] , our topological invariant acquires the following values: $N_Γ = 0$ whenever $b=0$ , since the propagator then displays only a (negative) real (double) pole.
Extracting topological information from momentum space propagators · A gluon propagator that fits lattice data · 0.99
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The lattice data [ref] show a cross-over type of signal in the ratio of the two inequivalent Lorentz structures for the gluon propagator, but no clear qualitative change at the deconfinement phase transition.
A covariant variational approach to Yang-Mills Theory at finite temperatures · Introduction · 0.89
Compares with it 10 papers
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The lattice study in Ref. [ref] , to which we compare, employs a similar prescription with $μ_∞= 5 GeV$.
A covariant variational approach to Yang-Mills Theory at finite temperatures · Numerical procedure at finite temperature · 0.85
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Both effects, the enhanced volume dependence and the temperature dependence agree with the situation in the quenched theory [ref] .
Finite-density gauge correlation functions in QC2D · Finite-temperature results · 0.94
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We made use of the rational function fits according to [ref] , and we could find a phase transition at a temperature within the range $T/T_c = 1.20$ and $T/T_c = 1.48$, which is slightly above the thermodynamic critical (deconfinement) temperature found by the authors.
Extracting topological information from momentum space propagators · Conclusions · 0.86
Cites it as support 1 paper
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The discrepancy above $∼1.2T_c$ should be attributed to the neglected $T$-dependence in the non-perturbative propagators as seen in Refs. [ref] .
Polyakov loop and QCD thermodynamics from the gluon and ghost propagators · Introduction · 1.00
Cites it as background 7 papers
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The lattice gluon propagator has oftentimes been interpreted in terms of the tree level predictions of the Gribov-Zwanziger action and its generalizations [ref] , with applications in [ref] .
High Precision Statistical Landau Gauge Lattice Gluon Propagator Computation vs. the Gribov-Zwanziger approach · Introduction · 0.99
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Lattice studies of the Landau-gauge gluon propagator around the deconfinement phase transition in pure $SU(2)$ and $SU(3)$ theory, as well as considering dynamical quarks, have been presented in [ref] .
Systematic Effects at Criticality for the SU(2)-Landau-Gauge Gluon Propagator · Gluon propagator at finite temperature · 0.99
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The Landau gauge gluon propagator has been studied using non-perturbative methods for a wide range of temperatures both for full QCD and for the pure gauge theory [ref] .
Finite Temperature Landau Gauge Lattice Quark Propagator · Introduction and Motivation · 0.93
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