% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Ferreira:364102,
author = {Ferreira, Mauricio N. and Papavassiliou, Joannis and
Pawlowski, Jan M. and Wink, Nicolas},
title = {{P}hysics of the gluon mass gap},
journal = {The European physical journal / C},
volume = {85},
number = {11},
issn = {1434-6044},
address = {Heidelberg},
publisher = {Springer},
reportid = {GSI-2026-00281, 2508.20568},
pages = {1339},
year = {2025},
note = {"This article is licensed under a Creative Commons
Attribution 4.0 International License, which permits use,
sharing, adaptation, distribution and reproduction in any
medium or format, as long as you give appropriate credit to
the original author(s) and the source, provide a link to the
Creative Commons licence, and indicate if changes were made.
The images or other third party material in this article are
included in the article’s Creative Commons licence, unless
indicated otherwise in a credit line to the material. If
material is not included in the article’s Creative Commons
licence and your intended use is not permitted by statutory
regulation or exceeds the permitted use, you will need to
obtain permission directly from the copyright holder. To
view a copy of this licence, visit
http://creativecommons.org/licenses/by/4.0/. Funded by
SCOAP3."},
abstract = {It has long been known that the gluon propagator in
Landau-gauge QCD exhibits a mass gap; and its emergence has
been ascribed to the action of the Schwinger mechanism in
the gauge sector of QCD. In the present work, we relate this
property to the physical mass gap of QCD by considering two
observables associated with confinement and chiral symmetry
breaking, namely the confinement-deconfinement transition
temperature and the pion decay constant, respectively. It
turns out that the first observable is linearly proportional
to the gluon mass gap, a fact that allows us to assign a
direct physical meaning to this scale. Moreover, we identify
three distinct momentum regimes in the gluon propagator,
ultraviolet, intermediate, and deep infrared, and assess
their impact on the aforementioned observables. Both
observables are sensitive to the first two regions of
momenta, where functional approaches essentially coincide,
but are insensitive to the third, deep infrared, regime. The
combined information is used for a simple fit for the gluon
propagator, all of whose parameters admit a clear physical
interpretation. Finally, we discuss how this fit can help us
access the intertwined dynamics of confinement and chiral
symmetry breaking in QCD-type theories.},
cin = {EXM},
ddc = {530},
cid = {I:(DE-Ds200)EXM-20080818OR100},
pnm = {612 - Cosmic Matter in the Laboratory (POF4-612) / SFB 1225
Z-V - Koordination des Sonderforschungsbereichs 1225
ISOQUANT (Z-V) (317302840) / DFG project G:(GEPRIS)390900948
- EXC 2181: STRUKTUREN: Emergenz in Natur, Mathematik und
komplexen Daten (390900948)},
pid = {G:(DE-HGF)POF4-612 / G:(GEPRIS)317302840 /
G:(GEPRIS)390900948},
experiment = {$EXP:(DE-Ds200)no_experiment-20200803$},
typ = {PUB:(DE-HGF)16},
UT = {WOS:001620913500002},
doi = {10.1140/epjc/s10052-025-15027-7},
url = {https://repository.gsi.de/record/364102},
}