Low-Lying Dirac Eigenmodes, Topological Charge Fluctuations and the Instanton Liquid Model.pdf
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Low-Lying Dirac Eigenmodes, Topological Charge Fluctuations and the Instanton Liquid Model
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LOW-LYING DIRAC EIGENMODES, TOPOLOGICAL CHARGE
FLUCTUATIONS AND THE INSTANTON LIQUID MODEL
I. HORVA?TH, S.J. DONG, T. DRAPER
Department of Physics Astronomy
University of Kentucky, Lexington, KY 40503, USA
F.X. LEE
Center for Nuclear Studies and Department of Physics
George Washington University
Washington, DC 20052, USA, and
Jefferson Laboratory, Newport News, VA 23606, USA
H.B. THACKER
Department of Physics
University of Virginia, Charlottesville, VA 22901, USA
AND
J.B. ZHANG
CSSM and Department of Physics and Mathematical Physics
University of Adelaide, Adelaide, SA 5005, Australia
Abstract. The local structure of low-lying eigenmodes of the overlap Dirac
operator is studied. It is found that these modes cannot be described as
linear combinations of ’t Hooft “would-be” zeromodes associated with in-
stanton excitations that underly the Instanton Liquid Model. This implies
that the instanton liquid scenario for spontaneous chiral symmetry break-
ing in QCD is not accurate. More generally, our data suggests that the
vacuum fluctuations of topological charge are not effectively dominated by
localized lumps of unit charge with which the topological “would-be” zero-
modes could be associated.
Presented by I. Horva?th at the NATO Advanced Research Workshop “Confinement,
Topology, and other Non-Perturbative Aspects of QCD”, January 21-27, 2002, Stara?
Lesna? (Slovakia).
21. Introduction
The idea of the instanton-dominated QCD vacuum appeared shortly af-
ter the discovery of the instanton [1]. In particular, the instanton gas pic-
ture [2] populates the vacuum with well-separated instantons which, using
semiclassical methods, leads to the possible qualitative resolution of the
U(1) problem [3], as well as to the conclusion that QCD physics depends
on the θ-parameter [4]. However, it became clear very soon that QCD is
not semiclassical in this sense because the instanton gas picture does not
lead to confin
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