2005
DOI: 10.1016/j.physletb.2005.04.076
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The negativity of the overlap-based topological charge density correlator in pure-glue QCD and the non-integrable nature of its contact part

Abstract: We calculate the lattice two-point function of topological charge density in pure-glue QCD using the discretization of the operator based on the overlap Dirac matrix. Utilizing data at three lattice spacings it is shown that the continuum limit of the correlator complies with the requirement of non-positivity at non-zero distances. For our choice of the overlap operator and the Iwasaki gauge action we find that the size of the positive core is ≈ 2 a (with a being the lattice spacing) sufficiently close to the … Show more

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Cited by 56 publications
(104 citation statements)
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“…The recent Monte Carlo studies of pure glue gauge theory have revealed a laminar structure in the vacuum consisting of extended, thin, coherent, locally low-dimensional sheets of topological charge embedded in 4d space, with opposite sign sheets interleaved, see original QCD lattice results [56,[63][64][65]. A similar structure has been also observed in QCD by a different group [57] and also in two dimensional CP N −1 model [66].…”
Section: B Insights From Numerical Lattice Simulations and Holographmentioning
confidence: 59%
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“…The recent Monte Carlo studies of pure glue gauge theory have revealed a laminar structure in the vacuum consisting of extended, thin, coherent, locally low-dimensional sheets of topological charge embedded in 4d space, with opposite sign sheets interleaved, see original QCD lattice results [56,[63][64][65]. A similar structure has been also observed in QCD by a different group [57] and also in two dimensional CP N −1 model [66].…”
Section: B Insights From Numerical Lattice Simulations and Holographmentioning
confidence: 59%
“…It is important to emphasize that the singular behaviour of the contact term ∼ δ 4 (x) is not an artifact of any approximations, in spite of the fact that this behaviour was established in simplified models: in the "deformed QCD" [46] and in the Veneziano model (19). This singular behaviour and the vanishing width (in continuum limit) of the contact term have been observed in the lattice simulations [56][57][58][59][60].…”
Section: B Insights From Numerical Lattice Simulations and Holographmentioning
confidence: 68%
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“…On the other hand the correlator Q(x)Q(0) is negative for x = 0 as shown in [54][55][56]. Also on the lattice this correlator is negative [57][58][59]. Then part of the contact divergences must add up to the total topological susceptibility in order to make it positive.…”
Section: Rlatticementioning
confidence: 99%