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Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/10868
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dc.contributor.authorLeinweber, D.-
dc.contributor.authorParrinello, C.-
dc.contributor.authorSkullerud, J.I.-
dc.contributor.authorWilliams, A.-
dc.date.issued1999-
dc.identifier.citationNuclear Physics B - Proceedings Supplements, 1999; 73(1-3):626-628-
dc.identifier.issn0920-5632-
dc.identifier.urihttp://hdl.handle.net/2440/10868-
dc.descriptionCopyright © 1989. Submitted to Cornell University’s online archive www.arXiv.org in 1989 by Jon Ivar Skullerud. Post-print sourced from www.arxiv.org.-
dc.description.abstractThe gluon propagator has been calculated for quenched QCD in the Landau gauge at beta=6.0 for volumes 16^3x48 and 32^3x64, and at beta=6.2 for volume 24^3x48$. The large volume and different lattice spacings allow us to identify and minimise finite volume and finite lattice spacing artefacts. We also study the tensor structure of the gluon propagator, confirming that it obeys the lattice Landau gauge condition.-
dc.language.isoen-
dc.publisherELSEVIER SCIENCE BV-
dc.source.urihttp://arxiv.org/abs/hep-lat/9809030-
dc.titleThe structure of the gluon propagator-
dc.typeJournal article-
dc.identifier.doi10.1016/S0920-5632(99)85156-1-
pubs.publication-statusPublished-
dc.identifier.orcidLeinweber, D. [0000-0002-4745-6027]-
dc.identifier.orcidWilliams, A. [0000-0002-1472-1592]-
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Special Research Centre for the Subatomic Structure of Matter publications

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