Chris Michael (auth.), Pierre van Baal (eds.)'s Confinement, Duality, and Non-Perturbative Aspects of QCD PDF

By Chris Michael (auth.), Pierre van Baal (eds.)

ISBN-10: 0306458268

ISBN-13: 9780306458262

ISBN-10: 030647056X

ISBN-13: 9780306470561

Hadronic Physics from the Lattice; C. Michael. Monte Carlo effects for the Hadron Spectrum; R. Kenway. Physics from the Lattice: Glueballs in QCD; Topology; SU(N) for all N; M. Teper. QCD on Coarse Lattices; G.P.Lepage. Finite dimension strategies and the robust Coupling consistent; P.Weisz. Continuum and Lattice Coulomb-Gauge Hamiltonian; D. Zwanziger. Gribov Ambiguities and the basic area; P. van Baal. excellent activities; P. Hasenfratz. Nonperturbative circulate Equations, Low-Energy QCD, and the Chiral part Transition; D.-U. Jungnickel, C. Wetterich. Light-Front QCD; A Constituent photo of Hadrons; R.J. Perry. Instantons in QCD and comparable Theories; E. Shuryak. common habit in Dirac Spectra; J. Verbaarschot. Duality and indirect Confinement; G.'t Hooft. Abelian Projections and Monopoles; M.N. Chernodub, M.I.Polikarpov. the twin Superconductor photograph for Confinement; A. DiGiacomo. twin Lattice Blockspin Transformation and ideal Monopole motion for SU(2) Gauge idea; T. Suzuki, et al. advent to inflexible Supersymmetric Theories; P.C. West. Non-Perturbatiev Gauge Dynamics in Supersymmetric Theories - A Primer; M. Shifman. levels of Supersymmetric Gauge Theories; A. Schwimmer. Index.

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B140 (1984) 392. 38. R. Allton et al. (APE Collaboration), Nucl. Phys. B431 (1994) 667. 39. W. , Fermilab preprint FERMILAB-PUB-97/121-T, hep-lat/9705008. K. INTRODUCTION In these lectures I will show, through three examples, how current lattice calcula- tions are able to tell us interesting things about the continuum physics of non-Abelian gauge theories. My first topic concerns the glueball spectrum. The physics question here is: where, in the experimentally determined hadron spectrum, are the glueballs hiding?

B478 (1996) 365. P. Weisz, these Proceedings. B. Sheikholeslami and R. Wohlert, Nucl. Phys. B259 (1985) 572. G. , Nucl. Phys. B352 (1991) 266. M. Bochicchio, L. Maiani, G. Martinelli, G. Rossi and M. Testa Nucl. Phys. B262 (1985) 331. P. B. Mackenzie, Phys. Rev. D48 (1993) 2250. D. Kenway (UKQCD Collaboration), Nucl. Phys. B (Proc. ) 53 (1997) 206. 25. A. Rowland, Nucl. Phys. B (Proc. Suppl,) 53 (1997) 308. 26. M. Lüscher et al. (Alpha Collaboration), DESY preprint 96-222, hep-lat/9611015. 27. M.

Baryon Masses Continuing this analysis for the baryons gives a similar picture of consistent continuum extrapolations for the two improvement schemes. This can be seen for the nucleon mass in Fig 10, although the continuum value appears to disagree with experiment (a bigger discrepancy is obtained if we use the scale from the string tension, rather than from ). The ratio of the mass to the nucleon mass, also shown in Fig 10, is only weakly dependent on lattice spacing (in both improvement schemes) and the continuum estimate is, in this case, in good agreement with experiment.

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Confinement, Duality, and Non-Perturbative Aspects of QCD by Chris Michael (auth.), Pierre van Baal (eds.)

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