Proceedings of the Workshop on Non-Perturbative Methods, Montpellier, 9-13 July 1985S. Narison |
From inside the book
Results 1-3 of 63
Page 69
... parameters cs , sino . The quantity 23 ( 1/2 ) Im n 98 □ HS2C2S3 Sing ( 2.21 ) Re g ( 1/2 ) defines the so called H - parameter , which governs the ratio ε ' / ε of CP - violation parameters . We have made a prediction of the H - parameter ...
... parameters cs , sino . The quantity 23 ( 1/2 ) Im n 98 □ HS2C2S3 Sing ( 2.21 ) Re g ( 1/2 ) defines the so called H - parameter , which governs the ratio ε ' / ε of CP - violation parameters . We have made a prediction of the H - parameter ...
Page 89
... parameters of vector mesons ( my and fv ) play an im- portant role . By contrast , the corresponding pseudoscalar parameters , mp and fp , with Р = π or K , do not appear and effects of selecting π + , K + or K ° simply reduce to change ...
... parameters of vector mesons ( my and fv ) play an im- portant role . By contrast , the corresponding pseudoscalar parameters , mp and fp , with Р = π or K , do not appear and effects of selecting π + , K + or K ° simply reduce to change ...
Page 124
... parameters that are needed and the values obtained . As we said above the value of g , is not important in this calculation . The u and d quarks are massless . The strange quark mass is required to be very low : m , ( 1Gev . ) = 100Mev ...
... parameters that are needed and the values obtained . As we said above the value of g , is not important in this calculation . The u and d quarks are massless . The strange quark mass is required to be very low : m , ( 1Gev . ) = 100Mev ...
Contents
OPENING TALK | 1 |
SVZ Gluon Condensate and Potential | 20 |
Sum Rules for Baryons | 41 |
Copyright | |
14 other sections not shown
Common terms and phrases
algebra analysis anomaly approximation asymptotic asymptotic freedom background field baryons behaviour Bertlmann Borel bosons calculations CHIRAL ANOMALIES chiral symmetry coefficients cohomology computed continuum contribution corrections corresponding coupling constant decay deconfinement defined determined diagram dimension dimensional discuss effective energy equation experimental factor fermions field theory finite flavour gauge theories GeV/c Gevē glueball gluon condensate hadronic higher order instanton integral interaction invariant Ioffe Lagrangian lattice Lett Lie G limit mesons method Montpellier Narison non-perturbative Nucl obtained operator parameters perturbation theory phenomenological Phys physical polynomial potential prediction preprint pseudoscalar QCD sum rules quantum numbers quark mass radiative Rafael ratio region renormalization renormalons Shifman spectral function strange quark supersymmetric theoretical topological torons transformations transition two-point function Univ vacuum Vainshtein vector Ward identity Wess Wilson loop Zakharov zero modes Zumino