Titlebook: Workshop on Non-Perturbative Quantum Chromodynamics; Kimball A. Milton,Mark A. Samuel Book 1983 Birkh?user Boston, Inc. 1983 Lattice gauge

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Topological Charge in Lattice Gauce Theory,ed that lattice regularization changes the semicalssical structure of the theories considerably. The reason is that states of the continuum theory with different topological charge are connected by singular gauge transformations [3]. With finite lattice spacing there are no singularities. Consequent

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Locally Gauge-Invariant Formulation of Parastatistics,ermi combinations of para-Fermi quarks are in one-to-one correspondence with the color singlets of the formulation with explicit color [11]. Thus the counting of states, and the explanation of the apparent conflict with the spin-statistics theorem with quarks in the symmetric representation of SU(6)

彎彎曲曲

Affine Algebras and Strong Interaction Theories,explicit representation in terms of the dual string is reviewed here in simple language. A nonlocal nonlinear realization of a subalgebra of the affine algebras on the self-dual class of solutions of the Yang Mills theory is also reviewed. It is remarked that this structure occurs naturally in a Kal

煩人

Gluon Condensation in QCD and Supersymmetric QCD,at it is becoming increasingly more critical for the deep understanding of physical laws of nature. It is probably not an exaggeration to say that it is an emblem of the particle physics of the 80’s. This I believe is an inevitable trend. The development of non-abelian gauge theories In the 70’s has

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Scalars and Pseudoscalars in Non-linear Chiral Dynamics Based on QCD, usual PCAC and U (1) anomaly constraints and the new (for non-linear lagrangians) SU(3) breaking effects due to the scalar field vacuum expectation values. F./F. ≠ 1 follows naturally in our approach, for example.

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