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Titlebook: Current Topics in Elementary Particle Physics; K. H. Mütter,K. Schilling Book 1981 Springer Science+Business Media New York 1981 Confineme

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31#
發(fā)表于 2025-3-26 23:14:06 | 只看該作者
Weak Decays and the Bound State Structure of Hadrons, the electroweak interactions. However at the same time it became clear that many of the unsolved problems in the physics of elementary particles will not find their solution within this theory. For example, it was thought years ago that within a well-defined theory of the electroweak interactions o
32#
發(fā)表于 2025-3-27 04:31:04 | 只看該作者
33#
發(fā)表于 2025-3-27 07:24:12 | 只看該作者
34#
發(fā)表于 2025-3-27 13:30:01 | 只看該作者
Muon-Nucleon Scattering, QCD Related Experimental Results,re of nucleons. With improved accuracy of the measurements and an increased scale of Q. in the scattering experiments violation of scaling was found giving an important basis for the new strong interaction theory, the Quantum Chromo Dynamics. It seems now that charged lepton nucleon scattering is en
35#
發(fā)表于 2025-3-27 15:01:44 | 只看該作者
36#
發(fā)表于 2025-3-27 18:34:10 | 只看該作者
Classical Solutions in Field Theory,would be impossible to review all the work that has been done and the intention here instead is to discuss a small, but to my mind significant, area of development taking place in Euclidean field theories. Other solutions, corresponding to Yang-Mills solitons or monopoles, will be discussed by David
37#
發(fā)表于 2025-3-28 01:24:13 | 只看該作者
38#
發(fā)表于 2025-3-28 02:56:01 | 只看該作者
Monte Carlo Computations for Lattice Gauge Theories with Finite Gauge Groups,such as strong coupling expansions, which cannot be applied to the continuum theory.. After a Wick rotation of time to imaginary time, the weighted sum over all configurations used to define quantum expectation values becomes formally identical to a statistical sum for a four-dimensional system. Thi
39#
發(fā)表于 2025-3-28 06:39:56 | 只看該作者
Chiral Dynamics for Colour and Technicolour QCD Like Theories at Large N,is a SU(3) gauge field theory describing the interaction between quarks and gluons which are assumed to be the constituents of the hadrons. Its Lagrangian can be written as follows:.where M is the mass matrix of the quarks.
40#
發(fā)表于 2025-3-28 12:24:51 | 只看該作者
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