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Titlebook: New Phenomena in Subnuclear Physics; Part A Antonino Zichichi Book 1977 Springer Science+Business Media New York 1977 energy.field theory.g

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樓主: Jurisdiction
31#
發(fā)表于 2025-3-27 00:48:44 | 只看該作者
32#
發(fā)表于 2025-3-27 01:16:27 | 只看該作者
33#
發(fā)表于 2025-3-27 07:34:20 | 只看該作者
Hadrodynamics with the Elusive Quarks Their number, as we are witnessing, is having an ominous tendency to increase under the effect of the exciting discoveries of new particles and unexpected lepton yields in e+e? and ν-nucleon collisions. However, I believe that after the experimental situation will more or less settle the usefulness
34#
發(fā)表于 2025-3-27 13:28:56 | 只看該作者
The M.I.T. Bag 1975the fundamental ideas and of the recent developments. My interpretation may or may not be accepted by the authors and developers of this theory : A. Chodos, T. DeGrand, R.L. Jaffe, K. Johnson, J. Kiskis and C. Thorn, naturally all of M.I.T.*.. I have not contributed much except what could be referre
35#
發(fā)表于 2025-3-27 16:36:43 | 只看該作者
36#
發(fā)表于 2025-3-27 19:38:32 | 只看該作者
Weak Non Leptonic Amplitudes in Unified Gauge Theoriesns. Much attention has been devoted to this problem in the last year, since it was realized that in asymtotically free theories of strong interactions the observed ΔT=1/2 (or octet enhancement) rule for strange particle decays, can be possibly explained.. Similar enhancement rules can also be derive
37#
發(fā)表于 2025-3-27 22:30:33 | 只看該作者
Relationship Between Gauge Field Theories and Dual Resonance Modelsime more and more linkages between the two theories are discovered and it seems inevitable that a fuller understanding of this relationship will play a central role in future developments, especially of strong interaction theory. I have been unable to find any systematic discussion of the relationsh
38#
發(fā)表于 2025-3-28 02:49:36 | 只看該作者
39#
發(fā)表于 2025-3-28 07:15:52 | 只看該作者
40#
發(fā)表于 2025-3-28 14:04:04 | 只看該作者
Gauge Theory for Strong InteractionsThere are good indications that the strong interactions can be described by a non-Abelian gauge theory based on the “color” gauge group SU(3). There are only gauge vector bosons and quarks in this theory, but no scalar fields, hence we have no symmetry breaking through a Higgs mechanism.
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