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Titlebook: Chiral Quark Dynamics; Reinhard Alkofer,Hugo Reinhardt Book 1995 Springer-Verlag Berlin Heidelberg 1995 Baryon.Boson.Chirale Solitonen.Chi

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Constants and functional reductionl. Here we have put more emphasis on the description of baryons than on the one of mesons. Surprisingly, there are two possibilities to build baryons. One, which is the only one in the limit of a large number of colors, is based on the picture of baryons as chiral solitons. A special feature of this
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Constants and functional reductionave been restricted to the case that meson fields are frozen to its vacuum expectation value. A complete investigation of Quantum Flavor Dynamics would require the explicit baryon field as introduced in Sect. 5.1 as well as the non-perturbative (solitonic) meson fields, especially the hedgehog (4.3) for the pseudoscalar field.
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0940-7677 quantum field theory. Emphasis is put on a didactic approach intended for graduate students with some background on functional integral techniques. Starting from QCD a motivation of a specific form of the effective quark interaction is given. Functional integral bosonization leads to a theory descr
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Rotation and translation: simultaneity?alvector meson masses. We discussed already that the Skyrme model describes pions for small energies and amplitudes reasonably well. Allowing also large amplitudes one realizes that this model possesses special localized solutions: topological solitons. These are then interpreted as baryons.
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Baryons as Chiral Solitons,alvector meson masses. We discussed already that the Skyrme model describes pions for small energies and amplitudes reasonably well. Allowing also large amplitudes one realizes that this model possesses special localized solutions: topological solitons. These are then interpreted as baryons.
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