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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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发表于 2025-3-21 19:43:49 | 显示全部楼层 |阅读模式
书目名称Chiral Quark Dynamics
编辑Reinhard Alkofer,Hugo Reinhardt
视频video
丛书名称Lecture Notes in Physics Monographs
图书封面Titlebook: Chiral Quark Dynamics;  Reinhard Alkofer,Hugo Reinhardt Book 1995 Springer-Verlag Berlin Heidelberg 1995 Baryon.Boson.Chirale Solitonen.Chi
描述These notes give an introduction to the description of hadrons, i.e., mesons and baryons, within a quark model based on a chirally invariant 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 describing successfully meson properties. It possesses solitonic solutions which are identified as baryons. Via functional integral techniques a Faddeev equation for baryons describing them as bound states of a diquark and a quark is derived. Finally, a unification of these two complementary pictures of baryons is proposed.
出版日期Book 1995
关键词Baryon; Boson; Chirale Solitonen; Chirale Symmetrie; Faddeec Equation; Fadeevgleichung; Mambu-Jona-Lasinio
版次1
doihttps://doi.org/10.1007/978-3-540-49454-6
isbn_softcover978-3-662-14020-8
isbn_ebook978-3-540-49454-6Series ISSN 0940-7677
issn_series 0940-7677
copyrightSpringer-Verlag Berlin Heidelberg 1995
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发表于 2025-3-21 21:59:29 | 显示全部楼层
The Effective Meson Theory,. Unfortunately, the effective meson theory of large . QCD cannot be constructed explicitly. The primary aim of the investigations using the NJL model was to understand the emergence of the effective meson theory [ER86] and in particular the appearance of baryons as solitons out of the quark flavor
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Lecture Notes in Physics Monographshttp://image.papertrans.cn/c/image/225955.jpg
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Quantities, laws and sign conventions elementary fermions of the theory, the quarks, live in the fundamental representation of the gauge group and carry therefore a quantum number called . which can take three different values, and which may be named . red, green and blue. The interaction between the quarks is mediated by the gauge bos
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Rotation and translation: simultaneity?model (3.1). We achieved this by using a covariant gradient expansion, the heat kernel method, and taking the limit of infinitely large vector and axialvector meson masses. We discussed already that the Skyrme model describes pions for small energies and amplitudes reasonably well. Allowing also lar
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Rotation and translation: simultaneity?term in eq. (2.55) has been taken into account. This was justified for large . which is the conceptual basis of the soliton picture. Now we will consider . = 3 and investigate the second term of the Lagrangian (2.55). We slightly generalize it by allowing different coupling constants . and . in the
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