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

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書(shū)目名稱Chiral Quark Dynamics影響因子(影響力)




書(shū)目名稱Chiral Quark Dynamics影響因子(影響力)學(xué)科排名




書(shū)目名稱Chiral Quark Dynamics網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Chiral Quark Dynamics網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Chiral Quark Dynamics被引頻次




書(shū)目名稱Chiral Quark Dynamics被引頻次學(xué)科排名




書(shū)目名稱Chiral Quark Dynamics年度引用




書(shū)目名稱Chiral Quark Dynamics年度引用學(xué)科排名




書(shū)目名稱Chiral Quark Dynamics讀者反饋




書(shū)目名稱Chiral Quark Dynamics讀者反饋學(xué)科排名

CALL

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

牢騷

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壓倒性勝利

Lecture Notes in Physics Monographshttp://image.papertrans.cn/c/image/225955.jpg

過(guò)時(shí)

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

過(guò)時(shí)

浮雕寶石

記憶

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

Banister

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