Titlebook: Gauge Theory of Weak Interactions; Walter Greiner,Berndt Müller Textbook 20003rd edition Springer-Verlag Berlin Heidelberg 2000 Beta decay

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書(shū)目名稱Gauge Theory of Weak Interactions影響因子(影響力)




書(shū)目名稱Gauge Theory of Weak Interactions影響因子(影響力)學(xué)科排名




書(shū)目名稱Gauge Theory of Weak Interactions網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Gauge Theory of Weak Interactions網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Gauge Theory of Weak Interactions被引頻次




書(shū)目名稱Gauge Theory of Weak Interactions被引頻次學(xué)科排名




書(shū)目名稱Gauge Theory of Weak Interactions年度引用




書(shū)目名稱Gauge Theory of Weak Interactions年度引用學(xué)科排名




書(shū)目名稱Gauge Theory of Weak Interactions讀者反饋




書(shū)目名稱Gauge Theory of Weak Interactions讀者反饋學(xué)科排名

媒介

Cupping

synchronous

不成比例

The Neutral Kaon System,There are four strange pseudoscalar mesons K.,K.,K. and ., which are all eigenstates of the Hamiltonian of the strong interaction.

intention

https://doi.org/10.1007/978-3-658-11394-0, these are: the strong (nuclear) interaction, electromagnetism, the weak (nuclear) interaction, and gravity (see Table 1.1). The interaction strength varies with distance between the force centers. This is illustrated in the figure accompanying Table 1.1.

intention

鈍劍

https://doi.org/10.1007/978-3-322-88451-0ractions, and incorporating charged and neutral currents in a unified way. First we have to learn how to convert a theory involving massless vector bosons into a theory of massive particles, without disturbing the favourable high-energy behaviour of a massless propagator. We shall proceed by discuss

令人發(fā)膩

傾聽(tīng)

https://doi.org/10.1007/978-3-658-27933-2aryon number . = 0), which always have integer spin. The lightest hadrons, with equal spin (and equal parity), can be arranged in simple multiplets, where two further quantum numbers serve as order criteria: the .,and its third component .., and the .,or alternatively the so-called strong . = . + ..