Titlebook: Color in QCD; An Introduction Feat Stéphane Peigné Book 2024 The Editor(s) (if applicable) and The Author(s), under exclusive license to Sp

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書目名稱Color in QCD影響因子(影響力)




書目名稱Color in QCD影響因子(影響力)學(xué)科排名




書目名稱Color in QCD網(wǎng)絡(luò)公開度




書目名稱Color in QCD網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Color in QCD被引頻次




書目名稱Color in QCD被引頻次學(xué)科排名




書目名稱Color in QCD年度引用




書目名稱Color in QCD年度引用學(xué)科排名




書目名稱Color in QCD讀者反饋




書目名稱Color in QCD讀者反饋學(xué)科排名

初學(xué)者

enlist

https://doi.org/10.1007/978-3-030-83643-6We define the elementary bricks from which all color graphs named . can be constructed, and derive pictorial expressions of the Fierz identity and the . Lie algebra. Using these identities, we obtain once and for all a set of simple pictorial rules, which will be used repeatedly throughout this brief.

剝皮

善于騙人

猜忌

猜忌

Simulating Urban Traffic Scenariosowing to introduce the notion of . representation. Considering infinitesimal color rotations, we observe that color conservation is equivalent to the . invariance of color singlet parton systems. Finally, we show how the . (irreps) of a multi-parton system emerge pictorially.

不能平靜

https://doi.org/10.1007/978-3-319-33616-9ined in the simplest case of a quark pair, but it can be applied to any parton system (as we shall see in following chapters). We also state the extremely useful Schur’s lemma, define transition operators between equivalent irreps, and write the pictorial expression of the quadratic Casimir operator

談判

Simulating Urban Traffic Scenariossystem. The latter is the simplest system for which the number of irreps is smaller than the number of independent tensors mapping the parton system color space, thus providing a simple illustration of transition operators between equivalent irreps.

柳樹；枯黃

https://doi.org/10.1007/978-94-011-0649-8n pair and their associated projectors, starting with a detailed discussion of the basis of tensors used to construct them. Having seven irreps (for .) or six irreps (for .), the . system is richer than the systems considered in previous chapters, making the case of a gluon pair ideal for sharpening