Titlebook: Quantum Chromodynamics; Walter Greiner,Stefan Schramm,Eckart Stein Textbook 20022nd edition Springer-Verlag Berlin Heidelberg 2002 QCD.gau

連結(jié)

書(shū)目名稱(chēng)Quantum Chromodynamics影響因子(影響力)




書(shū)目名稱(chēng)Quantum Chromodynamics影響因子(影響力)學(xué)科排名




書(shū)目名稱(chēng)Quantum Chromodynamics網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱(chēng)Quantum Chromodynamics網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱(chēng)Quantum Chromodynamics被引頻次




書(shū)目名稱(chēng)Quantum Chromodynamics被引頻次學(xué)科排名




書(shū)目名稱(chēng)Quantum Chromodynamics年度引用




書(shū)目名稱(chēng)Quantum Chromodynamics年度引用學(xué)科排名




書(shū)目名稱(chēng)Quantum Chromodynamics讀者反饋




書(shū)目名稱(chēng)Quantum Chromodynamics讀者反饋學(xué)科排名

stressors

Scattering Reactions and the Internal Structure of Baryons,en quarks cannot be easily deduced from the energies of the states, since different models yield nearly identical and well-fitting descriptions of the mass spectrum. Such models include the flavor SU(6) model, the MIT bag model, the Skyrmion bag model, and potential models with nonrelativistic quark

engender

Gauge Theories and Quantum-Chromodynamics, many experimental facts supporting this model, as we shall discuss later in more detail. It seems by now also to be proven that QCD (quantum chromodynamics) is able to correctly describe the most pronounced feature of quark—quark interactions, i.e., confinement, and that it will generate, for examp

Corroborate

Perturbative QCD I: Deep Inelastic Scattering,e treated perturbatively in the case of large momentum transfers. For practical purposes, however, it is indispensable to know at what momentum values the transition between perturbative and non-perturbative effects takes place. To this end we again take a look at Fig. 1.1. The quark confinement pro

intoxicate

Perturbative QCD II: The Drell-Yan Process and Small-, Physics,e experiments only information about nucleon structure functions can be extracted, while little is learned about the inner structure of pions, for example. There are, however, different options for high-energy collisions. Electrons can be made to collide with positrons (as is done at Stanford, DESY,

isotope

Phenomenological Models for Nonperturbative QCD Problems,reticants have tried to develop simple physical models for these problems. Using suitable assumptions and parameter choices, one then attempts to reproduce as many properties of QCD as possible. We shall consider two such problems here: the ground state of QCD and the quark—gluon plasma. In both cas

employor

Scattering Reactions and the Internal Structure of Baryons, mass spectrum. Such models include the flavor SU(6) model, the MIT bag model, the Skyrmion bag model, and potential models with nonrelativistic quarks. Luckily lattice calculations are now good enough to demonstrate that the . model, namely QCD, gives equally good results.

面包屑

Perturbative QCD I: Deep Inelastic Scattering, the transition between perturbative and non-perturbative effects takes place. To this end we again take a look at Fig. 1.1. The quark confinement problem will be considered later together with different models for its solution.

骯臟

Phenomenological Models for Nonperturbative QCD Problems,oduce as many properties of QCD as possible. We shall consider two such problems here: the ground state of QCD and the quark—gluon plasma. In both cases we shall restrict ourselves to a few remarks only.

legacy