Titlebook: Lectures on Nuclear Theory; C. Landau,Ya. Smorodinsky Book 1958 Springer Science+Business Media New York 1958 electrical engineering.elect

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,Interaction of π-Mesons with Nucleons,on of these particles with nucleons. It turns out that the situation here is fundamentally different from that which obtains in electrodynamics. In particular, in contrast with the interaction of an electron with the electromagnetic field, the interaction of mesons with nucleons is “strong” rather than “Weak.”

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Nuclear Forces,With the discovery of the neutron it became clear that the structural units of which the atomic nucleus is composed are two kinds of particles: protons and neutrons, usually called nucleons.

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Nuclear Structure (Independent Particle Model),ity, must have limited application. We should not be surprised if different effects require different models for their descriptiqn; sometimes these models may even have mutually exclusive properties (for example, the independent particle model and the optical model).

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Structure of the Nucleus (Heavy Nuclei),portant role is played by Coulomb forces, this assumption is no longer valid. Whereas in the light nuclei the important role is played by the total number of nucleons in a shell, the properties of heavy nuclei depend on the number of neutrons N and on the number of protons Z individually.