Handbook of Nuclear Chemistry: Basics of Nuclear Science, Volume 1

Chapter 2: Basic Properties of the Atomic Nucleus

T.F nyes

Institute of Nuclear Research of the Hungarian Academy of Sciences, Debrecen, Hungary

SUMMARY

In this chapter four topics are treated. 1. Fundamental constituents and interactions of matter, nuclear forces. 2. Properties of nuclei. 3. Single particle and collective motion, nuclear models. 4. Nuclear transitions, ?, ?, and ? decay.

1. NUCLEONS AND NUCLEAR FORCES

1.1 Fundamental constituents and interactions of matter

According to our present knowledge, the fundamental constituents of matter are quarks and leptons. Both quarks and leptons are pointlike and structureless on a scale of 10 ?17 m. These particles may interact with each other via four apparently different fundamental interactions: strong, weak, electromagnetic, and gravitational interactions. Any interaction is mediated by the exchange of specific interaction quanta. Some of the most important properties of quarks and leptons are summarized in TABLE 1. The table contains also the properties of quanta of electromagnetic, weak, and strong interactions [1]. The characteristic scale for gluons is <0.1 fm (i.e., <10 ? 16 m).

Table 1: Properties of fundamental constituents of matter: quarks [*], leptons, and field quanta (gauge bosons). R, G, B and R, G, B denote red, green, blue colors and antired, antigreen, antiblue complementary colors, respectively. Electron neutrinos have very small (<3 eV) or zero rest energy. Neutrinos are longitudinally spin polarized. If Z denotes the direction of velocity, for neutrinos S Z= ?1/2 (left-handed), for antineutrinos S z=+1/2 (right-handed).

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