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Chapter 1<br />
Introduction<br />
<strong>Nuclear</strong> physics is the study of atomic nuclei. The primary aim of nuclear physics<br />
is to underst<strong>and</strong> the force between nucleons, the structure of nuclei, <strong>and</strong> how nuclei<br />
<strong>in</strong>teract with each other <strong>and</strong> with other subatomic particles. These three questions<br />
are, to a large extent, related to each other. It has been known for years that the<br />
nucleus is a many-body system of protons <strong>and</strong> neutrons, the two lightest members<br />
of the baryon family, that is held together by the strong nuclear force. Traditional<br />
models of nuclei rely on the shell model, where it is assumed that both protons <strong>and</strong><br />
neutrons are mov<strong>in</strong>g <strong>in</strong>dependently <strong>in</strong> an average mean-field potential, which expresses<br />
the <strong>in</strong>teraction of the nucleon with the surround<strong>in</strong>g medium. The nucleons<br />
then occupy the lowest s<strong>in</strong>gle-particle levels up to the Fermi energy, whereas the<br />
s<strong>in</strong>gle-particle levels above the Fermi energy rema<strong>in</strong> unoccupied. From systematic<br />
<strong>in</strong>vestigations for a large number of target nuclei a richness of precise <strong>in</strong>formation<br />
about the <strong>in</strong>dependent-particle wave functions <strong>and</strong> spectroscopic strengths was assembled<br />
[1], <strong>and</strong> it turned out that many nuclear features could be expla<strong>in</strong>ed with<strong>in</strong><br />
this s<strong>in</strong>gle-particle picture.<br />
However, as nucleons <strong>in</strong> the nucleus <strong>in</strong>teract with each other through the strong,<br />
short-ranged <strong>in</strong>teraction, a number of nuclear structure properties rema<strong>in</strong>s unexpla<strong>in</strong>ed<br />
<strong>in</strong> the basic <strong>in</strong>dependent-particle model. An extensive amount of measurements<br />
has made it clear that the occupancy of the s<strong>in</strong>gle-particle level is substantially<br />
smaller than what is expected <strong>in</strong> a naive <strong>in</strong>dependent-particle model. This observation<br />
has resulted <strong>in</strong> the conjecture that 2/3’s of the nucleons <strong>in</strong> the nucleus act as<br />
<strong>in</strong>dependent quasi-particles, whereas the rema<strong>in</strong><strong>in</strong>g ones are then correlated [1].<br />
A full underst<strong>and</strong><strong>in</strong>g of the nucleus can not be achieved without some knowledge<br />
about the underly<strong>in</strong>g mechanisms that are responsible for the strong nuclear force.<br />
The strong nuclear force manifests itself as a result of the strongly <strong>in</strong>teract<strong>in</strong>g quark<br />
<strong>and</strong> gluon constituents which build up the nucleon. A better underst<strong>and</strong><strong>in</strong>g of<br />
the quantum chromodynamics (QCD) theory which describes the strong <strong>in</strong>teraction<br />
between quarks <strong>and</strong> gluons, will most certa<strong>in</strong>ly lead to a better underst<strong>and</strong><strong>in</strong>g of<br />
1