In the second part of this book we are going to consider hadronic bound-states. We will at first discuss the properties of mesons and baryons. The simplest example are heavy quark-antiquark (\(\mathrm{c\overline{c}}\) and \(\mathrm{b\overline{b}}\)) pairs, which are known as quarkonia. Due to the large quark masses they may be approximately treated in a nonrelativistic manner. The hydrogen atom and positronium will serve as electromagnetic analogues. The relative positions of the quarkonia’s energy levels are used to determine the potential and the coupling constant of the strong interaction.
Analogy is perhaps the physicist’s most powerful conceptual
tool for understanding new phenomena or opening new areas of
investigation. Early in this century, for example, Ernest
Rutherford and Niels Bohr conceived the atom as a miniature
solar system in which electrons circle the nucleus as planets
circle the Sun.
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NotesBy this we mean the average separation between the quark and the antiquark (see Fig. 14.2).
The standard nomenclature for mesons containing heavy quarks is such that the neutral meson with a b-quark is called a \(\mathrm{\overline{B}}^{0}\) and the meson with a \(\mathrm{\overline{b}}\) is known as a B0. An electrically neutral \(\mathrm{q\overline{q'}}\) state is marked with a bar, if the heavier quark/antiquark is negatively charged [8].
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Max-Planck-Institut für Kernphysik, Heidelberg, Germany
Bogdan Povh & Werner Rodejohann
Department Physik, Universität Erlangen-Nürnberg, Erlangen, Germany
Klaus Rith
SAP AG, Walldorf, Germany
Christoph Scholz
DFS Deutsche Flugsicherung GmbH, Langen, Germany
Frank Zetsche
© 2015 Springer-Verlag Berlin Heidelberg
About this chapter Cite this chapterPovh, B., Rith, K., Scholz, C., Zetsche, F., Rodejohann, W. (2015). Quarkonia. In: Particles and Nuclei. Graduate Texts in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-46321-5_14
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