Abstract
In our attempt to understand the strong interactions between hadrons, we have inferred a complicated substructure within the particles that we actually observe in our laboratories. Over the years, the understanding of this physics evolved into a constituent model of hadrons. We have not yet been able to detect the constituents by themselves, but most of the observed phenomena involving hadrons can be explained by their presence. The constituents I am referring to are, of course, quarks. The quark model has had particles added to it whose properties would determine how quarks interact with each other. These exchanged particles are called gluons. These ideas (and more) have now been formalized into the theory called Quantum Chromodynamics (QCD).
Work supported by the Department of Energy under contract number DE-AC03-76SF00515.
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Atwood, W.B. (1982). Lepton Nucleon Scattering. In: Lectures on Lepton Nucleon Scattering and Quantum Chromodynamics. Progress in Physics, vol 4. Birkhäuser, Boston, MA. https://doi.org/10.1007/978-1-4899-6691-9_1
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DOI: https://doi.org/10.1007/978-1-4899-6691-9_1
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