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Semi-Leptonic Interactions of Hadrons

  • Walter Greiner
  • Berndt Müller

Abstract

All strongly interacting particles are called hadrons. One distinguishes baryons (baryon number B = ±1), which are fermions and carry spin ½, 3/2,..., and mesons (baryon number B = 0), which always have integer spin. The lightest hadrons, with equal spin (and equal parity), can be arranged in simple multiplets, where two further quantum numbers serve as order criteria: the isospin I, and its third component I 3, and the strangeness S, or alternatively the so-called strong hypercharge Y = B + S. These quantum numbers are characterized by the fact that they are exactly conserved under strong interactions. Conservation of strangeness is broken by weak interactions, which leads to decays of, for example, the Λ particle. The most important multiplets1 are depicted in Figs. 6.1-4.

Keywords

Weak Interaction Neutrino Oscillation Baryon Number Neutral Current Parity Violation 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Notes

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Copyright information

© Springer-Verlag Berlin Heidelberg 1996

Authors and Affiliations

  • Walter Greiner
    • 1
    • 2
  • Berndt Müller
    • 3
  1. 1.Institut für Theoretische PhysikJohann Wolfgang Goethe-Universität FrankfurtFrankfurt am MainGermany
  2. 2.Frankfurt am MainGermany
  3. 3.Physics DepartmentDuke UniversityDurhamUSA

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