Book contents
- Frontmatter
- Contents
- Preface to the third edition
- Preface to the first and second editions
- Acknowledgements
- 1 Accelerators, beams and detectors
- 2 Pions and Muons
- 3 Conservation laws
- 4 Strong, weak and electromagnetic interactions
- 5 Strange particles
- 6 Spin and parity of the K-mesons and non-conservation of parity in weak interactions
- 7 Weak interactions: basic ideas
- 8 Invariance under the CP and T operations, properties of K0-mesons
- 9 Strongly-decaying resonances
- 10 SU(3) and the quark model: classification and dynamic probes
- 11 Weak interactions and weak–electromagnetic unification
- 12 New flavours
- 13 Quark and gluon interactions
- 14 Higher symmetries
- 15 Particle physics and cosmology
- 16 Epilogue
- Appendix A Relativistic kinematics and phase space
- Appendix B Clebsch–Gordan coefficients and particle properties
- References
- Index
4 - Strong, weak and electromagnetic interactions
Published online by Cambridge University Press: 05 June 2012
- Frontmatter
- Contents
- Preface to the third edition
- Preface to the first and second editions
- Acknowledgements
- 1 Accelerators, beams and detectors
- 2 Pions and Muons
- 3 Conservation laws
- 4 Strong, weak and electromagnetic interactions
- 5 Strange particles
- 6 Spin and parity of the K-mesons and non-conservation of parity in weak interactions
- 7 Weak interactions: basic ideas
- 8 Invariance under the CP and T operations, properties of K0-mesons
- 9 Strongly-decaying resonances
- 10 SU(3) and the quark model: classification and dynamic probes
- 11 Weak interactions and weak–electromagnetic unification
- 12 New flavours
- 13 Quark and gluon interactions
- 14 Higher symmetries
- 15 Particle physics and cosmology
- 16 Epilogue
- Appendix A Relativistic kinematics and phase space
- Appendix B Clebsch–Gordan coefficients and particle properties
- References
- Index
Summary
Types of interactions
In chapter 2 we have seen that the nuclear interaction is very much stronger than the electromagnetic interaction; their relative strengths are characterised by the difference in the ‘coupling constants’ which are discussed in more detail below. We may recognise at this stage two other forms of interaction, gravitational forces and the so-called ‘weak’ interaction. One of the most notable milestones of recent years has been the unification of the weak and electromagnetic interactions as different aspects of the same underlying force, in the theory of Glashow, Weinberg and Salam, and the discovery of the W and Z particles, the additional quanta of the unified interaction, with the properties predicted. This topic is treated in more detail in chapter 11.
We may summarise as follows:
Strong interactions are responsible for the interactions between nucleons, nucleons and mesons and a number of other particles. The mesons act as the quanta of the strong interaction on the nuclear scale. These interactions reflect the interaction between quarks due to the exchange of gluons on the sub-nucleon level.
Electromagnetic interactions are responsible for the force between electrically-charged particles and are mediated by the exchange of photons.
Weak interactions are responsible for many particle decays such as radioactive decay (the basic process n → p + e- + vg), pion and muon decay and a number of other decay processes.
Gravitational interactions exist between all particles having mass and are believed to be mediated by the so far undetected gravitons.
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- Information
- Elementary Particles , pp. 105 - 110Publisher: Cambridge University PressPrint publication year: 1991