Book contents
- Frontmatter
- Contents
- Foreword
- Preface
- 1 Classical mechanics
- 2 Quantum mechanics
- 3 Relativity, the Lorentz group, and Dirac's equation
- 4 Fiber bundles, connections, and representations
- 5 Classical field theory
- 6 Quantization of classical fields
- 7 Perturbative quantum field theory
- 8 Renormalization
- 9 The Standard Model
- Appendix A Hilbert spaces and operators
- Appendix B C* algebras and spectral theory
- Bibliography
- Index
2 - Quantum mechanics
Published online by Cambridge University Press: 05 March 2013
- Frontmatter
- Contents
- Foreword
- Preface
- 1 Classical mechanics
- 2 Quantum mechanics
- 3 Relativity, the Lorentz group, and Dirac's equation
- 4 Fiber bundles, connections, and representations
- 5 Classical field theory
- 6 Quantization of classical fields
- 7 Perturbative quantum field theory
- 8 Renormalization
- 9 The Standard Model
- Appendix A Hilbert spaces and operators
- Appendix B C* algebras and spectral theory
- Bibliography
- Index
Summary
In this chapter, we present the basic principles of the quantum mechanics of particle systems from a modern mathematical perspective. The proper study of quantum mechanics brings together several interesting mathematical ideas, ranging from group representations to the spectral theory of unbounded self-adjoint operators in Hilbert spaces and the theory of C* algebras. The facts from analysis of operators in Hilbert spaces and C* algebras needed in this chapter are presented in detail in the appendices at the end of the book. More on the mathematical foundations of quantum mechanics can be found in the books by L. Fadeev and O. Yakubovskii [FY], G. Mackey [M], and F. Strocchi [Str] listed in the bibliography.
The birth of quantum theory
The origins of quantum theory can be traced back to M. Planck's study, published in 1900, of so-called black-body radiation. It is well known that matter glows when heated, going from red-hot to white-hot as the temperature rises. The color (or frequency of radiation) of the radiating body is independent of its surface, and for a black body it is found to be a function of temperature alone. The behavior of the radiation energy as a function of temperature seemed quite different at high temperatures and low temperatures. In a desperate attempt to fit these different behaviors into a single law, Planck introduced the hypothesis that energy was not continuous, but came in discrete packets or quanta.
At the beginning of the twentieth century, a number of experiments pointed to a breakdown of the laws of classical mechanics at very small (subatomic) scales.
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- Mathematical Aspects of Quantum Field Theory , pp. 14 - 50Publisher: Cambridge University PressPrint publication year: 2010