Book contents
- Frontmatter
- Contents
- List of figures
- List of tables
- List of definitions, principles, etc.
- List of boxes
- List of symbols
- List of abbreviations
- Introduction
- Part I Basic features of quantum mechanics
- 1 From classical mechanics to quantum mechanics
- 2 Quantum observables and states
- 3 Quantum dynamics
- 4 Examples of quantum dynamics
- 5 Density matrix
- Part II More advanced topics
- Part III Matter and light
- Part IV Quantum information: state and correlations
- Bibliography
- Author index
- Subject index
2 - Quantum observables and states
Published online by Cambridge University Press: 05 June 2012
- Frontmatter
- Contents
- List of figures
- List of tables
- List of definitions, principles, etc.
- List of boxes
- List of symbols
- List of abbreviations
- Introduction
- Part I Basic features of quantum mechanics
- 1 From classical mechanics to quantum mechanics
- 2 Quantum observables and states
- 3 Quantum dynamics
- 4 Examples of quantum dynamics
- 5 Density matrix
- Part II More advanced topics
- Part III Matter and light
- Part IV Quantum information: state and correlations
- Bibliography
- Author index
- Subject index
Summary
In this chapter we shall mainly present the basic formalism that was initially developed by Heisenberg, also known as matrix mechanics (see Subsec. 1.5.7). We will first introduce in Sec. 2.1 the concept of quantum observables. Then, the problem of discrete and continuous spectra will be discussed and the basic non-commutability of quantum-mechanical observables will be deduced. While in Sec. 2.1 we discuss observables on a general formal level, in Sec. 2.2 some basic quantum-mechanical observables will be defined, and then different representations discussed and commutation relations derived. In Sec. 2.3 a basic uncertainty relation is derived. In the same section the relationship between uncertainty, superposition, and complementarity will be discussed. Finally, in Sec. 2.4 complete subsets of commuting observables will be shown to be Boolean subalgebras pertaining to a quantum algebra which is not Boolean.
BASIC FEATURES OF QUANTUM OBSERVABLES
This section is devoted to a general and formal exposition of quantum observables. In Subsec. 2.1.1 we shall learn how one can mathematically represent quantum observables as Hermitian operators. In Subsec. 2.1.2 we shall see how to change a basis, while in Subsec. 2.1.3 we shall find the relationship between eigenvalues of the observables and probabilities and learn how to calculate mean values. In Subsec. 2.1.4 we shall deal with an operator diagonalization. Finally, in Subsec. 2.1.5, the basic non-commutability of quantum observables will be presented by means of an example.
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- Quantum Mechanics , pp. 43 - 99Publisher: Cambridge University PressPrint publication year: 2009