Book contents
- Frontmatter
- Contents
- Editor's Statement
- Section Editor's Foreword
- Preface
- Acknowledgments
- PART I
- Chapter 1 Introduction
- Chapter 2 The Kinematics of Rotations
- Chapter 3 Standard Treatment of Angular Momentum in Quantum Mechanics
- Chapter 4 The Theory of Turns Adapted from Hamilton
- Chapter 5 The Boson Calculus Applied to the Theory of Turns
- Chapter 6 Orbital Angular Momentum and Angular Functions on the Sphere
- PART II
- Appendix of Tables
- Bibliography of Tables
- List of Symbols
- Author Index
- Subject Index
Chapter 4 - The Theory of Turns Adapted from Hamilton
Published online by Cambridge University Press: 04 August 2010
- Frontmatter
- Contents
- Editor's Statement
- Section Editor's Foreword
- Preface
- Acknowledgments
- PART I
- Chapter 1 Introduction
- Chapter 2 The Kinematics of Rotations
- Chapter 3 Standard Treatment of Angular Momentum in Quantum Mechanics
- Chapter 4 The Theory of Turns Adapted from Hamilton
- Chapter 5 The Boson Calculus Applied to the Theory of Turns
- Chapter 6 Orbital Angular Momentum and Angular Functions on the Sphere
- PART II
- Appendix of Tables
- Bibliography of Tables
- List of Symbols
- Author Index
- Subject Index
Summary
An Alternative Approach to Rotations
In the preceding chapters, we have discussed the standard view of the quantum theory of angular momentum. The present chapter is concerned with developing a new view of the subject starting from the beginning with a fresh look at rotations based on a viewpoint adapted primarily from Hamilton [1], but also partly from Klein and Sommerfeld [2] and from Wigner [3] (see Note 1). This new survey will be rewarded by the concept of a novel geometric entity – the turn – which in its quantal version (Chapter 5) will be realized by an elementary operator structure. In discussing this alternative viewpoint, we are primarily interested in motivation and in suggesting concepts. Accordingly, we shall proceed, at first, intuitively.
When reduced to fundamentals, the concept of an elementary (point) particle in physics (as discussed in Chapter 1) becomes synonymous with the fundamental symmetries assumed to characterize physical space. We have seen that, from the homogeneity and isotropy assumed for space, one induces the symmetries of spatial displacements (translations) and rotations; that is, one assumes that space is Euclidean and three-dimensional, having the isometry group, E(3), of rotations and translations.
It is quite easy to characterize translations, since three-dimensional translations necessarily (Artin [4]) form an abelian (commutative) group. For physics, the translation generator is the (Hermitian) momentum operator p, and the associated operator generating finite displacements is realized by U(a) = exp(–ia · p/ħ). This operator displaces the system by the (numerical) vector a.
- Type
- Chapter
- Information
- Angular Momentum in Quantum PhysicsTheory and Application, pp. 180 - 204Publisher: Cambridge University PressPrint publication year: 1984