Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Historical milestones
- 3 Basics of the classical description of light
- 4 Quantum mechanical understanding of light
- 5 Light detectors
- 6 Spontaneous emission
- 7 Interference
- 8 Photon statistics
- 9 Squeezed light
- 10 Measuring distribution functions
- 11 Optical Einstein–Podolsky–Rosen experiments
- 12 Quantum cryptography
- 13 Quantum teleportation
- 14 Summarizing what we know about the photon
- 15 Appendix. Mathematical description
- References
- Index
14 - Summarizing what we know about the photon
Published online by Cambridge University Press: 25 January 2010
- Frontmatter
- Contents
- Preface
- 1 Introduction
- 2 Historical milestones
- 3 Basics of the classical description of light
- 4 Quantum mechanical understanding of light
- 5 Light detectors
- 6 Spontaneous emission
- 7 Interference
- 8 Photon statistics
- 9 Squeezed light
- 10 Measuring distribution functions
- 11 Optical Einstein–Podolsky–Rosen experiments
- 12 Quantum cryptography
- 13 Quantum teleportation
- 14 Summarizing what we know about the photon
- 15 Appendix. Mathematical description
- References
- Index
Summary
How can we construct a picture of the photon from the wealth of observation material available to us? The photon appears to have a split personality: it is neither a wave nor a particle but something else which, depending on the experimental situation, exhibits a wave- or a particle-like behavior. In other words, in the photon (as in material particles such as the electron) the particle–wave dualism becomes manifest. Whereas classically the wave and the particle pictures are separate, quantum mechanics accomplishes a formal synthesis through a unified mathematical treatment.
Let us look first at the wave aspect familiar from classical electrodynamics, which seems to be the most natural description. It makes all the different interference phenomena understandable, such as the “interference of the photon with itself” on the one hand and the appearance of spatial and temporal intensity correlations in a thermal radiation field on the other (which are obviously brought about by superposition of elementary waves emitted independently from different atoms). It might come as a surprise (at least for those having quantum mechanical preconceptions) that the classical theory is valid down to arbitrarily small intensities: the visibility of the interference pattern does not deteriorate even for very small intensities – the zero point fluctuations of the electromagnetic field advocated by quantum mechanics do not have a disturbing effect – and is valid not only for conventional interference experiments but also for interference between independently generated light beams (in the form of laser light).
- Type
- Chapter
- Information
- Introduction to Quantum OpticsFrom Light Quanta to Quantum Teleportation, pp. 215 - 218Publisher: Cambridge University PressPrint publication year: 2004