Book contents
- Frontmatter
- Contents
- Acknowledgements
- 1 Introduction
- 2 Field quantization
- 3 Coherent states
- 4 Emission and absorption of radiation by atoms
- 5 Quantum coherence functions
- 6 Beam splitters and interferometers
- 7 Nonclassical light
- 8 Dissipative interactions and decoherence
- 9 Optical test of quantum mechanics
- 10 Experiments in cavity QED and with trapped ions
- 11 Applications of entanglement: Heisenberg-limited interferometry and quantum information processing
- Appendix A The density operator, entangled states, the Schmidt decomposition, and the von Neumann entropy
- Appendix B Quantum measurement theory in a (very small) nutshell
- Appendix C Derivation of the effective Hamiltonian for dispersive (far off-resonant) interactions
- Appendix D Nonlinear optics and spontaneous parametric down-conversion
- Index
- References
3 - Coherent states
Published online by Cambridge University Press: 05 September 2012
- Frontmatter
- Contents
- Acknowledgements
- 1 Introduction
- 2 Field quantization
- 3 Coherent states
- 4 Emission and absorption of radiation by atoms
- 5 Quantum coherence functions
- 6 Beam splitters and interferometers
- 7 Nonclassical light
- 8 Dissipative interactions and decoherence
- 9 Optical test of quantum mechanics
- 10 Experiments in cavity QED and with trapped ions
- 11 Applications of entanglement: Heisenberg-limited interferometry and quantum information processing
- Appendix A The density operator, entangled states, the Schmidt decomposition, and the von Neumann entropy
- Appendix B Quantum measurement theory in a (very small) nutshell
- Appendix C Derivation of the effective Hamiltonian for dispersive (far off-resonant) interactions
- Appendix D Nonlinear optics and spontaneous parametric down-conversion
- Index
- References
Summary
At the end of the preceding chapter, we showed that the photon number states |n〉 have a uniform phase distribution over the range 0 to 2π. Essentially, then, there is no well-defined phase for these states and, as we have already shown, the expectation value of the field operator for a number state vanishes. It is frequently suggested (see, for example, Sakurai) that the classical limit of the quantized field is the limit in which the number of photons becomes very large such that the number operator becomes a continuous variable. However, this cannot be the whole story since the mean field 〈n|Êx|n〉 = 0 no matter how large the value of n. We know that at a fixed point in space a classical field oscillates sinusoidally in time. Clearly this does not happen for the expectation value of the field operator for a number state. In this chapter we present a set of states, the coherent states, which do give rise to a sensible classical limit; and, in fact, these states are the “most classical” quantum states of a harmonic oscillator, as we shall see.
Eigenstates of the annihilation operator and minimum uncertainty states
In order to have a non-zero expectation value of the electric field operator or, equivalently, of the annihilation and creation operators, we are required to have a superposition of number states differing only by ±1.
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- Information
- Introductory Quantum Optics , pp. 43 - 73Publisher: Cambridge University PressPrint publication year: 2004