To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure no-reply@cambridge.org
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
In this chapter we discuss the interaction of radiation with matter, the latter taken to be a two-level atom. We consider interactions with both classical and quantum fields. We first introduce the dipole approximation and the rotating-wave approximation, and then study the Rabi model of a classical field interacting with a two-level atom. We next introduce the quantized field interaction with matter and discuss absorption, spontaneous emission, and stimulated emssion. We then discuss the long-time evolution of a single-mode field with a two-level atom –– the Jaynes––Cummings model.
In this chapter we first discuss the classical coherence functions and then introduce the quantum coherence functions. We present a quantum mechanical discussion of Young’s interference experiment. The Hanbury-Bown and Twiss experiment is discussed, along with higher-order coherence functions.
In this chapter we discuss nonclassical states of light. These include squeezed states of light, states with sub-Poissonian statistics, two-mode squeezed states, photon antibunching, superpositions of coherent states of light –– these being the Schrödinger-cat states. Also discussed in this chapter are the nonclassical states generated by the addition and subtraction of photons.
In this chapter we discuss optical tests of quantum mechanics. These include the Hong––Ou––Mandel effect, quantum erasure, induced coherence, superluminal tunneling of photons, violations of Bell’s inequality, and Franson’s experiment.
In this chapter we discuss the effects of losses on quantum optical systems. We discuss quantum jumps and master equations. We introduce the notion of using fictitious beam splitters to model losses. We introduce the decoherence of pure quantum mechanical states into a statistical mixture.
In this chapter we introduce the Glauber coherent states of a quantized field as eigenstates of the annihilation operator and as displaced vacuum states. The phase-space picture of coherent states is introduced, along with phase-space probability distributions, namely the Q distribution, the P distribution, and the Wigner function, and their interrelations are discussed.
In this chapter we discuss the application of entanglement to quantum optical interferometry and to quantum information processing. Quantum random number generation is discussed. Quantum cryptography is discussed, as is quantum computing. The quantum optical realization of some quantum gates is discussed.
In this chapter we discuss experiments in cavity QED and ion traps. We first discuss the nature of Rydberg atoms which are used in cavity QED experiments. The experimental realization of the Jaynes––Cummings model is discussed, as are the generation of Schrödinger-cat states in dispersive atom––field interactions in cavity QED. The quantum non-demolition measurement is discussed. The realization of the Jaynes––Cummings model in the context of trapped ions is discussed.