Titlebook: Elements of Quantum Optics; Pierre Meystre,Murray Sargent Textbook 19912nd edition Springer-Verlag Berlin Heidelberg 1991 Absorption.Laser

ACTIN

Three and Four Wave Mixing,rgies, e.g., in the third-order product .*.. This is built into the concept of the rotating-wave approximation, whether taken classically or quantum mechanically. Because of the .*, it is possible to conjugate a wave front. Section 2–4 discusses the conjugation of a plane wave front in a classical .

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小蟲

上漲

Field Quantization, to quantize the electromagnetic field. Such a semiclassical description is sufficient to describe most problems in quantum optics. However, there are a few notable exceptions where a classical description of the field leads to the wrong answer. These include spontaneous emission, the Lamb shift, re

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Interaction between Atoms and Quantized Fields, with many experiments. Nevertheless several significant experiments show strong disagreements with such semiclassical theories. The present Chapter treats the atom-field interaction fully quantum mechanically, providing a basic understanding of spontaneous emission and laying the foundations for th

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System-Reservoir Interactions,to a large system. In that case the small system is the atom and the large system is the continuum of modes of the electromagnetic field. When computing the atomic decay rate, we were not interested in the field itself, but only on its effect on the atomic dynamics. Thus we never explicitly computed

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EVICT

Quantum Theory of a Laser,2–14. So far, our treatment of quantized field-matter interactions has concentrated mostly on situations where the quantized field acts as a noise source: under these conditions the nonlinear atomic response originates from a . driving field, while the effects of the quantized modes are treated line

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