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Titlebook: An Open Systems Approach to Quantum Optics; Lectures Presented a Howard Carmichael Book 1993 Springer-Verlag Berlin Heidelberg 1993 Heisenb

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發(fā)表于 2025-3-21 16:15:11 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
期刊全稱(chēng)An Open Systems Approach to Quantum Optics
期刊簡(jiǎn)稱(chēng)Lectures Presented a
影響因子2023Howard Carmichael
視頻videohttp://file.papertrans.cn/156/155673/155673.mp4
學(xué)科分類(lèi)Lecture Notes in Physics Monographs
圖書(shū)封面Titlebook: An Open Systems Approach to Quantum Optics; Lectures Presented a Howard Carmichael Book 1993 Springer-Verlag Berlin Heidelberg 1993 Heisenb
影響因子This volume contains ten lectures presented in the series ULB Lectures in Nonlinear Optics at the Universite Libre de Bruxelles during the period October 28 to November 4, 1991. A large part of the first six lectures is taken from material prepared for a book of somewhat larger scope which will be published,by Springer under the title Quantum Statistical Methods in Quantum Optics. The principal reason for the early publication of the present volume concerns the material contained in the last four lectures. Here I have put together, in a more or less systematic way, some ideas about the use of stochastic wavefunctions in the theory of open quantum optical systems. These ideas were developed with the help of two of my students, Murray Wolinsky and Liguang Tian, over a period of approximately two years. They are built on a foundation laid down in a paper written with Surendra Singh, Reeta Vyas, and Perry Rice on waiting-time distributions and wavefunction collapse in resonance fluorescence [Phys. Rev. A, 39, 1200 (1989)]. The ULB lecture notes contain my first serious atte~pt to give a complete account of the ideas and their potential applications. I am grateful to Professor Paul Mand
Pindex Book 1993
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Master Equations and Sources I,ce, irreversibly, before they encounter the detector. In the second, the detector is a major intrusion; if it turns photons into photoelectrons it removes photons from an otherwise lossless cavity; the description of the cavity field dynamics when the detector is present must be quite different from the description when it is not.
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Photoelectric Detection I,. The bridge is built on an understanding of the way in which optical fields are observed. Photoemissive sources are eventually observed by photoelectric detectors. We will spend the next two lectures discussing various aspects of photoelectric detection.
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Master Equations and Sources II,ock for the construction of more interesting sources. Excited atoms act as a source of radiation through spontaneous and stimulated emission. We are going to use the master equation approach from Sect. 1.2 to treat these processes for an atom in thermal equilibrium.
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Photoelectric Detection II,he field amplitude; the amplitude fluctuations of a quantized field can also do things that are not reproducible by classical stochastics — so-called .. Homodyne detection and squeezing are the subjects of this lecture. We begin with a brief description of squeezed light.
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Book 1993ber 28 to November 4, 1991. A large part of the first six lectures is taken from material prepared for a book of somewhat larger scope which will be published,by Springer under the title Quantum Statistical Methods in Quantum Optics. The principal reason for the early publication of the present volu
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0940-7677 eriod October 28 to November 4, 1991. A large part of the first six lectures is taken from material prepared for a book of somewhat larger scope which will be published,by Springer under the title Quantum Statistical Methods in Quantum Optics. The principal reason for the early publication of the pr
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