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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Optical phase space ： ウィキペディア英語版 Optical phase space In quantum optics, an optical phase space is a phase space in which all quantum states of an optical system are described. Each point in the optical phase space corresponds to a unique state of an ''optical system''. For any such system, a plot of the ''quadratures'' against each other, possibly as functions of time, is called a phase diagram. If the quadratures are functions of time then the optical phase diagram can show the evolution of a quantum optical system with time. An optical phase diagram can give insight into the properties and behaviors of the system that might otherwise not be obvious. This can allude to qualities of the system that can be of interest to an individual studying an optical system that would be very hard to deduce otherwise. Another use for an optical phase diagram is that it shows the evolution of the state of an optical system. This can be used to determine the state of the optical system at any point in time. ==Background information== When discussing the quantum theory of light, it is very common to use an electromagnetic oscillator as a model. An electromagnetic oscillator describes an oscillation of the electric field. Since the magnetic field is proportional to the rate of change of the electric field, this too oscillates. Such oscillations describe light. Systems composed of such oscillators can be described by an optical phase space. Let u(x,t) be a vector function describing a single mode of an electromagnetic oscillator. For simplicitity, it is assumed that this electromagnetic oscillator is in vacuum. An example is the plane wave given by :$\backslash mathbf(\backslash mathbf,t)\; =\; \backslash mathbf\; \backslash cdot\; \backslash mathbf\; -\; wt)\}$ where u0 is the polarization vector, k is the wave vector, w the frequency, and A$\backslash cdot$B denotes the dot product between the vectors A and B. This is the equation for a plane wave and is a simple example of such an electromagnetic oscillator. The oscillators being examined could either be free waves in space or some normal mode contained in some cavity. A single mode of the electromagnetic oscillator is isolated from the rest of the system and examined. Such an oscillator, when quantized, is described by the mathematics of a quantum harmonic oscillator.〔 Quantum oscillators are described using creation and annihilation operators $\backslash widehat\; a^\backslash dagger$ and $\backslash widehat\; a$. Physical quantities, such as the electric field strength, then become quantum operators. In order to distinguish a physical quantity from the quantum mechanical operator used to describe it, a "hat" is used over the operator symbols. Thus, for example, where $E\_i$ might represent (one component of) the electric field, the symbol $\backslash widehat\; E\_i$ denotes the quantum-mechanical operator that describes $E\_i$. This convention is used throughout this article, but is not in common use in more advanced texts, which avoid the hat, as it simply clutters the text. In the quantum oscillator mode, most operators representing physical quantities are typically expressed in terms of the creation and annihilation operators. In this example, the electric field strength is given by: :$\backslash widehat\_=u\_^(\backslash mathbf,t)\backslash widehat^\; +\; u\_(\backslash mathbf,t)\backslash widehat$ (where ''xi'' is a single component of x, position). The Hamiltonian for an electromagnetic oscillator is found by quantizing the electromagnetic field for this oscillator and the formula is given by: :$\backslash widehat\; =\; \backslash hbar\backslash omega\; (\backslash widehat^\backslash widehat\; +\; 1/2)$〔 where $\backslash omega$ is the frequency of the (spatio-temportal) mode. The annihilation operator is the bosonic annihilation operator and so it obeys the canonical commutation relation given by: :$()\; =\; 1$ The eigenstates of the annihilation operator are called coherent states: :$\backslash widehat|\backslash alpha\backslash rangle\; =\; \backslash alpha|\backslash alpha\backslash rangle$ It is important to note that the annihilation operator is not Hermitian; therefore its eigenvalues $\backslash alpha$ can be complex. This has important consequences. Finally, the photon number is given by the operator $\backslash widehat\; =\; \backslash widehat^\; \backslash widehat,$ which gives the number of photons in the given (spatial-temporal) mode u. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Optical phase space」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.