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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 equivalence theorem ： ウィキペディア英語版 Optical equivalence theorem The optical equivalence theorem in quantum optics asserts an equivalence between the expectation value of an operator in Hilbert space and the expectation value of its associated function in the phase space formulation with respect to a quasiprobability distribution. The theorem was first reported by George Sudarshan in 1963 for normally ordered operators〔E. C. G. Sudarshan "Equivalence of Semiclassical and Quantum Mechanical Descriptions of Statistical Light Beams", ''Phys. Rev. Lett.'',10 (1963) pp. 277–279. 〕 and generalized later that decade to any ordering.〔K. E. Cahill and R. J. Glauber "Ordered Expansions in Boson Amplitude Operators", ''Phys. Rev.'',177 (1969) pp. 1857–1881. 〕〔K. E. Cahill and R. J. Glauber "Density Operators and Quasiprobability Distributions", ''Phys. Rev.'',177 (1969) pp. 1882–1902. 〕〔G. S. Agarwal and E. Wolf "Calculus for Functions of Noncommuting Operators and General Phase-Space Methods in Quantum Mechanics. I. Mapping Theorems and Ordering of Functions of Noncommuting Operators", ''Phys. Rev. D'',2 (1970) pp. 2161–2186. 〕〔G. S. Agarwal and E. Wolf "Calculus for Functions of Noncommuting Operators and General Phase-Space Methods in Quantum Mechanics. II. Quantum Mechanics in Phase Space", ''Phys. Rev. D'',2 (1970) pp. 2187–2205. 〕 Let Ω be an ordering of the non-commutative creation and annihilation operators, and let $g\_(\backslash hat,\backslash hat^)$ be an operator that is expressible as a power series in the creation and annihilation operators that satisfies the ordering Ω. Then the optical equivalence theorem is succinctly expressed as :$\backslash langle\; g\_(\backslash hat,\backslash hat^)\; \backslash rangle\; =\; \backslash langle\; g\_(\backslash alpha,\backslash alpha^$ *) \rangle. Here, α is understood to be the eigenvalue of the annihilation operator on a coherent state and is replaced formally in the power series expansion of ''g''. The left side of the above equation is an expectation value in the Hilbert space whereas the right hand side is an expectation value with respect to the quasiprobability distribution. We may write each of these explicitly for better clarity. Let $\backslash hat$ be the density operator and $\}(\backslash alpha,\backslash alpha^$ *) = \frac \int \rho_( \hat \cdot g_(\hat,\hat^)) = \int f_(\alpha,\alpha^ *) \, d^2\alpha. For example, let Ω be the normal order. This means that ''g'' can be written in a power series of the following form: :$g\_(\backslash hat^\backslash dagger,\; \backslash hat)\; =\; \backslash sum\_\; c\_\; \backslash hat^\; \backslash hat^m.$ The quasiprobability distribution associated with the normal order is the Glauber-Sudarshan P representation. In these terms, we arrive at :$\backslash mathrm(\; \backslash hat\; \backslash cdot\; g\_N(\backslash hat,\backslash hat^))\; =\; \backslash int\; P(\backslash alpha)\; g(\backslash alpha,\backslash alpha^$ *) \, d^2\alpha. This theorem implies the formal equivalence between expectation values of normally ordered operators in quantum optics and the corresponding complex numbers in classical optics. ==References== 〔 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 equivalence theorem」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.