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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 Schrödinger picture ： ウィキペディア英語版 Schrödinger picture In physics, the Schrödinger picture (also called the Schrödinger representation〔(【引用サイトリンク】url=http://www.encyclopediaofmath.org/index.php/Schr%C3%B6dinger_representation )〕) is a formulation of quantum mechanics in which the state vectors evolve in time, but the operators (observables and others) are constant with respect to time. This differs from the Heisenberg picture which keeps the states constant while the observables evolve in time, and from the interaction picture in which both the states and the observables evolve in time. The Schrödinger and Heisenberg pictures are related as active and passive transformations and commutation relations between operators are preserved in the passage between the two pictures. In the Schrödinger picture, the state of a system evolves with time. The evolution for a closed quantum system is brought about by a unitary operator, the time evolution operator. For time evolution from a state vector $|\backslash psi(t\_0)\backslash rangle$ at time $t\_0$ to a state vector $|\backslash psi(t)\backslash rangle$ at time $t$, the time-evolution operator is commonly written $U(t,\; t\_0)$, and one has :$|\backslash psi(t)\backslash rangle\; =\; U(t,\; t\_0)\; |\backslash psi(t\_0)\backslash rangle.$ In the case where the Hamiltonian of the system does not vary with time, the time-evolution operator has the form :$U(t,\; t\_0)\; =\; e^,$ where the exponent is evaluated via its Taylor series. The Schrödinger picture is useful when dealing with a time-independent Hamiltonian H; that is, $\backslash partial\_tH=0$. ==Background== In elementary quantum mechanics, the state of a quantum-mechanical system is represented by a complex-valued wavefunction ψ(''x'', ''t''). More abstractly, the state may be represented as a state vector, or ''ket'', $|\; \backslash psi\; \backslash rangle$. This ket is an element of a ''Hilbert space'', a vector space containing all possible states of the system. A quantum-mechanical operator is a function which takes a ket $|\; \backslash psi\; \backslash rangle$ and returns some other ket $|\; \backslash psi\text{'}\; \backslash rangle$. The differences between the Schrödinger and Heisenberg pictures of quantum mechanics revolve around how to deal with systems that evolve in time: the time-dependent nature of the system ''must'' be carried by some combination of the state vectors and the operators. For example, a quantum harmonic oscillator may be in a state $|\; \backslash psi\; \backslash rangle$ for which the expectation value of the momentum, $\backslash langle\; \backslash psi\; |\; \backslash hat\; |\; \backslash psi\; \backslash rangle$, oscillates sinusoidally in time. One can then ask whether this sinusoidal oscillation should be reflected in the state vector $|\; \backslash psi\; \backslash rangle$, the momentum operator $\backslash hat$, or both. All three of these choices are valid; the first gives the Schrödinger picture, the second the Heisenberg picture, and the third the interaction picture. 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「Schrödinger picture」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.