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< Exact Solution of Uda Equation (5) > | ||||||||||||
In this page, I write exact solutions of Energy Representation of Uda Equation (1). Any unentangled solution is functional Φ such that where ∀n ∈ Z; cn ∈ C. The quantum history represented by this solution is the same history as represented by wave function ψ such that ψ(n, t) = exp(-iωtn + cn) = λn exp(-iωnt) in the old grammar. Here, λn ≡ exp(cn). If A†A|n> = n|n>, Σn=0∞ ψ(n, t)|n> = Σn=0∞ λnexp(-iωnt)|n>, Σn=0∞ ψ(n, 0)|n> = Σn=0∞ λn|n>. Of course, any superposition of unentangled solutions is also a solution. Moreover, any entangled solution perhaps is a superposition of unentangled solutions. It is functional Φ such that where ∀n ∈ Z; an ∈ R and bn ∈ R and f(a0, b0, a1, b1, a2, b2, ・・・) ∈ C. cn = an + ibn, λn = exp(an + ibn). Normalization condition for initial state is that . To let the integral converge, b and ν is restricted. However, I do not put such a condition because there is no ambiguity even if the integral diverges. --- The content of this page was developed in Number Representation of Uda Equation @ Quantum History Theory @ Problems. |
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Author Yuichi Uda, Write start at 2019/11/08/17:22JST, Last edit at 2019/11/22/18:45JST | ||||||||||||
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