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3. /15 pts] Imagine solving the SE for a particular potential well and finding two stationary solutions. The first solution iConsider the quantum state ψ(r state at t = 0 is shown below: t)-V1 (a , t) + 2( , t A crude sketch of the PDF for this t 0 F

3. /15 pts] Imagine solving the SE for a particular potential well and finding two stationary solutions. The first solution i(x) has an energy Eo and of the (unnormalized) form: ψ1(x) = exp(-x2/2) The second solution U2(2) has an energy 3F0 and of the (unnormalized) form ψ2(x) = V2x exp(-x2/2
Consider the quantum state ψ(r state at t = 0 is shown below: t)-V1 (a , t) + 2( , t A crude sketch of the PDF for this t 0 Figure 1: PDF at t 0. (a) Write an explicit time dependent form for Ψ(a,t) in terms of E0 (b) Sketch the PDF at time - Th/(2Fo). (c) Find an expression for the earliest time where the PDF is an even function (i.e., PDF (r)-PDF(-)). And sketch the PDF at this time.
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e. 2 a NTPDF 又JT 어») 4与 一えー . 45+ 2x2-2Y2x) Exp[-x2], {x,-4, 4), AxesLabel Plot 2 EO PDF 2 EO 0.3 0.2 0.1 ()E], (x, -4, 4), axesLabel 4 EO PDF 0.35 0.25 0.20

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