Heisenberg's Uncertainty Principle — Question 9

Section 38-7 · Physics pages 6388–6389

Question 9 Optimizing the initial width minimizes free-packet spreading at a chosen time An unchirped minimum-uncertainty Gaussian of initial rms width a evolves freely for a fixed time T > 0. Its final position variance is f(a) = a2 + ℏ2T 2/(4m2a2). Only a may be varied; the initial covariance is fixed at zero. a σ2 x(T) aopt Schematic; labels, not drawing lengths, specify the data. (a) Find the initial width that minimizes f. (b) Find the smallest final width and compare the two terms in f at the optimum.
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Question 9 - Solution Optimizing the initial width minimizes free-packet spreading at a chosen time a σ2 x(T) aopt (a) Method and calculation df da = 2a −ℏ2T 2 2m2a3 = 0 ⇒ a4 = ℏ2T 2 4m2 . a2 opt = ℏT/(2m) . (b) Interpretation and further calculation fmin = ℏT 2m + ℏT 2m = ℏT m . σx,min(T) = √ ℏT/m = √ 2 aopt . Physical check Tighter initial localization increases momentum spread. This optimization applies to the stated unchirped family; allowing initial correlations changes the focusing problem.

Question 9

Optimizing the initial width minimizes free-packet spreading at a chosen time

An unchirped minimum-uncertainty Gaussian of initial rms width a evolves freely for a fixed time T>0T>0. Its final position variance is f(a)=a2+ℏ2T2/(4m2a2)f(a)=a^2+\hbar^2T^2/(4m^2a^2). Only a may be varied; the initial covariance is fixed at zero.

Diagram shown in the original SVG worksheet.

  1. Find the initial width that minimizes f.

  2. Find the smallest final width and compare the two terms in f at the optimum.

Question 9 - Solution

Optimizing the initial width minimizes free-packet spreading at a chosen time

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dfda=2a−ℏ2T22m2a3=0⇒a4=ℏ2T24m2.\frac{df}{da}=2a-\frac{\hbar^2T^2}{2m^2a^3}=0\quad\Rightarrow\quad a^4=\frac{\hbar^2T^2}{4m^2}.aopt2=ℏT/(2m).\boxed{a_{\mathrm{opt}}^2=\hbar T/(2m)}.

(b) Interpretation and further calculation

fmin=ℏT2m+ℏT2m=ℏTm.f_{\min}=\frac{\hbar T}{2m}+\frac{\hbar T}{2m}=\frac{\hbar T}{m}.σx,min(T)=ℏT/m=2aopt.\boxed{\sigma_{x,\min}(T)=\sqrt{\hbar T/m}=\sqrt2\,a_{\mathrm{opt}}}.

Physical check

Tighter initial localization increases momentum spread. This optimization applies to the stated unchirped family; allowing initial correlations changes the focusing problem.