Heisenberg's Uncertainty Principle — Question 8

Section 38-7 · Physics pages 6386–6387

Question 8 A freely evolving minimum-uncertainty packet spreads through momentum dispersion Initially a free particle has an unchirped Gaussian with σx(0) = a, σp = ℏ/(2a) and Cxp(0) = 0. In free evolution x(t) = x(0) + p(0)t/m and p is constant. x later Schematic; labels, not drawing lengths, specify the data. (a) Derive the position variance at time t. (b) Find the positive time when the width doubles and the uncertainty product then.
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Question 8 - Solution A freely evolving minimum-uncertainty packet spreads through momentum dispersion x later (a) Method and calculation σ2 x(t) = σ2 x(0) + 2t mCxp(0) + t2 m2 σ2 p. σx(t) = a √ 1 + (t/t0)2 , t0 = 2ma2/ℏ. (b) Interpretation and further calculation σx(td) = 2a ⇒ td = √ 3 t0 = 2 √ 3 ma2/ℏ. σx(td)σp = (2a) ℏ 2a = ℏ. Physical check Free evolution preserves the momentum distribution but builds position-momentum correlation. The ordinary uncertainty product can increase even though the state remains pure.

Question 8

A freely evolving minimum-uncertainty packet spreads through momentum dispersion

Initially a free particle has an unchirped Gaussian with σx(0)=a\sigma_x(0)=a, σp=ℏ/(2a)\sigma_p=\hbar/(2a) and Cxp(0)=0C_{xp}(0)=0. In free evolution x(t)=x(0)+p(0)t/mx(t)=x(0)+p(0)t/m and p is constant.

Diagram shown in the original SVG worksheet.

  1. Derive the position variance at time t.

  2. Find the positive time when the width doubles and the uncertainty product then.

Question 8 - Solution

A freely evolving minimum-uncertainty packet spreads through momentum dispersion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σx2(t)=σx2(0)+2tmCxp(0)+t2m2σp2.\sigma_x^2(t)=\sigma_x^2(0)+\frac{2t}{m}C_{xp}(0)+\frac{t^2}{m^2}\sigma_p^2.σx(t)=a1+(t/t0)2,t0=2ma2/ℏ.\boxed{\sigma_x(t)=a\sqrt{1+(t/t_0)^2}},\quad t_0=2ma^2/\hbar.

(b) Interpretation and further calculation

σx(td)=2a⇒td=3t0=23ma2/ℏ.\sigma_x(t_d)=2a\quad\Rightarrow\quad\boxed{t_d=\sqrt3\,t_0=2\sqrt3\,ma^2/\hbar}.σx(td)σp=(2a)ℏ2a=ℏ.\boxed{\sigma_x(t_d)\sigma_p=(2a)\frac\hbar{2a}=\hbar}.

Physical check

Free evolution preserves the momentum distribution but builds position-momentum correlation. The ordinary uncertainty product can increase even though the state remains pure.