Heisenberg's Uncertainty Principle — Question 5

Section 38-7 · Physics pages 6380–6381

Question 5 An exponential position state obeys the bound without saturating it A normalized state is ψ(x) = √κe−κ|x|, where κ > 0. Use ∫∞ 0 x2e−bxdx = 2/b3 and the momentum second-moment form ⟨p2⟩= ℏ2 ∫|ψ′|2dx. Both means vanish by symmetry. All uncertainties here are standard deviations, with σxσp ≥ℏ/2. x ψ Schematic; labels, not drawing lengths, specify the data. (a) Find the position variance. (b) Find the momentum variance and compare the uncertainty product with the Gaussian limit.
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Question 5 - Solution An exponential position state obeys the bound without saturating it x ψ (a) Method and calculation σ2 x = 2κ ∫∞ 0 x2e−2κxdx = 1 2κ2 . σx = 1/( √ 2κ) . (b) Interpretation and further calculation |ψ′|2 = κ2|ψ|2 away from 0 ⇒ σp = ℏκ . σxσp = ℏ/ √ 2 > ℏ/2 . Physical check The cusp has a square-integrable first derivative, so the momentum second moment is finite. It must not be confused with a discontinuous top-hat wave function.

Question 5

An exponential position state obeys the bound without saturating it

A normalized state is ψ(x)=κe−κ|x|\psi(x)=\sqrt\kappa e^{-\kappa|x|}, where κ>0\kappa>0. Use ∫0∞x2e−bxdx=2/b3\int_0^\infty x^2e^{-bx}dx=2/b^3 and the momentum second-moment form ⟨p2⟩=ℏ2∫|ψ′|2dx\langle p^2\rangle=\hbar^2\int|\psi\prime|^2dx. Both means vanish by symmetry. All uncertainties here are standard deviations, with σxσp≥ℏ/2\sigma_x\sigma_p\ge\hbar/2.

Diagram shown in the original SVG worksheet.

  1. Find the position variance.

  2. Find the momentum variance and compare the uncertainty product with the Gaussian limit.

Question 5 - Solution

An exponential position state obeys the bound without saturating it

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σx2=2κ∫0∞x2e−2κxdx=12κ2.\sigma_x^2=2\kappa\int_0^\infty x^2e^{-2\kappa x}dx=\frac1{2\kappa^2}.σx=1/(2κ).\boxed{\sigma_x=1/(\sqrt2\kappa)}.

(b) Interpretation and further calculation

|ψ′|2=κ2|ψ|2away from 0⇒σp=ℏκ.|\psi\prime|^2=\kappa^2|\psi|^2\quad\text{away from }0\quad\Rightarrow\quad\boxed{\sigma_p=\hbar\kappa}.σxσp=ℏ/2>ℏ/2.\boxed{\sigma_x\sigma_p=\hbar/\sqrt2>\hbar/2}.

Physical check

The cusp has a square-integrable first derivative, so the momentum second moment is finite. It must not be confused with a discontinuous top-hat wave function.