More Electron Traps — Question 2

Section 39-5 · Physics pages 6494–6495

Question 2 The ground-state rms size is smaller than the classical turning radius A one-dimensional harmonic trap has V (x) = mω2x2/2 and En = (n + 1/2)ℏω, n = 0, 1, 2, . . .. The ground state has ⟨x2⟩= ℏ/(2mω) and zero mean position. For an electron use ℏω = .0800 eV and ℏ2/(2me) = .0381 eV nm2. x −xt xt Schematic; labels, not drawing lengths, specify the data. (a) Find the ground-state position standard deviation. (b) Find the classical turning position at energy E0 and compare it with the standard deviation.
Show solutionHide solution
Question 2 - Solution The ground-state rms size is smaller than the classical turning radius x −xt xt (a) Method and calculation σ2 x = ℏ2/(2me) ℏω = .0381 .0800 nm2. σx = .690109 nm . (b) Interpretation and further calculation 1 2mω2x2 t = 1 2ℏω ⇒xt = √ ℏ/(mω) = √ 2 σx . xt = .975961 nm . Physical check A quantum ground state has tails beyond the classical turning positions. The rms size is a moment of the full density, not a sharp edge.

Question 2

The ground-state rms size is smaller than the classical turning radius

A one-dimensional harmonic trap has V(x)=mω2x2/2V(x)=m\omega^2x^2/2 and En=(n+1/2)ℏωE_n=(n+1/2)\hbar\omega, n=0,1,2,…n=0,1,2,\ldots. The ground state has ⟨x2⟩=ℏ/(2mω)\langle x^2\rangle=\hbar/(2m\omega) and zero mean position. For an electron use ℏω=.0800eV\hbar\omega=.0800\,\mathrm{eV} and ℏ2/(2me)=.0381eVnm2\hbar^2/(2m_e)=.0381\,\mathrm{eV\,nm^2}.

Diagram shown in the original SVG worksheet.

  1. Find the ground-state position standard deviation.

  2. Find the classical turning position at energy E0E_0 and compare it with the standard deviation.

Question 2 - Solution

The ground-state rms size is smaller than the classical turning radius

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σx2=ℏ2/(2me)ℏω=.0381.0800nm2.\sigma_x^2=\frac{\hbar^2/(2m_e)}{\hbar\omega}=\frac{.0381}{.0800}\,\mathrm{nm^2}.σx=.690109nm.\boxed{\sigma_x=.690109\,\mathrm{nm}}.

(b) Interpretation and further calculation

12mω2xt2=12ℏω⇒xt=ℏ/(mω)=2σx.\tfrac12m\omega^2x_t^2=\tfrac12\hbar\omega\Rightarrow\boxed{x_t=\sqrt{\hbar/(m\omega)}=\sqrt2\,\sigma_x}.xt=.975961nm.\boxed{x_t=.975961\,\mathrm{nm}}.

Physical check

A quantum ground state has tails beyond the classical turning positions. The rms size is a moment of the full density, not a sharp edge.