More Electron Traps — Question 9

Section 39-5 · Physics pages 6508–6509

Question 9 Detuning two traps suppresses the maximum tunneling transfer probability For two localized states use H = (∆/2)(|L⟩⟨L| −|R⟩⟨R|) −J(|L⟩⟨R| + |R⟩⟨L|), with J > 0. If the electron starts on the left, PR(t) = [J2/Ω2] sin2(Ωt/ℏ), where Ω= √ J2 + ∆2/4. L R ∆ Schematic; labels, not drawing lengths, specify the data. (a) Find the two energies and the maximum transfer probability. (b) Find the smallest magnitude of detuning that makes the maximum probability no greater than .200.
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Question 9 - Solution Detuning two traps suppresses the maximum tunneling transfer probability L R ∆ (a) Method and calculation det(H −EI) = E2 −J2 −∆2/4 = 0 ⇒E± = ±Ω. PR,max = 4J2 4J2 + ∆2 . (b) Interpretation and further calculation 4J2 4J2 + ∆2 ≤.200 ⇒∆2 ≥16J2. |∆|min = 4J . Physical check Increasing detuning raises the oscillation frequency while reducing transfer contrast. Faster oscillation therefore does not imply more complete transport.

Question 9

Detuning two traps suppresses the maximum tunneling transfer probability

For two localized states use H=(Δ/2)(|L⟩⟨L|−|R⟩⟨R|)−J(|L⟩⟨R|+|R⟩⟨L|)H=(\Delta/2)(|L\rangle\langle L|-|R\rangle\langle R|)-J(|L\rangle\langle R|+|R\rangle\langle L|), with J>0J>0. If the electron starts on the left, PR(t)=[J2/Ω2]sin⁡2(Ωt/ℏ)P_R(t)=[J^2/\Omega^2]\sin^2(\Omega t/\hbar), where Ω=J2+Δ2/4\Omega=\sqrt{J^2+\Delta^2/4}.

Diagram shown in the original SVG worksheet.

  1. Find the two energies and the maximum transfer probability.

  2. Find the smallest magnitude of detuning that makes the maximum probability no greater than .200.

Question 9 - Solution

Detuning two traps suppresses the maximum tunneling transfer probability

Diagram shown in the original SVG worksheet.

(a) Method and calculation

det⁡(H−EI)=E2−J2−Δ2/4=0⇒E±=±Ω.\det(H-EI)=E^2-J^2-\Delta^2/4=0\Rightarrow\boxed{E_\pm=\pm\Omega}.PR,max=4J24J2+Δ2.\boxed{P_{R,\max}=\frac{4J^2}{4J^2+\Delta^2}}.

(b) Interpretation and further calculation

4J24J2+Δ2≤.200⇒Δ2≥16J2.\frac{4J^2}{4J^2+\Delta^2}\le.200\Rightarrow\Delta^2\ge16J^2.|Δ|min=4J.\boxed{|\Delta|_{\min}=4J}.

Physical check

Increasing detuning raises the oscillation frequency while reducing transfer contrast. Faster oscillation therefore does not imply more complete transport.