Magnetic Resonance — Question 4

Section 40-5 · Physics pages 6658–6659

Question 4 Detuning limits the maximum transfer even for an ideal pulse For a spin initially in its lower state, use Pe(t) = Ω2 Ω2+δ2 sin2[ √ Ω2 + δ2 t/2], with angular detuning δ = ω −ω0. Let δ = √ 3Ω. t Pe 1 Schematic; labels, not drawing lengths, specify the data. (a) Find the largest achievable excitation probability. (b) Find the first time this maximum occurs and compare it with the resonant inversion time.
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Question 4 - Solution Detuning limits the maximum transfer even for an ideal pulse t Pe 1 (a) Method and calculation Ωeff= √ Ω2 + 3Ω2 = 2Ω. Pe,max = Ω2/(4Ω2) = 1/4 . (b) Interpretation and further calculation Ωefftmax/2 = π/2 ⇒tmax = π/(2Ω) . tπ = π/Ω⇒tmax = tπ/2 . Physical check Faster oscillation away from resonance does not imply more efficient inversion. The rotation axis tilts and the accessible population excursion decreases.

Question 4

Detuning limits the maximum transfer even for an ideal pulse

For a spin initially in its lower state, use Pe(t)=Ω2Ω2+δ2sin⁡2[Ω2+δ2t/2]P_e(t)=\frac{\Omega^2}{\Omega^2+\delta^2}\sin^2[\sqrt{\Omega^2+\delta^2}\,t/2], with angular detuning δ=ω−ω0\delta=\omega-\omega_0. Let δ=3Ω\delta=\sqrt3\Omega.

Diagram shown in the original SVG worksheet.

  1. Find the largest achievable excitation probability.

  2. Find the first time this maximum occurs and compare it with the resonant inversion time.

Question 4 - Solution

Detuning limits the maximum transfer even for an ideal pulse

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ωeff=Ω2+3Ω2=2Ω.\Omega_{\mathrm{eff}}=\sqrt{\Omega^2+3\Omega^2}=2\Omega.Pe,max=Ω2/(4Ω2)=1/4.\boxed{P_{e,\max}=\Omega^2/(4\Omega^2)=1/4}.

(b) Interpretation and further calculation

Ωefftmax/2=π/2⇒tmax=π/(2Ω).\Omega_{\mathrm{eff}}t_{\max}/2=\pi/2\Rightarrow\boxed{t_{\max}=\pi/(2\Omega)}.tπ=π/Ω⇒tmax=tπ/2.t_\pi=\pi/\Omega\Rightarrow\boxed{t_{\max}=t_\pi/2}.

Physical check

Faster oscillation away from resonance does not imply more efficient inversion. The rotation axis tilts and the accessible population excursion decreases.