Diffraction by Organized Layers — Question 10

Section 36-9 · Physics pages 6030–6031

Question 10 Scattering-vector magnitude is independent of the chosen probe wavelength at a fixed reflection Elastic scattering has incident and outgoing wave-vector magnitudes k = 2π/λ and angle 2θ between them. Define Q = kf −ki. Consider first-order scattering from planes spaced d = 0.200 nm. ki kf Q Schematic; labels, not drawing lengths, specify the data. (a) Use vector geometry and Bragg’s law to derive Q at the reflection. (b) Find the scattering angles for wavelengths 0.100 nm and 0.150 nm, and verify that both give the same Q.
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Question 10 - Solution Scattering-vector magnitude is independent of the chosen probe wavelength at a fixed reflection ki kf Q (a) Method and calculation Q2 = 2k2[1 −cos(2θ)] = 4k2 sin2 θ =⇒Q = 4π sin θ/λ. 2d sin θ = λ =⇒Q = 2π/d = 10π nm−1 . (b) Interpretation and further calculation 2θ0.100 = 2 sin−1(0.25) = 28.9550◦. 2θ0.150 = 2 sin−1(0.375) = 44.0486◦; 4π(0.25)/0.100 = 4π(0.375)/0.150 = 10π. Physical check Changing wavelength moves the measured angular position but leaves the reciprocal-space location of the same lattice reflection unchanged.

Question 10

Scattering-vector magnitude is independent of the chosen probe wavelength at a fixed reflection

Elastic scattering has incident and outgoing wave-vector magnitudes k=2π/λk=2\pi/\lambda and angle 2θ2\theta between them. Define 𝑸=𝒌f−𝒌i\mathbf Q=\mathbf k_f-\mathbf k_i. Consider first-order scattering from planes spaced d=0.200nmd=0.200\,\mathrm{nm}.

Diagram shown in the original SVG worksheet.

  1. Use vector geometry and Bragg’s law to derive Q at the reflection.

  2. Find the scattering angles for wavelengths 0.100nm0.100\,\mathrm{nm} and 0.150nm0.150\,\mathrm{nm}, and verify that both give the same Q.

Question 10 - Solution

Scattering-vector magnitude is independent of the chosen probe wavelength at a fixed reflection

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q2=2k2[1−cos⁡(2θ)]=4k2sin⁡2θ⇒Q=4πsin⁡θ/λ.Q^2=2k^2[1-\cos(2\theta)]=4k^2\sin^2\theta\Longrightarrow Q=4\pi\sin\theta/\lambda.2dsin⁡θ=λ⇒Q=2π/d=10πnm−1.2d\sin\theta=\lambda\Longrightarrow\boxed{Q=2\pi/d=10\pi\,\mathrm{nm^{-1}}}.

(b) Interpretation and further calculation

2θ0.100=2sin⁡−1(0.25)=28.9550∘.\boxed{2\theta_{0.100}=2\sin^{-1}(0.25)=28.9550^\circ}.2θ0.150=2sin⁡−1(0.375)=44.0486∘;4π(0.25)/0.100=4π(0.375)/0.150=10π.\boxed{2\theta_{0.150}=2\sin^{-1}(0.375)=44.0486^\circ};\quad4\pi(0.25)/0.100=4\pi(0.375)/0.150=10\pi.

Physical check

Changing wavelength moves the measured angular position but leaves the reciprocal-space location of the same lattice reflection unchanged.