Diffraction by Organized Layers — Question 8

Section 36-9 · Physics pages 6026–6027

Question 8 A finite stack of planes gives a finite Bragg-peak width N equally spaced coherent planes have adjacent-plane phase δ = 4πd sin θ/λ. Near a Bragg maximum, the first array zero occurs at |∆δ| = 2π/N. For a large stack define thickness T ≃Nd. Let T = 50.0 nm, λ = 0.154 nm, and θB = 30◦. d θ T Schematic; labels, not drawing lengths, specify the data. (a) Derive the offset in Bragg angle from the peak to its nearest zero. (b) Find that offset in detector scattering angle 2θ, in radians and degrees.
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Question 8 - Solution A finite stack of planes gives a finite Bragg-peak width d θ T (a) Method and calculation ∆δ ≃4πd cos θB λ ∆θ = 2π N . |∆θ| = λ 2Nd cos θB ≃ λ 2T cos θB . (b) Interpretation and further calculation |∆(2θ)| = λ T cos θB = 0.00355648 rad . |∆(2θ)| = 0.203771◦ from peak to first zero . Physical check This is a first-zero offset, not a full width at half maximum; line-width conventions must be kept separate.

Question 8

A finite stack of planes gives a finite Bragg-peak width

N equally spaced coherent planes have adjacent-plane phase δ=4πdsin⁡θ/λ\delta=4\pi d\sin\theta/\lambda. Near a Bragg maximum, the first array zero occurs at |Δδ|=2π/N|\Delta\delta|=2\pi/N. For a large stack define thickness T≃NdT\simeq Nd. Let T=50.0nmT=50.0\,\mathrm{nm}, λ=0.154nm\lambda=0.154\,\mathrm{nm}, and θB=30∘\theta_B=30^\circ.

Diagram shown in the original SVG worksheet.

  1. Derive the offset in Bragg angle from the peak to its nearest zero.

  2. Find that offset in detector scattering angle 2θ2\theta, in radians and degrees.

Question 8 - Solution

A finite stack of planes gives a finite Bragg-peak width

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δδ≃4πdcos⁡θBλΔθ=2πN.\Delta\delta\simeq\frac{4\pi d\cos\theta_B}{\lambda}\Delta\theta=\frac{2\pi}{N}.|Δθ|=λ2Ndcos⁡θB≃λ2Tcos⁡θB.\boxed{|\Delta\theta|=\frac{\lambda}{2Nd\cos\theta_B}\simeq\frac{\lambda}{2T\cos\theta_B}}.

(b) Interpretation and further calculation

|Δ(2θ)|=λTcos⁡θB=0.00355648rad.\boxed{|\Delta(2\theta)|=\frac{\lambda}{T\cos\theta_B}=0.00355648\,\mathrm{rad}}.|Δ(2θ)|=0.203771∘from peak to first zero.\boxed{|\Delta(2\theta)|=0.203771^\circ\quad\text{from peak to first zero}}.

Physical check

This is a first-zero offset, not a full width at half maximum; line-width conventions must be kept separate.