Compton scattering – the momentum of a photon

PhysicsQuantum & Nuclear PhysicsAges 17–18Virtual lab

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Use with my class

An X-ray photon hits an electron at rest and leaves at angle θ with a longer wavelength: λ′ − λ = (h/mₑc)(1 − cos θ). Drag to change the scattering angle and read the wavelength and photon energy before and after, the kinetic energy and direction of the recoil electron, and a vector diagram showing that momentum is conserved: p = p′ + pₑ. The Compton's experiment screen measures the scattered X-ray spectrum with a crystal spectrometer, with an unshifted and a shifted peak; record readings at several angles and plot Δλ against (1 − cos θ) to find the Compton wavelength and the Planck constant.

Lesson: Wave–particle duality: Compton scattering

What it shows

In 1923 Arthur Compton found that X-rays scattered by graphite contain a second, longer wavelength. He explained it by treating the X-rays as photons, each with energy E = hc/λ and momentum p = h/λ, bouncing off free electrons like billiard balls. Conservation of energy and momentum gives λ′ − λ = (h/mₑc)(1 − cos θ), where h/mₑc = 2.43 pm is the Compton wavelength. The shift depends only on the angle, not on the wavelength or the material, so it is large for X-rays and gamma rays but invisible for light. The model treats the electron as free and at rest.

How to use

On Photon–electron collision, set Incident X-ray wavelength λ and drag in the picture or move Scattering angle θ; press Fire photon to watch the collision and Record to add a row to the table. On Compton's experiment, choose the Scattering block and an angle, then drag on the graph or use Spectrometer reading λ′ and its − / + buttons to sit on the shifted peak; press Take reading. Plot Δλ against (1 − cos θ).

Parameters you can change

  • Screen Photon–electron collision, Compton's experiment
  • Incident X-ray wavelength 2–100 pm
  • Scattering angle 0–180 °
  • Scattering block Graphite, Aluminium, Copper
  • Show momentum diagram

Questions to explore

  1. Why is the wavelength shift at 90° the same for every incident wavelength?
  2. At which scattering angle does the recoil electron gain the most kinetic energy, and why?
  3. Why is the Compton shift easy to detect with X-rays but not with visible light?