Compton Effect
The Compton Effect is experimental proof that photons carry momentum. When X-rays scatter off electrons, the scattered photons have longer wavelengths than the incident photons — a result that classical wave theory cannot explain.
The Experiment (1923)
Arthur Compton fired X-rays at a target and measured the scattered radiation.
What He Observed
- Some X-rays scattered with the same wavelength
- Some X-rays scattered with longer wavelength
- The wavelength shift depended on the scattering angle
Classical wave theory predicted no wavelength change — only particle collision with momentum transfer explains this.
What Happens
Before Collision
- Photon: moving with momentum $p = \frac{h}{\lambda}$
- Electron: nearly at rest
During Collision
- Photon strikes electron
- Momentum is transferred
After Collision
- Electron: recoils with kinetic energy
- Photon: scatters with lower momentum → longer wavelength
The Compton Shift Formula
$$\Delta \lambda = \lambda' - \lambda = \frac{h}{m_e c}(1 - \cos \theta)$$
Where:
| Symbol | Meaning | Value |
|---|---|---|
| $\Delta \lambda$ | Wavelength shift | — |
| $\lambda'$ | Scattered photon wavelength | — |
| $\lambda$ | Incident photon wavelength | — |
| $h$ | Planck's constant | $6.63 \times 10^{-34}$ J·s |
| $m_e$ | Electron mass | $9.11 \times 10^{-31}$ kg |
| $c$ | Speed of light | $3.0 \times 10^8$ m/s |
| $\theta$ | Scattering angle | — |
Compton Wavelength of Electron
$$\frac{h}{m_e c} = 2.43 \times 10^{-12} \text{ m}$$
Key Insights
Maximum Shift
Maximum wavelength increase occurs at $\theta = 180°$ (backscattering): $$\Delta \lambda_{max} = \frac{2h}{m_e c} = 4.86 \times 10^{-12} \text{ m}$$
No Shift at Zero Angle
At $\theta = 0°$: $\cos 0° = 1$, so $\Delta \lambda = 0$
Why Classical Theory Fails
- Classical wave theory: scattering doesn't change wavelength
- Only particle collision with momentum conservation explains the shift
Example Calculation
Problem: X-rays with $\lambda = 1.0 \times 10^{-11}$ m scatter at $\theta = 90°$. Find $\lambda'$.
Solution: $$\Delta \lambda = \frac{h}{m_e c}(1 - \cos 90°) = 2.43 \times 10^{-12} \times (1 - 0) = 2.43 \times 10^{-12} \text{ m}$$
$$\lambda' = \lambda + \Delta \lambda = 1.0 \times 10^{-11} + 2.43 \times 10^{-12} = 1.243 \times 10^{-11} \text{ m}$$
Related
- Concept: Photon Momentum — The underlying principle
- Concept: Wave-Particle Duality
- FAD1022 Lecture 45 — Photon Momentum, Compton Effect, de-Broglie Waves & Heisenberg Uncertainty
- Rapid-Fire Drill Pack — Modern Physics Wave-Particle Duality