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Home/Electricity & Magnetism/Compton Scattering

Compton Scattering

Compton scattering describes the inelastic collision between a photon and a free, stationary electron, a foundational experiment confirming the particle nature of light. This simulator visualizes the core phenomenon: the increase in the photon's wavelength as it scatters through an angle θ. The process is governed by the Compton scattering formula: Δλ = λ' - λ = (h / (m_e c)) (1 - cos θ), where λ is the initial wavelength, λ' is the scattered wavelength, h is Planck's constant, m_e is the electron rest mass, and c is the speed of light. The constant h/(m_e c) is the Compton wavelength of the electron (λ_C ≈ 2.426 pm), a key scale for the effect. The model calculates and displays the wavelength shift and the corresponding energy loss of the photon (E = hc/λ) as the scattering angle changes. It simplifies the real-world scenario by assuming the target electron is initially at rest and unbound, neglecting binding energies and Doppler effects. It also typically ignores the possibility of multiple scatterings or relativistic corrections for the electron's recoil beyond the standard formula. By interacting with the simulator, students can explore the direct relationship between scattering angle and wavelength shift, observe that the shift is maximal at 180° (backscattering) and zero at 0°, and solidify their understanding of photon momentum (p = h/λ) and energy conservation in particle-like interactions.

Who it's for: Undergraduate physics students in modern physics, quantum mechanics, or electromagnetism courses studying the photon model of light and particle-wave duality.

Key terms

  • Compton Scattering
  • Photon
  • Wavelength Shift
  • Compton Wavelength
  • Inelastic Scattering
  • Planck's Constant
  • Electron Recoil
  • Conservation of Momentum

Incoming X-ray or γ-ray (λ) scatters through angle θ; the outgoing photon is redder. Try θ = 180° for maximum shift (backscatter).

Before
2.40 pm
→
After
4.83 pm

Live graphs

Photons

2.4 pm
90°

λ′ − λ = (h/m_e c)(1 − cos θ) with h/m_e c ≈ 2.426 pm (Compton wavelength of electron). Energy is transferred to the recoiling electron (not shown in detail).

Measured values

Δλ2.4263 pm
λ′4.8263 pm

How it works

Elastic scattering on quasi-free electrons; at high energy the wavelength shift is a clean test of photon momentum.

Key equations

λ′ − λ = λ_C (1 − cos θ), λ_C ≈ 2.426 pm

Frequently asked questions

Why does the photon lose energy during Compton scattering?
The photon transfers some of its energy and momentum to the recoiling electron to conserve both quantities in the collision. Since the photon's energy is inversely proportional to its wavelength (E = hc/λ), this energy loss results in an increase, or shift, in its wavelength. The greater the scattering angle, the greater the energy transfer and thus the larger the wavelength shift.
Is the electron really 'free and at rest' in a real material?
This is a key simplification of the basic model. In actual experiments with atomic targets, electrons are bound with varying energies. For photons with energy much greater than the electron's binding energy (e.g., X-rays or gamma rays), the approximation is excellent. For lower-energy photons, the binding energy cannot be ignored, leading to more complex 'incoherent' or bound-electron scattering.
What is the significance of the Compton wavelength (λ_C)?
The Compton wavelength (λ_C = h/(m_e c) ≈ 2.43 pm) sets the natural scale for the scattering effect. It represents the maximum possible wavelength shift, which occurs when the photon is backscattered (θ = 180°). It is a fundamental constant combining quantum mechanics (h), relativity (c), and the property of a specific particle (m_e).
How does Compton scattering prove light is made of particles?
The classical wave theory of light cannot explain the wavelength shift's dependence on angle or the existence of a scattered electron. The successful derivation of the Compton formula requires treating the photon as a discrete particle with energy E = hf and momentum p = h/λ, which collides with an electron like a billiard ball, conserving energy and momentum. The precise agreement with experiment was pivotal evidence for the photon concept.