Wave-Particle Duality

Light behaves like a wave — until it doesn't. Black body radiation, the photoelectric effect, and the Compton effect all forced physicists to accept that light comes in discrete packets called photons. Then de Broglie flipped the idea around: if waves can act like particles, maybe particles can act like waves too.

Act 1 · Black Body Radiation & Planck's Quantum Hypothesis

A hot object glows across a spread of wavelengths, and classical physics couldn't explain the curve

Every heated body radiates energy over a range of wavelengths, peaking at one dominant wavelength that shifts as temperature rises (hotter objects glow bluer). Classical wave theory predicted infinite energy at short wavelengths — the "ultraviolet catastrophe." Planck fixed this by proposing that atoms emit and absorb energy only in discrete packets, E = nhf, not continuously.

wavelength λ intensity visible peak: orange-red glow
λmax = b/T = 0 nm · (Wien's Law, b = 2.898×10⁻³ m·K)
Temperature, T3000 K
Hotter bodies shift the peak to shorter (bluer) wavelengths.

Planck's quantum idea explained the glow of a hot body — Einstein used the same idea to explain why light knocks electrons out of a metal.

Act 2 · The Photoelectric Effect

Light knocks electrons out of a metal — but only above a threshold frequency

Shining light on a metal plate can eject electrons, but only if each photon carries enough energy hf to overcome the metal's work function W. Below the threshold frequency, no electrons escape no matter how intense the light. Above it, each ejected electron carries maximum kinetic energy KEmax = hf − W, and a stopping voltage can just halt the fastest ones.

metal plate collector A
KEmax = hf − W = 0 eV · stopping voltage Vs = 0 V
frequency, f KEmax
Light frequency, f7.5×10¹⁴ Hz
Work function, W2.3 eV
Different metals have different work functions.

A photon doesn't just carry energy — it also carries momentum, and can bounce off an electron like a billiard ball.

Act 3 · The Compton Effect

A photon scattering off an electron loses energy and comes out with a longer wavelength

When an X-ray photon collides with a loosely bound electron, momentum and energy are conserved just like a billiard-ball collision. The scattered photon emerges with less energy — hence a longer wavelength — by an amount that depends only on the scattering angle θ, confirming that photons carry momentum p = h/λ.

incident photon λ scattered λ' recoil electron scattering angle θ measured from the incident direction
Δλ = (h/mec)(1 − cosθ) = 0 pm
Scattering angle, θ60°
At θ=0° there's no collision at all; the shift is greatest at θ=180° (photon bounces straight back).

If light-waves can behave as particles, de Broglie asked: could particles like electrons behave as waves?

Act 4 · De Broglie's Matter Waves

Every moving particle has a wavelength, λ = h/p

De Broglie proposed that any moving mass has an associated wavelength λ = h/(mv), just as a photon does. For everyday objects this wavelength is immeasurably small, but for electrons it's comparable to atomic spacing — enabling electron microscopes to resolve details far finer than any light microscope, since resolution improves as wavelength shrinks.

de Broglie wave accompanying a moving electron shorter λ (higher speed / mass) packs more crests into the same distance
λ = h/(mv) = 0 pm
Speed, v2.0×10⁶ m/s
Particleelectron
Toggle between an electron and a much heavier proton — same speed, very different wavelength.

In the electron microscope, a beam of fast electrons has a de Broglie wavelength thousands of times shorter than visible light, letting it image structures like viruses that light microscopes cannot resolve.

In a nutshell
  • Black body radiation: Planck's hypothesis — energy is emitted/absorbed only in packets E = nhf; λmaxT = constant (Wien's law).
  • Photoelectric effect: KEmax = hf − W; no emission below the threshold frequency regardless of intensity.
  • Compton effect: Δλ = (h/mec)(1−cosθ) — direct proof that photons carry momentum p = h/λ.
  • De Broglie wavelength: λ = h/(mv) — matter has wave properties too, exploited in the electron microscope.