Published by Patrick Mutisya · 14 days ago
At the turn of the 20th century it became clear that light and matter cannot be described solely as particles or solely as waves. The concept of wave‑particle duality states that every quantum entity exhibits both wave‑like and particle‑like properties, the dominant behaviour depending on the experimental arrangement.
Louis de Broglie proposed that any particle with momentum \$p\$ has an associated wavelength \$\lambda\$ given by
\$\lambda = \frac{h}{p}\$
where \$h\$ is Planck’s constant. For an electron of kinetic energy \$K\$ (non‑relativistic), \$p = \sqrt{2m_e K}\$, so
\$\lambda = \frac{h}{\sqrt{2m_e K}}\$
This wavelength is typically of the order of a few picometres for electrons accelerated through a few hundred volts – comparable to inter‑atomic spacings in crystals, making diffraction observable.
Electrons were accelerated through a potential \$V\$, giving them kinetic energy \$eV\$ and wavelength \$\lambda = h/\sqrt{2m_e eV}\$. The beam struck a nickel crystal and the intensity of scattered electrons was measured as a function of angle \$\theta\$.
Key observations:
\$2d\sin\theta = n\lambda\$
where \$d\$ is the spacing between crystal planes and \$n\$ is an integer.
In modern surface‑science labs, electrons of 20–200 e \cdot are directed onto a crystalline surface. The resulting diffraction pattern is recorded on a phosphor screen.
The pattern consists of a set of bright spots whose positions are related to the reciprocal lattice of the surface, exactly as predicted for wave diffraction.
When electrons are treated as particles, we would expect a smooth angular distribution determined only by classical scattering (Rutherford‑type). The appearance of discrete, angle‑dependent intensity maxima is inexplicable in a purely particle picture.
In the wave picture:
Thus the experiment directly demonstrates that electrons possess a wavelength and interfere, satisfying the wave description.
| Aspect | Particle Model | Wave Model (Observed) |
|---|---|---|
| Scattering distribution | Continuous, isotropic (except for geometric factors) | Discrete peaks at specific angles |
| Dependence on crystal spacing \$d\$ | No dependence | Peak angles satisfy \$2d\sin\theta = n\lambda\$ |
| Effect of electron energy | Higher energy → more forward scattering | Higher energy → shorter \$\lambda\$, peaks shift according to Bragg law |
| Interpretation of intensity pattern | Random collisions | Interference of coherent wavefronts |