Atomic physics

Experiments you can run yourself.

Radioactive decay — half-life and the formula N = N₀(½)^(t/T)

The law of radioactive decay: why after each half-life one half of the nuclei remains. An interactive simulation, the formula, and C-14 dating.

The atomic model — energy levels and spectrum

The Bohr model of the atom: why an excited electron emits light and where the spectral lines of elements come from. An interactive simulation of energy levels.

The photoelectric effect

Light ejects electrons from a metal only above the threshold frequency f₀=W/h. The kinetic energy E_k=hf−W depends on frequency, while intensity controls only the number of electrons.

The de Broglie wave — matter duality

The greater the particle's momentum, the shorter its matter wave.

Heisenberg's uncertainty principle

The more precisely we know the position, the less precisely we know the momentum.

The Davisson–Germer experiment — matter waves

Electrons produce a diffraction pattern on a crystal — confirming de Broglie waves (Nobel Prize 1937).

The Compton effect — the photon has momentum

The scattered photon has a longer wavelength — proof that light carries momentum (Nobel 1927).

The Franck–Hertz experiment — quantised energy levels

The current dips at evenly spaced voltages — the atom's energy is quantised (Nobel Prize 1925).

Laser cooling of atoms

A photon carries momentum — the right light can slow down and cool atoms (Nobel 1997).

The laser — stimulated emission

Population inversion lets one photon trigger an avalanche of identical photons (Nobel Prize 1964).

Scanning tunnelling microscope STM — seeing atoms

The tunnelling current depends exponentially on the tip–surface distance — which makes it possible to image single atoms (Nobel Prize in Physics 1986).

The Zeeman effect — spectral lines in a magnetic field

When a magnetic field is switched on, an atom's spectral line splits into several closely spaced lines (Nobel Prize in Physics 1902).