Chapter 1
Introductory Quantum Mechanics · Chapter 1

Matter Waves

Chapter 0 ended with patches: energy comes in packets, atoms sit on rungs – but nobody knew why. In 1924 a French PhD student proposed something outrageous: everything is a wave. Electrons included. You included.

Louis de Broglie’s idea sounds like a riddle. Light, which everyone thought was a wave, turned out to also be particles (Chapter 0). So de Broglie asked: what if the reverse is true too? What if particles – electrons, atoms, footballs – are also waves? Each moving thing would carry a wavelength: the faster and heavier it is, the shorter its wave. It sounded absurd. Within three years, experiments proved him right, and it earned him the Nobel Prize. This chapter is about what those matter waves are – and about the experiment Richard Feynman called “the only mystery” of quantum mechanics.

1.1A ridiculous idea: everything has a wavelength

De Broglie’s rule, in plain words: every moving thing carries a wave, and the heavier or faster the thing, the smaller its wave. The waves of everyday objects are absurdly, unmeasurably small – a thrown baseball’s wave is a billion billion times smaller than an atomic nucleus. That’s why the world looks solid and un-wavy: not because quantum mechanics stops applying to big things, but because their waves are far too small to ever notice.

Shrink down to an electron, though – the lightest particle there is – and the wave becomes as big as an atom: impossible to ignore. Explore the scale below.

The de Broglie scale – from electrons to baseballs
FIG. 1.1
atomnucleus1e-361e-321e-281e-241e-201e-161e-121e-8de Broglie wavelength λ (m) – log scalethermal neutronC₆₀ molecule (200 m/s, interfered 1999!)grain of pollen (drifting)baseball (40 m/s)you, walkingelectron
the electron’s wave is about the size of an atom – impossible to ignorea baseball’s wave is unimaginably smaller than anything ever measured
Wavelengths on a log scale. The shaded bands mark the size of an atom and of a nucleus – wave effects appear when λ reaches the scale of the apparatus. Every marker is a real computed value, and C₆₀ interference was actually measured in 1999.

1.2The only mystery: electrons through two slits

Fire electrons – one at a time, with long gaps between them – at a wall with two narrow slits, and record where each lands on a screen behind. Each electron arrives as a single dot: particle. But wait, and the dots organise into stripes – zones where electrons often land, separated by zones where they never do: an , the unmistakable fingerprint of a wave passing through both slits at once. Each electron interferes with itself.

Stranger still: put a detector at the slits to see which one each electron went through, and the stripes vanish. Watching the wave forces it to pick a side. Run the experiment below – and try the detector toggle.

Single-electron double slit (Bach et al. 2013 geometry)
FIG. 1.2
each dot = one electron, arriving one at a timethe stripes are the fingerprint of a waveelectrons so far: 0
Each dot is one electron. The histogram accumulates arrivals; fringes emerge only statistically. Switching the detector on removes the interference term – and resets the screen, since the two situations are different experiments.

1.3Wave packets: building a particle out of waves

A pure wave goes on forever – but a particle is somewhere. The fix: of slightly different wavelengths. They agree in one region (a lump) and cancel everywhere else. That lump – a wave packet – is the closest a wave gets to being a particle.

Watch two speeds in the animation: the little ripples inside the packet move at one speed, while the lump itself moves at another – twice as fast, in fact. The lump is what carries the particle. And notice the packet slowly spreading out: the price of building “somewhere” out of waves is that “somewhere” gets blurrier over time.

Wave packet – phase vs. group velocity, and dispersion
FIG. 1.3
the lump moves twice as fast as the ripples inside itand it slowly spreads out as it travels
Blue: Re ψ (the ripples). Purple: the envelope |ψ|. The red dot rides a crest (phase velocity); the gold dot rides the envelope peak (group velocity – the particle's velocity). Units: ħ = m = 1.

1.4Why Bohr was right: standing waves

Now the payoff. Chapter 0 left a mystery: why is an electron allowed only on certain orbits? De Broglie’s answer: wrap the electron’s wave around its orbit. If a whole number of wavelengths fits the loop, the wave closes on itself and reinforces – a stable , like a guitar string’s note. If not, the wave comes back out of step and cancels itself out. The allowed orbits are simply the ones where the wave fits. Try the slider: only whole numbers work.

De Broglie waves on a Bohr orbit
FIG. 1.4
3 whole waves fit around the loop – the wave reinforces itself: allowed
Integer n: the wave closes on itself – a stationary state (2πr = nλ, i.e. L = nħ). Non-integer n: the wave returns out of phase and destroys itself – no such orbit exists.

1.5Where this leaves us

Particles are waves; waves that fit are the allowed states; and watching a wave changes what it does. But what exactly is waving? Water waves are water; sound waves are air. The electron’s wave, it turns out, is made of something much stranger: complex numbers – numbers with a direction. That’s Chapter 2.

Next chapter
Chapter 2 – The Wavefunction
What is waving? Phasors, the corkscrew wave, and why quantum mechanics cannot live without i.
Chapter 2 of 7