Chapter 1
Relativistic Quantum Mechanics · Chapter 1

The Wrong Equation

Feed relativity's energy–momentum relation to the quantum recipe and out comes the Klein–Gordon equation – along with two diseases nobody ordered: energies with no floor, and probabilities that go negative. The first honest attempt fails, and the exact ways it fails write the specification for what must come next.

The plan from Chapter 0 was simple: rebuild the quantum equation on relativity’s correct relation between energy and motion. Doing it gives a real, named equation – the Klein–Gordon equation – and it is not exactly wrong. It describes genuine particles. But taken as a theory of a single electron, the way the quantum course took the Schrödinger equation, it comes down with two diseases at once. Both are worth catching, because the cure for them is the equation that finally succeeds.

1.1The square-root problem

The relativistic energy is a square root: E=(pc)2+(mc2)2E = \sqrt{(pc)^2 + (mc^2)^2}. To build a wave equation you have to feed that expression the quantum recipe, which turns momentum into an instruction to measure how the wave bends in space. But the square root of such an instruction is a monster – loosely, you are being asked for the square root of “wiggliness,” and there is no clean way to take it. So the obvious dodge is to get rid of the root by squaring everything first, and work with E2E^2 instead of EE.

1.2The equation with two roots

Squaring to dodge the square root came at a price. A square has two roots – (−3)2(-3)^2 and 323^2 are both 99 – so the squared equation quietly describes not just the ordinary positive energies but a whole mirror set of negative ones, a bottomless basement below zero. In classical physics you could shrug and ignore states you never start in. In quantum physics you cannot: anything that can happen eventually does. A particle could tumble down the basement stairs forever, releasing more and more energy with no floor to land on.

That is not a small blemish – it is the same catastrophe, one storey down, that the quantum course showed doomed the classical atom, where an electron should have spiralled into the nucleus radiating endlessly. Use the button in the figure to send a particle cascading down the negative branch and watch the energy it pours out never stop.

The equation with two roots
FIG. 1.1
the upper curve is ordinary energy; the lower curve is its unwanted mirror twin, separated by a forbidden gap of two rest energies. Squaring the equation let the twin in – and nothing in the theory stops a particle falling onto it, forever.
Relativity's energy–momentum relation E² = (pc)² + (mc²)² has two square roots, and the Klein–Gordon equation inherits both. Slide the mass toward zero and the branches hug the light cone – a photon is the massless limit. The Schrödinger overlay shows the parabola m + p²/2m kissing the true curve at low momentum: the quantum course lived entirely in that corner. The cascade shows why the negative branch cannot just be ignored: with anything to couple to, a state can step down the bottomless ladder and radiate at every step.

1.3Probability goes negative

The second disease is, if anything, worse. All of quantum mechanics rests on probabilities, and a probability can never be negative – there is no such thing as a −30%-30\% chance of finding the electron in a box. Yet the Klein–Gordon equation’s natural “probability meter” can swing below zero. A quantity that goes negative is not measuring a probability at all, and without a probability the equation has no way to say where the particle is likely to be – which was the entire job.

1.4Where this leaves us

Two dragons, then: bottomless negative energies, and probabilities that turn negative. Dirac’s insight was to trace the second dragon to its lair – the equation’s two time-derivatives – and to demand an equation with only one, like Schrödinger’s. But relativity will not let him treat time more gently than space. An equation first order in time must be first order in space too, and that innocent-sounding requirement turns out to be impossible with ordinary numbers. What Dirac paid to satisfy it anyway is the next chapter.

Next chapter
Chapter 2 – Dirac's Gamble
Demand first order in time and space, and the coefficients can't be numbers – they must anticommute. The smallest things that do it are 4×4 matrices.
Chapter 2 of 7