theorem

spin–statistics theorem

The spin-statistics theorem links a particle's spin to its quantum statistics, distinguishing fermions from bosons.
29 related articles · 1 formulas · 1 who worked here

Description

In the quantum world, particles are divided into unsociable individualists and sociable party-goers — that's what the spin–statistics theorem states. A particle's character is rigidly tied to its spin: half-integer spin — 'don't like neighbors' (fermions, like electrons), integer spin — 'the more the merrier' (bosons, like photons).

History

Wolfgang Pauli (1940) played a key role in the proof, building on earlier work by Markus Fierz (1939). Pauli showed that without accounting for the spin–statistics connection, quantum electrodynamics would give negative probabilities and causality violation. Later, the generality of the theorem was confirmed by Lüders and Zumino (1958) within the framework of axiomatic field theory.

How it works

In practice, the theorem determines which fields can be used to describe matter (fermionic Dirac fields) and force carriers (bosonic gauge fields). It underlies all quantum statistics, from atomic structure to early universe cosmology. Limits of applicability: strictly holds in 3+1-dimensional spacetime for free particles and under the condition of Lorentz invariance.

Fun fact

If electrons were bosons, all atoms would collapse into uniform lumps, and the Periodic Table would disappear.

Concept graph →

Formulas

$$\mathrm{Bi} = \frac{\sigma_y}{\sigma_{\text{prop}}}$$
Bingham number compares yield stress to propulsion stress.
What is in the formula
BivariableBingham number — bingham number
σ_yvariableYield stress of the material — yield stress pascal
σ_propvariableCharacteristic propulsion stress — propulsion stress pascal
{bi}=\frac{σ_y}{σ_{{prop}}} · 2607.10734

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