Identical particles & statistics

indistinguishability

Indistinguishability is the principle that swapping two identical particles cannot change anything you could ever measure. If you have two electrons and you imagine exchanging their roles, every prediction the theory makes — the probability of finding an electron here, the energy of the atom, the pattern on a screen — must come out exactly the same. Nature offers no experiment that could tell the 'before' from the 'after' of such a swap.

This is stronger than saying the particles look alike. It says the very question 'which electron is which?' has no answer in the world, only in our notation. Quantum theory describes both particles with a single shared wavefunction, and that wavefunction is required to respect the swap. The mathematics enforces this by demanding that exchanging two identical particles leaves all physical quantities — built from the probability density — untouched.

From this modest-sounding requirement flows a sharp consequence. When you exchange two particles, the wavefunction itself is allowed to pick up at most a sign: it either stays exactly the same or flips to its negative. Those two options are not arbitrary; they define bosons and fermions, and they are why the periodic table, the laser, and the white dwarf star all behave as they do. A principle about what we cannot know becomes a principle about how matter is built.

|psi(1,2)|^2 = |psi(2,1)|^2 for any two identical particles

The probability density is unchanged by the swap; only an unobservable sign of the wavefunction is free to differ.

Indistinguishability does not mean the particles are 'merged' or share one location. They are still two particles; what vanishes is any meaningful label saying which one is which.

Also called
principle of indistinguishability不可分辨性全同性