Volume 27 · Part Three · Chapter 12 of 19
Braided Statistics and Worldlines
The one setting where braiding is literally the operation performed.
Why two dimensions changes the question
Exchange two identical particles in three dimensions and the paths by which you did it are all deformable into one another; only the endpoint matters, and the state can pick up at most a sign — bosons or fermions. In two dimensions paths that wind around one another cannot be deformed into paths that do not. The relevant group is the braid group rather than the permutation group, and the state may acquire an arbitrary phase, or, if the ground state is degenerate, may be rotated within that degenerate space by a matrix.
Those are anyons: abelian if the exchange multiplies by a phase, non-abelian if it applies a matrix that does not commute with other exchanges. In the non-abelian case the worldlines' braid — the actual history of crossings in spacetime — is the computation. This is the standard against which every looser use of 'braid' in this volume is measured.
Where the evidence stands
Anyonic statistics in the fractional quantum Hall regime have been observed in interferometry and in collision experiments, and abelian anyonic phases are now reasonably well established. Non-abelian braiding is the harder claim; results in quantum-Hall systems and in engineered superconducting devices are suggestive, contested, and in some cases have been withdrawn. A chapter written in 2026 should say partial and recent rather than demonstrated.
Equations borrowed
- Braid group statistics in 2+1 dimensions
- Non-abelian anyons and topological quantum computation (Nayak et al., 2008)
- Fractional quantum Hall interferometry results
Validity band
Two-dimensional systems with a gapped, degenerate ground-state manifold at low temperature. Not a statement about particles in three dimensions.
Falsifier
A well-controlled braiding experiment in a candidate non-abelian phase returning results independent of exchange order would falsify the non-abelian claim.
Where this chapter is weakest
The chapter carries the load for the whole of Part Three: it is the one place where braiding is literal, and the volume leans on it. If the non-abelian experimental record weakens further, the figure elsewhere in the book loses its anchor and must be labelled as figure throughout.
The volume-wide audit of these weak points is collected in Where This Volume Is Weak.