Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1854634 | Annals of Physics | 2014 | 10 Pages |
•The spin–statistics theorem is not required for particles on a lattice.•Spin emerges dynamically when spinless fermions have a relativistic continuum limit.•Graphene and staggered fermions are examples of this phenomenon.•The phenomenon is intimately tied to chiral symmetry and fermion doubling.•Anomaly cancellation is a crucial feature of any valid lattice fermion action.
Quantum mechanics and relativity in the continuum imply the well known spin–statistics connection. However for particles hopping on a lattice, there is no such constraint. If a lattice model yields a relativistic field theory in a continuum limit, this constraint must “emerge” for physical excitations. We discuss a few models where a spin-less fermion hopping on a lattice gives excitations which satisfy the continuum Dirac equation. This includes such well known systems such as graphene and staggered fermions.