Discrete spacetime, quantum walks and relativistic wave equations

TL;DR

This paper demonstrates how symmetric 3D quantum walks on a lattice naturally lead to relativistic wave equations, incorporating antimatter and Lorentz invariance, and discusses potential experimental distinctions from the Dirac equation.

Contribution

It shows that symmetry constraints on 3D quantum walks imply Lorentz invariance and the inclusion of antimatter, providing a discrete model for relativistic quantum particles.

Findings

Quantum walks on cubic lattices can produce relativistic wave equations in the continuum limit.

Symmetry requirements lead to Lorentz invariance and the necessity of a four-dimensional internal space.

The paper discusses possible experimental tests to distinguish discrete walks from continuum Dirac dynamics.

Abstract

It has been observed that quantum walks on regular lattices can give rise to wave equations for relativistic particles in the continuum limit. In this paper we define the 3D walk as a product of three coined one-dimensional walks. The factor corresponding to each one-dimensional walk involves two projection operators that act on an internal coin space, each projector is associated with either the "forward" or "backward" direction in that physical dimension. We show that the simple requirement that there is no preferred axis or direction along an axis---that is, that the walk be symmetric under parity transformations and rotations that swap the axes of the cubic lattice---leads to the requirement that the continuum limit of the walk is fully Lorentz invariant. We show further that, in the case of a massive particle, this simple symmetry requirement necessitates that inclusion of antimatter---the use of a four-dimensional internal space---and that the "coin flip" operation is generated by the parity transformation on the internal coin space, while the differences of the projection operators associated to each dimension must all anticommute. Finally, we discuss the leading correction to the continuum limit, and the possibility of distinguishing through experiment between the discrete random walk and the continuum-based Dirac equation as a description of fermion dynamics.