Generalized causal set d’Alembertians
Siavash Aslanbeigi (Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo, ON, N2L 2Y5, Canada, Department of Physics and Astronomy, University of Waterloo, Waterloo, ON, N2L 3G1, Canada); Mehdi Saravani (Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo, ON, N2L 2Y5, Canada, Department of Physics and Astronomy, University of Waterloo, Waterloo, ON, N2L 3G1, Canada); Rafael D. Sorkin (Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo, ON, N2L 2Y5, Canada, Department of Physics and Astronomy, University of Waterloo, Waterloo, ON, N2L 3G1, Canada, Raman Research Institute, C.V.Raman Avenue, Sadashivanagar, Bangalore 560 080, India, Department of Physics, Syracuse University, Syracuse, NY 13244-1130, U.S.A.)
We introduce a family of generalized d’Alembertian operators in D -dimensional Minkowski spacetimes $ {\mathbb M} $ D which are manifestly Lorentz-invariant, retarded, and non-local, the extent of the nonlocality being governed by a single parameter ρ . The prototypes of these operators arose in earlier work as averages of matrix operators meant to describe the propagation of a scalar field in a causal set. We generalize the original definitions to produce an infinite family of “Generalized Causet Box (GCB) operators” parametrized by certain coefficients { a , b n }, and we derive the conditions on the latter needed for the usual d’Alembertian to be recovered in the infrared limit. The continuum average of a GCB operator is an integral operator in $ {\mathbb M} $ D , and it is these continuum operators that we mainly study. To that end, we compute their action on plane waves, or equivalently their Fourier transforms g ( p ) [ p being the momentum-vector]. For timelike p , g ( p ) has an imaginary part whose sign depends on whether p is past or future-directed. For small p , g ( p ) is necessarily proportional to p · p , but for large p it becomes constant, raising the possibility of a genuinely Lorentzian perturbative regulator for quantum field theory in $ {\mathbb M} $ D . We also address the question of whether or not the evolution defined by the GCB operators is stable, finding evidence that the original 4D causal set d’Alembertian is unstable, while its 2D counterpart is stable.
