Metric-induced non-Hermitian physics

I consider the longstanding issue of the hermiticity of the Dirac equation in curved spacetime. Instead of imposing hermiticity by adding ad hoc terms, I renormalize the field by a scaling function, which is related to the determinant of the metric, and then regularize the renormalized field on a discrete lattice. I found that, for time-independent and diagonal (or conformally flat) coordinates, the Dirac equation returns a pseudo-Hermitian (i.e., \mathcal{PT} ???? ???? -symmetric) Hamiltonian when properly regularized on the lattice. Notably, the \mathcal{PT} ???? ???? -symmetry is unbroken, ensuring a real energy spectrum and unitary time evolution. This establishes stringent conditions for the existence of complex spectra in non-Hermitian models in one dimension. Conversely, time-dependent spacetime coordinates break pseudohermiticity, yielding non-Hermitian Hamiltonians with nonunitary time evolution. Similarly, space-dependent spacetime coordinates lead to the non-Hermitian skin effect, i.e., the accumulation of localized states on the boundaries. Arguably, these non-Hermitian effects are physical: time dependence leads to local gain and loss processes and nonunitary growth or decay. Conversely, space dependence leads to the non-Hermitian skin effect with spatial decay of the fields in a preferential direction. In other words, the curvature gradients induce an imaginary gauge field on the lattice, corresponding to a drift force acting in space and time, pushing the eigenmodes to the boundaries or forcing their probability density to increase or decrease over time. Hence, temporal curvature gradients produce nonunitary gain or loss, while spatial curvature gradients correspond to the non-Hermitian skin effect, allowing for the description of these two phenomena in a unified framework. This also suggests a duality between non-Hermitian physics and spacetime deformations, framing non-Hermitian physics in purely geometric terms. This metric-induced nonhermiticity unveils an unexpected connection between the spacetime metric and non-Hermitian phases of matter.