The Relative Fermionic Entropy in Two-Dimensional Rindler Spacetime
Felix Finster, Albert Much
TL;DR
This work analyzes fermionic relative entropy in a two‑dimensional Rindler setting via two complementary approaches: modular theory and reduced one‑particle density operators. It derives a general Gaussian‑state relative entropy formula and applies it to both unitary vacuum excitations and non‑unitary Gaussian excitations, demonstrating consistency between the modular and one‑particle methods where their domains overlap. The results yield explicit expressions such as $S(\tilde{\omega}\Vert \omega)=2\pi\langle f|H_{\mathcal{R}}\tanh(2\pi H_{\mathcal{R}})|f\rangle$ (and equivalent Gaussian forms) and show how non‑unitary excitations extend the analysis beyond the reach of modular theory. The work clarifies the relationship between modular flow and one‑particle covariance, highlighting a complementary toolkit for studying entropic quantities in relativistic quantum fields and opening paths to treat more general quasi‑free states and other spacetimes.
Abstract
The fermionic relative entropy in two-dimensional Rindler spacetime is studied using both modular theory and the reduced one-particle density operators. The methods and results are compared. A formula for the relative entropy for general Gaussian states is derived. As an application, the relative entropy is computed for a class of non-unitary excitations.
