The Information in a Wave

Abstract

We provide the notion of entropy for a classical Klein–Gordon real wave, that we derive as particular case of a notion entropy for a vector in a Hilbert space with respect to a real linear subspace. We then consider a localised automorphism on the Rindler spacetime, in the context of a free neutral Quantum Field Theory, that is associated with a second quantised wave, and we explicitly compute its entropy S, that turns out to be given by the entropy of the associated classical wave. Here S is defined as the relative entropy between the Rindler vacuum state and the corresponding sector state (coherent state). By ${\lambda }$-translating the Rindler spacetime into itself along the upper null horizon, we study the behaviour of the corresponding entropy $S({\lambda })$. In particular, we show that the QNEC inequality in the form $\frac{d^2}{d{\lambda }^2}S({\lambda })\ge 0$ holds true for coherent states, because $\frac{d^2}{d{\lambda }^2}S({\lambda })$ is the integral along the space horizon of a manifestly non-negative quantity, the component of the stress-energy tensor in the null upper horizon direction.