In spite of their simple description in terms of rotations or symplectic transformations in phase space, quadratic Hamiltonians such as those modelling the most common Gaussian operations on bosonic modes remain poorly understood in terms of entropy production. For instance, determining the quantum entropy generated by a Bogoliubov transformation is notably a hard problem, with generally no known analytical solution, while it is vital to the characterisation of quantum communication via bosonic channels. Here we overcome this difficulty by adapting the replica method, a tool borrowed from statistical physics and quantum field theory. We exhibit a first application of this method to continuous-variable quantum information theory, where it enables accessing entropies in an optical parametric amplifier. As an illustration, we determine the entropy generated by amplifying a binary superposition of the vacuum and a Fock state, which yields a surprisingly simple, yet unknown analytical expression.
INTRODUCTIONGaussian transformations are ubiquitous in quantum physics, playing a major role in quantum optics, quantum field theory, solid-state physics or black-hole physics. 1 In particular, the Bogoliubov transformations resulting from Hamiltonians that are quadratic (bilinear) in mode operators are among the most significant Gaussian transformations, well known to model superconductivity 2 but also describing a much wider range of physical situations, from squeezing or amplification in the context of quantum optics 3-6 to Unruh radiation in an accelerating frame 7-9 or even Hawking radiation as emitted by a black hole. [10][11][12] In the present article, we focus on Gaussian bosonic transformations, which are at the heart of so-called Gaussian quantum information theory. 13 These transformations encompass the passive coupling between modes of the electromagnetic field as effected by a beam splitter in bulk optics or an optical coupler in fibre optics, as well as the active transformations resulting from parametric downconversion in a nonlinear optical medium, which are traditionally used as a source of quantum entanglement.Although they are common, quantum Gaussian processes are poorly understood in terms of entropy generation. Indeed, the symplectic formalism in phase-space representation is not suited to calculate von Neumann entropies as this requires diagonalising density operators in state space. 14 When amplifying an optical state using parametric downconversion, for example, the output state suffers from quantum noise, which is an increasing function of the amplification gain. 15 Characterising this noise in terms of entropy is indispensable for determining the capacity of Gaussian bosonic channels. [16][17][18] However, the output entropy is not accessible for an arbitrary input state because it is hard-usually impossible-to diagonalise the corresponding output state in infinite-dimensional Fock space. With the notable exception of