  The derivation of mean-field limits for quantum systems at zero temperature
has attracted many researchers in the last decades. Recent developments are the
consideration of pair correlations in the effective description, which lead to
a much more precise description of both spectral properties and the dynamics of
the Bose gas in the weak coupling limit. While mean-field results typically
lead to convergence for the reduced density matrix only, one obtains norm
convergence when considering the pair correlations proposed by Bogoliubov in
his seminal 1947 paper. In this article we consider an interacting Bose gas in
the case where both the volume and the density of the gas tend to infinity
simultaneously. We assume that the coupling constant is such that the
self-interaction of the fluctuations is of leading order, which leads to a
finite (non-zero) speed of sound in the gas. In our first main result we show
that the difference between the N-body and the Bogoliubov description is small
in $L^2$ as the density of the gas tends to infinity and the volume does not
grow too fast. This describes the dynamics of delocalized excitations of the
order of the volume. In our second main result we consider an interacting Bose
gas near the ground state with a macroscopic localized excitation of order of
the density. We prove that the microscopic dynamics of the excitation coming
from the N-body Schr\"odinger equation converges to an effective dynamics which
is free evolution with the Bogoliubov dispersion relation. The main technical
novelty are estimates for all moments of the number of particles outside the
condensate for large volume, and in particular control of the tails of their
distribution.
