Abstract
Using the theory of generalized hydrodynamics (GHD), we derive exact
Euler-scale dynamical two-point correlation functions of conserved
densities and currents in inhomogeneous, non-stationary states of
many-body integrable systems with weak space-time variations. This
extends previous works to inhomogeneous and non-stationary situations.
Using GHD projection operators, we further derive formulae for
Euler-scale two-point functions of arbitrary local fields, purely from
the data of their homogeneous one-point functions. These are new also in
homogeneous generalized Gibbs ensembles. The technique is based on
combining a fluctuation-dissipation principle along with the exact
solution by characteristics of GHD, and gives a recursive procedure able
to generate nn-point
correlation functions. Owing to the universality of GHD, the results are
expected to apply to quantum and classical integrable field theory such
as the sinh-Gordon model and the Lieb-Liniger model, spin chains such as
the XXZ and Hubbard models, and solvable classical gases such as the
hard rod gas and soliton gases. In particular, we find
Leclair-Mussardo-type infinite form-factor series in integrable quantum
field theory, and exact Euler-scale two-point functions of exponential
fields in the sinh-Gordon model and of powers of the density field in
the Lieb-Liniger model. We also analyse correlations in the partitioning
protocol, extract large-time asymptotics, and, in free models, derive
all Euler-scale nn-point
functions.
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