  With the advent of spatially resolved fluorescence imaging in quantum gas
microscopes, it is now possible to directly image glassy phases and probe the
local effects of disorder in a highly controllable setup. Here we present
numerical calculations using a spatially-resolved local mean-field theory, show
that it captures the essential physics of the disordered system and use it to
simulate the density distributions seen in single-shot fluorescence microscopy.
From these simulated images we extract local properties of the phases which are
measurable by a quantum gas microscope and show that unambiguous detection of
the Bose glass is possible. In particular, we show that experimental
determination of the Edwards-Anderson order parameter is possible in a strongly
correlated quantum system using existing experiments. We also suggest
modifications to the experiments which will allow further properties of the
Bose glass to be measured.
