  When mass-deformed ABJM theory is considered on S(3), the partition function
of the theory localises and is given by a matrix model. We solve this model at
large-N in the decompactification limit, where the radius of the three-sphere
is taken to infinity. In this limit, the theory exhibits a rich phase structure
with an infinite number of third-order quantum phase transitions accumulating
at strong coupling.

High Energy Physics - Theory