  There is a close connection between the ground state of non-interacting
fermions in a box with classical (absorbing, reflecting, and periodic) boundary
conditions and the eigenvalue statistics of the classical compact groups. The
associated determinantal point processes can be extended in two natural
directions: i) we consider the full family of admissible quantum boundary
conditions (i.e., self-adjoint extensions) for the Laplacian on a bounded
interval, and the corresponding projection correlation kernels; ii) we
construct the grand canonical extensions at finite temperature of the
projection kernels, interpolating from Poisson to random matrix eigenvalue
statistics. The scaling limits in the bulk and at the edges are studied in a
unified framework, and the question of universality is addressed. Whether the
finite temperature determinantal processes correspond to the eigenvalue
statistics of some matrix models is, a priori, not obvious. We complete the
picture by constructing a finite temperature extension of the Haar measure on
the classical compact groups. The eigenvalue statistics of the resulting grand
canonical matrix models (of random size) corresponds exactly to the grand
canonical measure of non-interacting free fermions with classical boundary
conditions.
