The density of Andreev levels in a normal metal (N) in contact with two
superconductors (S) is known to exhibit an induced minigap related to the
inverse dwell time. We predict a small secondary gap just below the
superconducting gap edge---a feature that has been overlooked so far in
numerous studies of the density of states in S−N−S structures. In a generic
structure with N being a chaotic cavity, the secondary gap is the widest at
zero phase bias. It closes at some finite phase bias, forming the shape of a
"smile". Asymmetric couplings give even richer gap structures near the phase
difference \pi. All the features found should be amendable to experimental
detection in high-resolution low-temperature tunneling spectroscopy.Comment: 5 pages, 4 figure