  We calculate the density of states of electron-hole excitations in a
superconductor/normal-metal/superconductor (SNS) junction in graphene, in the
long-junction regime that the superconducting gap is much larger than the
Thouless energy. If the normal region is undoped, the excitation spectrum
consists of neutral modes that propagate along the boundaries - transporting
energy but no charge. These ``Andreev modes'' are a coherent superposition of
electron states from the conduction band and hole states from the valence band,
coupled by specular Andreev reflection at the superconductor. The lowest
Andreev mode has an excitation gap, which depends on the superconducting phase
difference across the SNS graphene channel. At high doping the excitation gap
vanishes and the usual gapless density of states of Andreev levels is
recovered. We use our results to calculate the superconducting phase dependence
of the thermal conductance of the graphene channel.
