We investigate the color-spin locked (CSL) phase of spin-one color-
superconducting quark matter using a truncated Dyson-Schwinger equation for the
quark propagator in Landau gauge. Starting from the most general parity
conserving ansatz allowed by the CSL symmetry, the Dyson-Schwinger equation is
solved self-consistently and dispersion relations are discussed. We find that
chiral symmetry is spontaneously broken due to terms which have previously been
neglected. As a consequence, the excitation spectrum contains only gapped modes
even for massless quarks. Moreover, at moderate chemical potentials the
quasiparticle pairing gaps are several times larger than expected from
extrapolated weak-coupling results.Comment: 9 pages, 7 figure