  We show that harmonic driving of either the magnitude or the phase of the
nearest-neighbor hopping amplitude in a p-wave superconducting wire can
generate modes localized near the ends of the wire. The Floquet eigenvalues of
these modes can either be equal to $\pm 1$ (which is known to occur in other
models) or can lie near other values in complex conjugate pairs which is
unusual; we call the latter anomalous end modes. All the end modes have equal
probabilities of particles and holes. If the amplitude of driving is small, we
observe an interesting bulk-boundary correspondence: the Floquet eigenvalues
and the peaks of the Fourier transform of the end modes lie close to the
Floquet eigenvalues and momenta at which the Floquet eigenvalues of the bulk
system have extrema.
