  We address the issue of how triplet superconductivity emerges in an
electronic system near a ferromagnetic quantum critical point (FQCP). Previous
studies found that the superconducting transition is of second order, and Tc is
strongly reduced near the FQCP due to pair-breaking effects from thermal spin
fluctuations. In contrast, we demonstrate that near the FQCP, the system avoids
pair-breaking effects by undergoing a first order transition at a much larger
Tc. A second order superconducting transition emerges only at some distance
from the FQCP.
