In this paper, a delocalization-localization transition within a supercondu
cting state is explored. The symmetries of the Bogoliubov deGennes Hamilton
ian endow the two associated superconducting phases-the thermal metal and t
he thermal insulator-and the critical point between them, with properties t
hat are in stark contrast with analogous phases in normal systems. Here, fo
r systems preserving spin-rotational invariance and time-reversal symmetry
in three dimensions, the transition is shown to be of a different universal
ity class from its normal partner by extracting and comparing the localizat
ion length exponent. The density of states, which may be regarded as the "o
rder parameter" for the field theory describing the superconducting system,
is studied for its unusual properties about criticality.