  We show that every even-denominator fractional quantum Hall (FQH) state
possesses at least two robust, topologically distinct gapless edge phases if
charge conservation is broken at the boundary by coupling to a superconductor.
The new edge phase allows for the possibility of a direct coupling between
electrons and emergent neutral fermions of the FQH state. This can potentially
be experimentally probed through geometric resonances in the tunneling density
of states at the edge, providing a probe of fractionalized, yet electrically
neutral, bulk quasiparticles. Other measurable consequences include a charge
$e$ fractional Josephson effect, a charge $e/4q$ quasiparticle blocking effect
in filling fraction $p/2q$ FQH states, and modified edge electron tunneling
exponents.
