As the other answer stated, the answer to both questions is yes. A superfluid can be understood from a macroscopic perspective as a fluid with zero viscosity, or from a microscopic perspective as an ensemble of interacting particles that form a condensate. This means the number of particles in the quantum ground state (the lowest energy state) has become a finite fraction of the total number of particles. This is in contrast with most systems, where the number of particles in the ground state is vanishingly small. When people talk about the superfluid and normal fluid fractions, they are conceptually dividing the system into a mixture of two fluids. The superfluid component is the subset of particles in the ground state, and the normal fluid component is all other particles. Only the superfluid component has the special property of zero viscosity, though there are caveats to this claim when one considers the role of defects like vortices.
The reason why the ratio of the components changes with temperature is simply because reducing the temperature means lowering the average energy of particles by definition. This means the fraction of particles in the lowest energy state increases. Eventually, at T=0 (not that you can actually reach this limit), the superfluid fraction becomes 100% and the viscosity essentially approaches zero.
I could go on to talk about superfluid 3He, but this answer is too long already.
Reference: "Superconductivity, Superfluids, and Condensates" by James F Annett.