  The abelian-projected monopole loop distribution is extracted from maximal
abelian gauge simulations. The number of loops of a given length falls as a
power of the length nearly independent of lattice size. This power increases
with $\beta=4/g^2$, reaching five around $\beta=2.85$, beyond which loops any
finite fraction of the lattice size vanish in the infinite lattice limit,
suggesting the continuum theory lacks confinement.
