  Vortices in thin-film superconductors are often modelled as a system of
particles interacting via a repulsive logarithmic potential. Arguments are
presented to show that the hypothetical (Abrikosov) crystalline state for such
particles is unstable at any finite temperature against proliferation of
screened disclinations. The correlation length of crystalline order is
predicted to grow as $\sqrt{1/T}$ as the temperature $T$ is reduced to zero, in
excellent agreement with our simulations of this two-dimensional system.
