The anomalous scaling behavior of the topological susceptibility Οtβ in
two-dimensional CPNβ1 sigma models for Nβ€3 is studied using the
overlap Dirac operator construction of the lattice topological charge density.
The divergence of Οtβ in these models is traced to the presence of small
instantons with a radius of order a (= lattice spacing), which are directly
observed on the lattice. The observation of these small instantons provides
detailed confirmation of L\"{u}scher's argument that such short-distance
excitations, with quantized topological charge, should be the dominant
topological fluctuations in CP1 and CP2, leading to a divergent
topological susceptibility in the continuum limit. For the \CP models with
N>3 the topological susceptibility is observed to scale properly with the
mass gap. These larger N models are not dominated by instantons, but rather
by coherent, one-dimensional regions of topological charge which can be
interpreted as domain wall or Wilson line excitations and are analogous to
D-brane or ``Wilson bag'' excitations in QCD. In Lorentz gauge, the small
instantons and Wilson line excitations can be described, respectively, in terms
of poles and cuts of an analytic gauge potential.Comment: 33 pages, 12 figure