Center vortices, nexuses, and fractional topological charge - art. no. 085012

It has been remarked in several previous works that the combination of cent er vortices and nexuses (a nexus is a monopole-like soliton whose world lin e mediates certain allowed changes of held strengths on vortex surfaces) ca rries topological charge quantized in units of 1/N for gauge group SU(N). T hese fractional charges arise from the interpretation of the standard topol ogical charge integral G (G) over tilde as a sum of (integral) intersection numbers weighted by certain (fractional) traces. We show that without nexu ses the sum of intersection numbers gives vanishing topological charge (sin ce vortex surfaces are closed and compact). With nexuses residing as world lines on vortices, the contributions to the total intersection number are w eighted by different trace factors, and yield a picture of the total topolo gical charge as a linking of a closed nexus world line with a vortex surfac e; this linking gives rise to non-vanishing bur integral total topological charge. This reflects the standard 2 pi periodicity of the theta;ingle. We argue that the Witten-Veneziano eta' relation. naively violating 2 pi perio dicity, scales properly with N at large N without requiring theta periodici ty of 2 pi N. This reflects the underlying composition of localized fractio nal topological charges, which are in general widely separated. Some simple models are given of this behavior. In the intersection-number picture of t opological charge, nexuses lead to non-standard surfaces for all SU(N) and intersections of surfaces which do not constitute manifolds for N > 2. We g eneralize previously introduced nexuses to all SU(N) in terms of a set of f undamental nexuses, which can be distorted into a configuration resembling the 't Hooft-Polyakov monopole with no strings. Nexuses can also be exhibit ed with thick non-singular strings, which generate vortices with nexus (and anti-nexus) world lines appearing as boundaries on the vortex surface. The existence of localized but widely separated fractional topological charges , adding to integers only on long distance scales, has important implicatio ns for fermion zero modes and the existence of standard chiral condensates in chiral symmetry breakdown, avoiding the usual difficulty when the number of flavors exceeds one, as we review.