A two-parameter family of spherically symmetric, static Lorentzian wormholes
is obtained as the general solution of the equation ρ=ρt=0, where
ρ=Tijuiuj, ρt=(Tij−21Tgij)uiuj, and
uiui=−1. This equation characterizes a class of spacetimes which are
``self dual'' (in the sense of electrogravity duality). The class includes the
Schwarzschild black hole, a family of naked singularities, and a disjoint
family of Lorentzian wormholes, all of which have vanishing scalar curvature
(R=0). Properties of these spacetimes are discussed. Using isotropic
coordinates we delineate clearly the domains of parameter space for which
wormholes, nakedly singular spacetimes and the Schwarzschild black hole can be
obtained. A model for the required ``exotic'' stress-energy is discussed, and
the notion of traversability for the wormholes is also examined.Comment: 8 pages, RevTex two column, one figur