Gravitational lensing statistics can provide a direct and powerful tes
t of cosmic structure formation theories. Since lensing tests, directl
y, the magnitude of the nonlinear mass density fluctuations on lines o
f sight to distant objects, no issues of '' bias '' (of mass fluctuati
ons with respect to galaxy density fluctuations) exist here, although
lensing observations provide their own ambiguities of interpretation.
We develop numerical techniques for generating model density distribut
ions with the very large spatial dynamic range required by lensing con
siderations and for identifying regions of the simulations capable of
multiple image lensing in a conservative and computationally efficient
way that should be accurate for splittings significantly larger than
3''. Applying these techniques to existing standard Cold dark matter (
CDM) (OMEGA = 1) and Primeval Baryon Isocurvature (PBI) (OMEGA = 0.2)
simulations (normalized to the COBE amplitude), we find that the CDM m
odel predicts large splitting (>8'') lensing events roughly an order-o
f-magnitude more frequently than the PBI model. Under the reasonable b
ut idealized assumption that lensing structures can be modeled as sing
ular isothermal spheres (SIS), the predictions can be directly compare
d to observations of lensing events in quasar samples. Several large s
plitting (DELTAtheta > 8'') cases are predicted in the standard CDM mo
del (the exact number being dependent on the treatment of amplificatio
n bias), whereas none is observed. In a formal sense, the comparison e
xcludes the CDM model at high confidence (essentially for the same rea
son that CDM predicts excessive small-scale cosmic velocity dispersion
s.) A very rough assessment of low-density but flat CDM model (OMEGA =
0.3, LAMBDA/3H-0(2) = 0.7) indicates a far lower and probably accepta
ble level of lensing. The PBI model is consistent with, but not strong
ly tested by, the available lensing data, and other open models would
presumably do as well as PBI. These preliminary conclusions and the as
sumptions on which they are based can be tested and the analysis can b
e applied to other cosmogonic models by straightforward extension of t
he work presented