It is likely that nucleon-nucleon elastic scattering at large, fixed {vert_bar}{ital t}{vert_bar} can be described by the Landshoff three-gluon exchange mechanism. However, a phenomenological normalization rules out the possibility that the Landshoff mechanism is involved in producing the sharp structure of the two-spin asymmetry {ital A}{sub {ital N}{ital N}}, observed experimentally at {ital p}{sub lab}{approx}13 GeV/{ital c}, or that it is involved in producing the oscillations observed in {ital d}{sigma}/{ital dt} at 90{degree} in the c.m. frame. A simplified analysis of the 90{degree} amplitudes shows that it is likely that some subasymptotic mechanism interfering with the dominant quark-interchange amplitudes is responsible for both these intriguing phenomena. While the large-angle data show evidence for amplitudes approaching those of exclusive QCD, the Landshoff region in {ital pp}{r_arrow}{ital pp} shows no evidence for Sudhakov suppression nor evidence for effects associated with the running of the QCD coupling. We suggest that a measurement of the energy depenence of the polarization asymmetry at large {vert_bar}{minus}{ital t}{vert_bar} can greatly enlarge the understanding of exclusive QCD.