The twin issues of the nature of the normal state and competing order(s) in
the iron arsenides are central to understanding their unconventional, high-Tc
superconductivity. We use a combination of transport anisotropy measurements on
detwinned Sr(Fe(1-x)Co(x))2As2 single crystals and local density approximation
plus dynamical mean field theory (LDA + DMFT) calculations to revisit these
issues. The peculiar resistivity anisotropy and its evolution with x are
naturally interpreted in terms of an underlying orbital-selective Mott
transition (OSMT) that gaps out the dxz or dyz states. Further, we use a
Landau-Ginzburg approach using LDA + DMFT input to rationalize a wide range of
anomalies seen up to optimal doping, providing strong evidence for secondary
electronic nematic order. These findings suggest that strong dynamical
fluctuations linked to a marginal quantum-critical point associated with this
OSMT and a secondary electronic nematic order constitute an intrinsically
electronic pairing mechanism for superconductivity in Fe arsenides.Comment: 9 pages, revtex4-1, published versio