In this talk I will discuss some of the many fascinating and highly
unusual impurity aspects of iron-based superconductors. This includes,
for example, the induction of impurity-induced long-range ordered phases
due to unconventional RKKY exchange couplings that would not be present
without the disorder. I will also discuss disorder effects in the
nematic phase above the transition temperature to the (pi, 0) magnetic
state but below the orthorhombic structural transition. The anisotropic
spin fluctuations in this region can be frozen by disorder, to create
elongated magnetic droplets whose anisotropy grows as the magnetic
transition is approached. Such states act as strong anisotropic defect
potentials that scatter with much higher probability perpendicular to
their length than parallel, although the actual crystal symmetry
breaking is tiny. From the calculated scattering potentials, relaxation
rates, and conductivity in this region we conclude that such emergent
defect states are essential for the transport anisotropy observed in
experiments. Below the SDW transition the nematogens freeze into dimer
states that show many characteristics in agreement with STM
measurements.
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