“…As is typical with large organic molecules [3,5,11,28], the partial cross-section for photoemission varies according to the orientation of the light vector potential A and the symmetry of the initial state ψ i , assuming that the fi nal state wave function ψ f (for electrons collected along the surface normal) is fully symmetric. The evidence of strong light polarization effects suggests a preferential orientation of the polymer chains as has been observed in other polymer systems [3,5,11,28], including a number of spin coated conducting polymers fi lms like such as polyaniline [3], polypyrrole [3], poly(3,4-ethylenedioxythiophene)-polyethylglycol (PEDOT-PEG) [28] and poly[2methoxy-5-(2′-ethyl-hexyloxy)-1,4-phenylene-vinylene] (MEH-PPV) [5]. Unfortunately, due to the low symmetry of RR-P3HT combined with the large number of overlapping molecular orbitals that contribute to each photoemission feature, we cannot conclusively ascertain, from Figure 2, the specifi c preferential orientation adopted by RR-P3HT in our fi lms.…”