In thin films of doped organic semiconductors, the position
of
the Fermi level (E
F) within the semiconductor
fundamental gap depends not only on the dopant loading but also on
the energy-level alignment with the substrate. We show that the energy-level
alignment of the prototypical conjugated polymer poly(3-hexylthiophene)
(P3HT) with the common electrode material indium–tin oxide
puts E
F far from the midgap and close
to the highest occupied molecular orbital (HOMO) level of P3HT already
for undoped films, which are intrinsically p-doped through energy-level
alignment without dopant admixture. Intentional p-doping with molecular
electron acceptors does not necessarily result in notable E
F shifts, as we demonstrate by ultraviolet photoelectron
spectroscopy (UPS) for the common dopant tetracyanoquinodimethane
(TCNQ), which undergoes fractional charge transfer with P3HT. Fluorinated
TCNQ derivatives of higher electron affinity (EA), however, do show E
F shifts toward the P3HT HOMO, where high EA
and dopant loading can put E
F into the
P3HT-occupied density of states. This renders the conjugated polymer
semimetallic and is reminiscent of the degenerate doping scenario
found for inorganic semiconductors. By numerical energy-level alignment
modeling, which explicitly takes into account the substrate electronic
properties, we demonstrate that initial doping-related E
F shifts are clearly overestimated if a midgap position
of E
F is assumed for the undoped organic
semiconductor. For P3HT and a series of differently strong p-dopants,
we calculate E
F positions fully in line
with experimental UPS, which also allows for estimating the width
of the P3HT HOMO density of states and its doping-related broadening..