posted on 2021-10-05, 06:03authored byNicholas Hight-Huf, Yehiel Nagar, Adi Levi, James Nicolas Pagaduan, Avdhoot Datar, Reika Katsumata, Todd Emrick, Ashwin Ramasubramaniam, Doron Naveh, Michael D. Barnes
We
investigated the nature of graphene surface doping by zwitterionic
polymers and the implications of weak in-plane and strong through-plane
screening using a novel sample geometry that allows direct access
to either the graphene or the polymer side of a graphene/polymer interface.
Using both Kelvin probe and electrostatic force microscopies, we observed
a significant upshift in the Fermi level in graphene of ∼260
meV that was dominated by a change in polarizability rather than pure
charge transfer with the organic overlayer. This physical picture
is supported by density functional theory (DFT) calculations, which
describe a redistribution of charge in graphene in response to the
dipoles of the adsorbed zwitterionic moieties, analogous to a local
DC Stark effect. Strong metallic-like screening of the adsorbed dipoles
was observed by employing an inverted geometry, an effect identified
by DFT to arise from a strongly asymmetric redistribution of charge
confined to the side of graphene proximal to the zwitterion dipoles.
Transport measurements confirm n-type doping with no significant impact
on carrier mobility, thus demonstrating a route to desirable electronic
properties in devices that combine graphene with lithographically
patterned polymers.