Label-free
detection of charged biomolecules, such as DNA, has
experienced an increase in research activity in recent years, mainly
to obviate the need for elaborate and expensive pretreatments for
labeling target biomolecules. A promising label-free approach is based
on the detection of changes in the electrical surface potential on
biofunctionalized silicon field-effect devices. These devices require
a reliable and selective immobilization of charged biomolecules on
the device surface. In this work, self-assembled monolayers of phosphonic
acids are used to prepare organic interfaces with a high density of
peptide nucleic acid (PNA) bioreceptors, which are a synthetic analogue
to DNA, covalently bound either in a multidentate (∥PNA) or monodentate (⊥PNA) fashion to the underlying
silicon native oxide surface. The impact of the PNA bioreceptor orientation
on the sensing platform’s surface properties is characterized
in detail by water contact angle measurements, atomic force microscopy,
X-ray photoelectron spectroscopy, cyclic voltammetry, and electrochemical
impedance spectroscopy. Our results suggest that the multidentate
binding of the bioreceptor via attachment groups at the γ-points
along the PNA backbone leads to the formation of an extended, protruding,
and netlike three-dimensional metastructure. Typical “mesh”
sizes are on the order of 8 ± 2.5 nm in diameter, with no preferential
spatial orientation relative to the underlying surface. Contrarily,
the monodentate binding provides a spatially more oriented metastructure
comprising cylindrical features, of a typical size of 62 ± 23
× 12 ± 2 nm2. Additional cyclic voltammetry measurements
in a redox buffer solution containing a small and highly mobile Ru-based
complex reveal strikingly different insulating properties (ion diffusion
kinetics) of these two PNA systems. Investigation by electrochemical
impedance spectroscopy confirms that the binding mode has a significant
impact on the electrochemical properties of the functional PNA layers
represented by detectable changes of the conductance and capacitance
of the underlying silicon substrate in the range of 30–50%
depending on the surface organization of the bioreceptors in different
bias potential regimes.