MicroRNAs (miRNAs) are small non-coding nucleic acids of about 18-25 nucleotides which play a pivotal role in gene regulation of all superior organisms, including humans, and are involved in several cellular processes, such as proliferation, differentiation and apoptosis [1-3]. Given their physiological importance, deregulation of miRNAs is related to the development of numerous disease states, including multiple forms of cancer [4,5] Therefore, miRNAs are excellent molecular biomarkers with high potentialities in diagnostics [6-8]. However, their small size and low concentrations make the detection of miRNAs rather difficult. Currently, oligonucleotides are essentially detected by biomolecular techniques (e.g. real time PCR, northern blotting, microarray analysis) [9-11]. Although these methods may reach relatively high performances, their use in the clinical diagnostic field is rather hampered by several reasons. Indeed, they require long waiting times, necessitate the use of specific labels, and often involve extensive sample handling by highly specialized personnel with significant costs [
12]. Biosensors technologies are susceptible to offer good solutions to the above-mentioned problems, allowing, additionally, optimized and sensitive clinical detection of miRNAs [
13,
14]. A biosensor is a device able to perceive biological events (e.g., the interaction between two molecular partners) and to transduce them in the form of a chemical, physical or electrical signal [
15]. In the last decades, electrochemical biosensors, and in particular bio-Field Effect Transistor (bioFET) based device, have received great attention essentially because they can reach levels of sensitivity and specificity comparable to the canonical methods, being at the same time label-free, low cost, and presenting high potentiality to be automatized with no-or little sample pre-treatment [
16,
17,
18]. Briefly, in a FET device, the electric current flows between two electrodes (source and drain) linked by a semiconductor channel; a third electrode (gate), coupled to the device through a thin dielectric layer, can modulate the conductance between the drain-source electrodes according to its voltage [
19]. When specific biological probes, previously immobilized onto the gate surface, capture the target of interest a release of charges towards the gate electrode occurs. Accordingly, the change of the gate voltage will affect the source-drain current, allowing thus to correlate this variation to the target concentration [
20]. However, current detection involves only the accumulated charges within the so-called Debye distance from the electrode which, in turn, strongly depends on the ionic strength of the solution [
21,
22]. Natural capturing probes for miRNAs are constituted by their complementary DNA or RNA strands which give rise to duplexes via a hybridization process. Since both partners display negatively charged phosphate backbones, a high ionic strength is required to optimize the hybridization process; about 500mM represents the optimum ionic strength to shield the electrostatic repulsion and to facilitate nucleic acid hybridization [
23,
24]. Therefore, such a constraint limits the bioFET capabilities: indeed, the greater the ionic strength of the working solution, the smaller is the Debye length within which the charges carried by the target miRNAs that can be perceived [
21]. One promising solution to this problem may be represented by the use of peptide nucleic acids (PNAs) as capturing probe for miRNAs. PNAs are nucleotide analogues where the negative phosphate backbones are replaced by repeated units of N-(2- amminoetil)-glycine connected by peptide bond [
25,
26]. Accordingly, PNA, can hybridize with complementary nucleic acids at lower ionic strengths, when compared to canonical counterparts [
27,
28]; with a subsequent reduction of the Debye length leading to a substantial improvement of the bioFET detection capability. Therefore, this approach presents the important advantage to render accessible bioFET-based detection at physiological conditions which are usually characterized by an ionic strength of about 150mM [
29]. However, the absence of the negative phosphate backbones also modifies the interaction kinetics between PNA and the complementary nucleic acids; and the relationship between ionic strength and PNA-miRNAs interaction on solid surfaces should be therefore investigated [
30,
31,
32,
33]. On such a basis, the present work has the objective of paving the way for the development of a bioFET-based biosensor for a clinically relevant microRNA at physiological-like conditions by using PNA molecules as capturing probes. Our target is microRNA 155 (miR-155), a multifunctional miRNA regulating B cell differentiation and development stages, by also playing a key role in the mammalian immune system [
34,
35]. MiR-155 is overexpressed in various malignant tumor cells, such as hepatocellular carcinoma, breast cancer, colon cancer [
36,
37] whose detection deserves high interest, as biomarker, in diagnostics and prognosis [
38].