voltages. For this reason, these devices have entered successfully the fields of biosensors and bioelectronics, unfolding their innovative potential in biomolecules detection, [2][3][4][5] electrophysiology, [6][7][8] in vitro and in vivo cellular recordings. [9][10][11] Currently, intensive research effort is focused on novel OECT channel materials [12] and architectures [13] to gain faster response time, increased sensitivity, and lower power consumption targeting new applications in wearable technology and health care. [14][15][16][17][18] Despite their well-established relevance in the development of novel biotechnologies, the device physics still lacks a comprehensive understanding. Operational models able to accurately define and interpret the device working principle are required, as they would reveal well-aimed strategies for metrics refinement and guide targeted optimization of novel materials. Therefore, an improved knowledge of OECTs operation would impact on applications requiring higher sensitivity and amplification of the output signal, fast response time as well as selectivity.In a typical OECT configuration, an organic film deposited between two metal electrodes, that is, source (grounded) and drain collectors, and a gate electrode are in contact with the same electrolyte solution. The organic material constituting the transistor channel is usually poly(3,4-ethylenedioxythioph ene):poly(styrene sulfonate) (PEDOT:PSS), that is, a polyelectrolyte complex containing a degenerately p-doped semiconductor (PEDOT) and a polyelectrolyte counterion (PSS). The presence of multiple phases in thin films of PEDOT:PSS at the nanoscale has been revealed by scanning probe microscopy. Pancake-shaped PEDOT-rich islands are separated by lamellas of PSS-rich domains, thus forming a blend of electronic and ionic phases. [19] Mixed ionic and electronic transport is crucial in OECT operation and originates from the reversible doping/ dedoping mechanism of the organic film. It is well known that doping and dedoping of conjugated polymers like PEDOT rely on reversible electrochemical redox processes (oxidation and reduction, respectively). [20] Electrochemical doping is the phenomenon that rules OECTs operation and is driven by the applied potential between the polymer in the channel and the gate material. Concurrently, cations from the electrolyte are needed to compensate the charge excess of PSS − when PEDOT is dedoped and therefore the speed of electrochemical doping depends on the rate of the ionic flux across the electrolyte. [21] A comprehensive understanding of electrochemical and physical phenomena originating the response of electrolyte-gated transistors is crucial for improved handling and design of these devices. However, the lack of suitable tools for direct investigation of microscale effects has hindered the possibility to bridge the gap between experiments and theoretical models. In this contribution, a scanning probe setup is used to explore the operation mechanisms of organic electrochemical transistors b...