Electrical AFM Characterization of Devices Using an Integrated Multi-Probe Platform

Jay Son¹, Edward Park¹, Luna Kim¹, John Park¹, Charles Kim¹, James Kerfoot², Andrea Cerreta²
¹Park Systems Corp., Gwacheon, South Korea ²Park Systems GmbH, Mannheim, Germany

 

 

Introduction
As research on next-generation semiconductor devices and two-dimensional (2D) materials continues to accelerate, there is growing demand for measurement platforms capable of probing both electrical behavior and nanoscale surface properties simultaneously. Atomic force microscopy (AFM) has long been an essential tool for nanoscale characterization, providing high-resolution imaging alongside electrical and mechanical measurements¹˒². However, advanced electrical AFM techniques—such as Kelvin probe force microscopy (KPFM), conductive AFM (C-AFM), and scanning thermal microscopy (SThM)—often require precise electrical contacts to nanoscale devices while scanning, creating significant experimental challenges³˒⁴.
In many laboratories, these contacts are made using external probe stations or manual probing approaches. While functional, such configurations frequently introduce complications including mechanical interference with the AFM scanner, poor reproducibility, limited placement precision, and additional mechanical loading on the sample stage. Large manipulators or external stages may also reduce stability during high-resolution AFM imaging.
To address these limitations, Park Systems and Imina Technologies have developed an integrated solution combining Park Systems AFM instrumentation with the Imina Technologies Microprobing Platform (4-Bot). In this configuration, up to four independently controlled miBot™ micro-robotic probes are mounted directly inside the AFM stage environment. Each miBot unit can be positioned with micrometer-scale precision to establish electrical contacts with the sample while maintaining full compatibility with AFM scanning.
The tungsten probes mounted on the miBot units can be connected directly to the auxiliary input/output channels of the AFM controller, enabling simultaneous source–drain biasing and electrical measurements during AFM operation. The integrated platform therefore enables multi-electrode device characterization and high-resolution nanoscale imaging within a single instrument.
This article outlines the integrated hardware configuration and demonstrates three representative applications enabled by this platform:

  1. Electrical contacting of layered materials and layered material heterostructures on insulating substrates
  2. In-operando nanoscale voltage mapping in lateral field-effect transistors
  3. Measurement of Joule heating in nano-structured electronic devices
    Together, these examples illustrate how the integrated system enables advanced electrical and thermal AFM characterization with improved flexibility and experimental control.

 

Integrated Hardware Platform
The experimental setup was configured by integrating a Park Systems FX200 AFM with the Imina Technologies Microprobing Platform (4-Bot). The probe station is mounted directly onto the FX200 sample chuck, allowing electrical probes to be positioned precisely near the region of interest without interfering with the AFM cantilever.

 

Figure 1. Integrated configuration of the Park Systems FX200 AFM and the Imina Technologies Microprobing Platform (4-Bot). (A) Photograph of the Imina Technologies Microprobing Platform (4-Bot) installed inside the Park Systems FX200 AFM, and (B) top view of the integrated setup. Up to four miBot units can be placed on the sample stage without mechanical interference with the AFM head or the cantilever.


Each miBot unit is magnetically anchored to the AFM stage, allowing rapid manual installation or removal. Up to four units can be positioned simultaneously, providing independent multi-electrode contacts for device measurements. The probes are manipulated using a dedicated positioning controller and a PC-connected control pad, which allows precise control of probe movement speed and direction.
An example configuration is shown with a device containing patterned gold electrodes placed on the FX200 stage. The AFM cantilever is first positioned near the region of interest. Tungsten probes mounted on the miBot units are then carefully aligned with the device contact pads. The alignment process is facilitated by the high-resolution optical vision system of the AFM and the intuitive operation of the Precisio™ software.

 

Figure 2. Multi-probe arrangement inside the Park Systems FX200 AFM, and signal & control configuration. (A) Optical image of a device with patterned gold electrodes loaded into the Park Systems FX200 AFM, acquired using the built-in vision system. Four tungsten probes mounted on miBot units are positioned on the targeted electrode pads in the vicinity of the AFM cantilever, enabling AFM measurements without mechanical interference with the individual probes. (B) Schematic diagram of the operating configuration in which the probe station is integrated with the AFM system. Each miBot is connected via two separate communication lines to the AFM controller and the positioning controller, respectively. The tungsten probes mounted on the miBot units are interfaced with the Aux1 and Aux2 Out channels of the AFM controller to apply AC/DC drive signals to the device, and with the Aux1 In and Aux2–4 In channels to acquire AC or AC/DC measurement signals. Up to four miBot units can be used simultaneously and are finely positioned by the positioning controller, while a PC-connected control pad provides an intuitive interface for independent probe manipulation.

 

Electrical connections are made through the AFM controller’s auxiliary channels. In the configuration used in this study:

  • Aux1 Out and Aux2 Out supply AC or DC drive signals to the device
  • Aux1 In and Aux2–4 In acquire electrical response signals from the device

This configuration enables simultaneous electrical excitation and measurement while the AFM performs nanoscale imaging. Because each miBot probe can be positioned independently, the system supports flexible multi-probe measurement configurations, including two-probe and four-probe device geometries.
The integrated system therefore provides a unified platform for studying nanoscale electrical behavior while maintaining stable AFM operation.

 

Electrical AFM of Electrically Floating Layered Materials
Layered materials (LMs) and layered material heterostructures (LMHs) have become key platforms for next-generation nanoelectronic devices. AFM-based electrical techniques such as conductive AFM and Kelvin probe force microscopy are widely used to study these materials, enabling nanoscale measurements of conductivity, potential distribution, and interfacial phenomena⁵.
However, these techniques generally require reliable electrical contacts. Conventional approaches often involve lithographic patterning and deposition of metal electrodes, which can complicate sample preparation and make it difficult to study materials during intermediate fabrication stages⁶.
Using the miBot microprobing system, electrical contacts can instead be applied directly to individual flakes of layered materials placed on insulating substrates.
In one experiment, a tungsten probe was positioned to contact a graphite region connected to a few-layer graphene (FLG) flake. The miBot contact served as a grounding point, preventing charge accumulation during KPFM measurements while simultaneously acting as a drain electrode during conductive AFM imaging.
To demonstrate the effect of grounding, local anodic oxidation was used to create channels that divided the FLG flake into electrically isolated regions. These channels completely separated portions of the flake from the contacted region.
AFM measurements revealed that the isolated regions developed distinct electrical potentials due to charge accumulation. In contrast, the region connected to the miBot probe remained electrically stable. Current mapping performed with C-AFM confirmed that current flow occurred only within the electrically contacted portion of the flake.

 

Figure 3. Contact-enabled HD-KPFM imaging and current mapping of FLG. (A) An optical view from the Park Systems FX200 camera showing a tungsten probe touching a graphite flake connected to FLG, with a schematic inset. (B) Non-contact mode height images of the FLG flake showing the height in addition to patterning achieved by anodic oxidation. (C, D) The electrical contact to the FLG enabled the acquisition of both stable single-pass HD-KPFM imaging over the contacted FLG in addition to maps of the current flow over different regions of the FLG.

 

This experiment demonstrates that direct electrical contacting using miBot probes enables stable electrical AFM measurements on layered materials without the need for pre-fabricated electrodes.

 

Electrical Characterization of Layered Material Heterostructures
The ability to electrically contact individual flakes also enables advanced characterization of layered material heterostructures.
One example involved heterodyne Kelvin probe force microscopy (HD-KPFM) measurements of a ferroelectric superlattice formed between two parallel stacked hexagonal boron nitride (hBN) layers on a few-layer graphene substrate deposited on SiO₂.
Single-pass HD-KPFM imaging revealed nanoscale variations in surface potential associated with the ferroelectric superlattice structure. The electrical grounding provided by the miBot probe was essential for stable measurements, since the KPFM tip bias would otherwise charge the flake and cause drift in the measured potential.
A second demonstration involved contacting a graphene flake aligned with a ~25 nm thick hBN layer on a mica membrane supported by PDMS. In this case the layered structure was still on the fabrication stamp used during heterostructure assembly.
Non-contact AFM imaging combined with conductive AFM revealed a moiré pattern between the graphene and hBN layers. The ability to perform electrical characterization directly on the fabrication stamp enables researchers to verify layer alignment and interfacial properties before additional fabrication steps are performed.
This capability reduces the risk of continuing nanofabrication on misaligned structures and allows researchers to study interfaces that may later become buried during device processing.

 

Figure 4. Contact-enabled HD-KPFM imaging and C-AFM moiré mapping of hBN/FLG heterostructures. (A,B,C) A parallel stacked hBN homostructure on an underlying FLG on 90 nm SiO₂ exhibiting a ferroelectric superlattice was contacted by a miBot before being measured by non-contact mode height and HD-KPFM potential, again revealing the absence of charging. (D,E,F) The utility of the technique was further exemplified by contacting an FLG flake on hBN on a mica/PDMS stamp prior to non-contact mode and C-AFM imaging revealing a moiré pattern between the FLG and hBN.

 

In-Operando KPFM of MoS₂ Field-Effect Devices
The integrated multi-probe platform also enables in-operando AFM measurements of operating electronic devices.
In this study, a MoS₂ thin-film device was fabricated by transferring a ~4 nm exfoliated MoS₂ flake onto a ~60 nm hBN layer deposited on a Si substrate with 280 nm thermal SiO₂. Source and drain electrodes composed of Cr/Au (10 nm/100 nm) were patterned using electron-beam lithography.
Local UV-ozone treatment was applied to selected regions of the MoS₂ channel to induce partial oxidation and modify the electronic properties of the device⁷⁻⁹.
For AFM measurements, two tungsten probes mounted on miBot units were placed on the source and drain electrodes. The AFM cantilever was positioned above the MoS₂ channel to perform Kelvin probe force microscopy.
During the experiment:

  • The drain electrode was held at 0 V (ground)
  • The source electrode was sequentially biased at −5 V, 0 V, and +5 V

KPFM surface potential maps were acquired for each bias condition.
The measurements revealed clear bias-dependent changes in the potential distribution across the channel. Line profiles extracted from the KPFM images showed that the potential at the source electrode accurately reflected the applied bias. A nearly linear potential drop was observed along the MoS₂ channel between the source and drain contacts.
This in-operando KPFM technique enables quantitative extraction of contact resistance and analysis of potential drop distributions within nanoscale devices. By comparing measurements obtained under different bias conditions, researchers can identify spatial variations in resistance, edge-related effects, and other localized transport phenomena.

Combining KPFM imaging with electrical measurements such as current–voltage (I–V) and gate-dependent transport measurements further enables correlations between the spatial potential landscape and the overall electronic behavior of the device.

 

Figure 5. KPFM measurements of a UV-ozone-treated MoS₂ thin-film device under source–drain bias. (A) Cross-sectional schematic of the MoS₂ thin-film device fabricated for KPFM measurements. (B) Optical microscope image of the fabricated MoS₂ thin-film device, where the blue box indicates the MoS₂ channel region used for the KPFM measurements. (C) Image acquired via the Park Systems FX200 camera after loading the sample and approaching the dedicated KPFM cantilever to the device for surface potential measurements. (D) AFM height image of the MoS₂ device transferred onto the hBN layer. Gold electrodes acting as the source (S) and drain (D) are located on the left and right, respectively, and KPFM measurements were performed in the central region indicated by the red dashed box. (E) KPFM surface potential images of the MoS₂ channel acquired with a source bias equal to +5, 0 and -5 V DC (from top to bottom) and with the drain electrode held at ground (0 V). (F) Line profiles of the KPFM surface potential.

 

Scanning Thermal Microscopy of Nano-Structured Devices
Beyond electrical characterization, the integrated platform also enables thermal measurements of nanoscale devices under electrical operation.
Scanning thermal microscopy (SThM) experiments were performed on nano-structured devices consisting of chains of nano-constrictions connected between large electrodes. These structures form spin Hall nano-oscillator chains¹⁰⁻¹².
Each device was electrically connected to top and bottom electrode pads, which were contacted using tungsten probes mounted on the miBot units. A Keithley Instruments 2636B source meter was used to inject constant DC current through the devices.
Thermal measurements were performed using the AppNano VertiSense™ SThM module with thermocouple-based AFM probes. The thermocouple voltage measured by the probe can be converted into temperature after calibration.
During the experiment, a constant 2 mA DC current was applied through the device while topography and thermal maps were acquired simultaneously.
The SThM measurements revealed localized temperature increases at the nano-constrictions. These locations correspond to regions where current density is highest, producing increased Joule heating.

 

Figure 6. Thermal mapping of nano devices. (A) Structures consist of a chain of nano-constrictions which are in electrical contact with a top and bottom pad, each one contacted via a needle probe. (B) Topographical map of a device with two nano-constrictions (top) and relative SThM map (bottom), where higher SThM voltage indicates a higher temperature. The same applies to (C) where a structure with five nano-constrictions was probed. For both (B) and (C), topography was mapped by means of a PPP-MFMR probe (Nanosensors) in non-contact mode, while SThM maps were obtained using a VTP-200 probe and the VertiSense™ setup from AppNano, with a constant current of 2 mA applied through the needles interfaced with a Keithley Instruments 2636B source meter.

 

By systematically varying the injected current, researchers can observe how thermal response evolves with electrical loading. Such measurements also allow identification of non-uniformities between constrictions that may indicate increased resistance or imperfect electrical connectivity.
This approach provides direct visualization of thermal hotspots and current crowding effects in nanoscale electronic devices.

 

Conclusions
The integration of the Park Systems FX200 AFM with the Imina Technologies Microprobing Platform (4-Bot) provides a powerful and flexible platform for advanced electrical and thermal characterization at the nanoscale.
By enabling precise alignment of miBot-mounted tungsten probes with the AFM cantilever inside the FX200 instrument, stable electrical contacts can be established while maintaining interference-free AFM scanning. This configuration allows simultaneous device biasing, electrical measurements, and high-resolution AFM imaging.
Several application examples demonstrate the capabilities of the integrated platform:
Electrical contacting of individual layered materials and layered material heterostructures on insulating substrates
In-operando Kelvin probe force microscopy mapping of voltage distribution in MoS₂ field-effect devices
Scanning thermal microscopy visualization of Joule heating in nano-structured electronic devices
For layered materials research, the ability to electrically contact individual flakes without lithographic processing provides significant experimental flexibility. For device characterization, the system enables direct visualization of potential distributions, contact resistance effects, and thermal hotspots during device operation.
These results demonstrate that the combination of Park Systems AFM technology and the Imina Technologies microprobing platform provides an integrated solution for nanoscale electrical and thermal characterization of 2D materials and thin-film electronic devices.

 

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