07.12.2020 •

Electronic Materials for Sustainable Energy Conversion and Storage

Harvesting energy directly from the sun in order to generate electricity, solar cells appear to represent the epitome of green energy. Unfortunately, the manufacturing process of common starting materials, like crystalline silicon as the main component of conventional solar cells, requires a huge amount of energy. Firstly, transforming silica ore into its crystallized form requires temperatures of above 2,000°C. Not only is this an incredibly energy-hungry process in itself, but obtaining ultra-pure silicon also involves several hazardous chemicals and a potent greenhouse gas. Other main offenders in the modern manufacture of many inorganic thin-film solar cells include components comprising finite resources such as indium, or the toxic elements selenium and cadmium. 

With the increasing strain on the global power grid and the drive towards sustainable energy production, we must therefore ensure that methods of manufacturing green-energy devices are equally sustainable – and this is the goal of Dr Manuela Schiek’s research group at the University of Oldenburg, Germany. Their research focuses on alternative materials for solar cell manufacture that are both non-hazardous and readily available. This includes the use of organic semiconductors within the energy-capturing active layer, and a transparent electrode system formed from a silver nanowire mesh embedded in an organic polymer matrix (see text box “organic solar cell architecture”).

With its complex multi-layered structure, surface analysis techniques provide vital insights into the workings of a solar cell. While tactile profilometry and Atomic Force Microscopy (AFM) have been the mainstays of surface metrology for a number of years, 3D confocal laser scanning microscopy (CLSM) is becoming an ever more popular tool.

Combining the ability to generate detailed, true-color optical images with the non-contact capabilities of laser scanning technology, the confocal laser scanning microscope really comes into its own as an optical profilometer. Faster and more efficient than stylus-based techniques, 3D CLSM is able to measure soft or adhesive surfaces and offers a resolution of 0.2 µm.

Organic solar cell architecture


The most popular organic solar cell architecture is based on a photon-harvesting active layer, sandwiched between two electrodes – one of which must be transparent in order to allow light to penetrate.

Photons hitting the organic semiconductor generate the charge-carrying excitons, which by the use of two materials – an electron donor and an electron acceptor - are then separated into their separate electron and holes. Driven by an electrical field, the electrons and holes travel toward their respective electrodes, creating the charge separation necessary to form an electrical circuit.

Dr Schiek’s research looks at using a transparent silver nanowire (AgNW) mesh electrode to replace the brittle and rare ITO, in addition to forming the active layer from organic materials as an alternative to environmentally damaging chemicals – creating flexible, sustainable and affordable thin-film solar cells for consumer applications.

Organic materials in the active layer

The active layer is where energy is captured from photons, and within organic solar cells this is often formed from a discontinuous blend of two materials – a polymer and a fullerene. With the polymer acting as an electron donor and the fullerene as an electron acceptor, this bulk heterojunction structure leads to enhanced charge separation of electrons and holes, and hence improved solar cell function. But polymers are often roughly defined mixtures of material with differing chain lengths, and with properties that are highly batch-specific. Molecular semiconductors, on the other hand, are defined building blocks with properties that can be adjusted by small changes to their structure, which can therefore be optimized for improved solar cell function. An interesting class of such molecules are the squaraine dyes (Figure 2), whose structure gives a broad absorption in the red region of the light spectrum. Dr Schiek’s research is investigating a bulk heterojunction active layer formed from squaraines mixed with a fullerene acceptor (for more information, see reference 1). The thickness of the active layer is crucial for this application: too thin and the mobility of charge carriers is restricted, but too thick and both light absorbance and flexibility are significantly reduced.

Accurate measurement of layer thickness is therefore equally important. Within Dr Schiek’s laboratory, once a scratch is made through the active layer surface with a fine needle, the step edges of this ‘valley’ are subsequently measured using profilometry. Tactile profilometry was previously relied upon, but the softness of the organic material hampered accurate measurement. In fact, a height discrepancy of around 20 nm was frequently observed between the two step edges, which is significant considering the average thickness of the active layer is 100 nm. As the needle steps up from the valley, it scratches into the surface and results in the false lower height reading.

With 3D confocal laser scanning microscopy, it is the laser that scans the surface, and such a non-contact approach achieves far greater accuracy of surface profilometry (Figure 3). Moreover, providing a visual image of the sample is more intuitive, and with the LEXT OLS4100 this information is easily compiled into a report, presenting the image in support of numerical data (Figure 2B).

Squaraines under polarized light

These molecular dyes present a sustainable alternative for the active layer, here visualized between crossed polars.

Fig. 2A: single crystals exhibit a golden metallic luster.
Fig. 2A: single crystals exhibit a golden metallic luster.
Fig. 2B: a spincoated layer of neat squaraine, with spherulite aggregates...
Fig. 2B: a spincoated layer of neat squaraine, with spherulite aggregates forming through crystallization upon thermal annealing.

Accurate metrology of soft material

Formed from soft organic material, the active layer is typically 100 nm thick and easily damaged by contact.

Fig. 3A: Non-contact profilometry.
Fig. 3A: Non-contact profilometry.
Fig. 3B: Data compiled into a report.
Fig. 3B: Data compiled into a report.

Transparent electrodes

Combining optical transparency with conduction, transparent electrodes form the anode of the solar cell while also allowing light to pass through to the active layer. The rapidly diminishing resource of ITO is currently the industrial standard for transparent electrodes. Moreover, ITO is a brittle material, restricting its use in mechanically flexible devices, and the hunt is on for a lightweight, cheap, flexible alternative that is also compatible with large-scale processing. Graphene presents a potential alternative, for example (Figure 3), but the flakes are quite small, which limits its use for larger areas.

One promising alternative is a mesh of silver nanowires (AgNWs) embedded in a polymer matrix, and a second project within Dr Schiek’s laboratory focuses on the production of the AgNWs, the subsequent processing to form the electrodes and ultimately the integration into organic solar cells.

For optimum conductivity, a uniform connection must exist between the active later and electrode, demanding a homogenous AgNW mesh. Since the diameter of AgNWs at 100 nm is equivalent to the thickness of the active layer, it is also important to avoid these regions of aggregation and to prevent puncturing the active layer. However, in practice this is challenging to achieve across the whole solar cell using current spin-coating production techniques, and surface roughness evaluation plays a central role in optimizing the synthesis protocol.

AFM has been the main technique employed for the surface roughness evaluation of the AgNW mesh, but CLSM (using the LEXT OLS4100) has vastly improved the efficiency of this. Firstly, Dr Schiek found that expanding the field of view using the image stitching function allowed her to view a more representative sample of the electrode surface. The AgNW mesh may appear regular on a smaller scale, but by creating high-resolution images of one mm2 (ten times greater than possible with AFM), regions of aggregation are easily identified that would otherwise have been missed (Figure 4A,B). As can be seen in Figure 4C, the software also allows the height profile to be visualized in 3D, useful for both analysis and documentation. Moreover, the ability to increase the low-pass filter from a height of 80 µm to 800 µm allows more insightful analysis of the elevated regions of the silver nanowires.

It is also the case that AFM is time consuming. Not only does the scan itself take up to an hour, after setting up the instrument and adjusting for tip-related artefacts, it can often take a whole day to acquire a single useful image. With 3D CLSM, image acquisition is rapid and also highly intuitive owing to the dedicated software, even for students lacking microscopy experience. In terms of performance, the researchers found that AFM and CLSM produced comparable results, and have benefited from the improved efficiency of surface roughness evaluation of transparent electrodes.

Another interesting aspect of this project is the far-reaching potential of transparent electrodes throughout opto-electronic applications, including LEDs and touch screens, where developing alternatives to ITO is also a focus of intense investigation. In the future, opto-electronic interfaces might even enable sight restoration, with retinal implants using light to generate electrical output and stimulating neuronal activity.

Fig. 4: A flake of multilayer graphene coated with a light emitting organic...
Fig. 4: A flake of multilayer graphene coated with a light emitting organic semiconductor.

This structure is currently under investigation for organic light emitting diodes, while graphene also has potential for use as a transparent electrode – although flakes are too small for larger photovoltaic surfaces. Visualized with crossed.

Surface roughness evaluation of silver nanowire mesh electrodes

Image stitching function expands the field of view, Low-pass cut-off filter set to 800 µm.

Fig. 5A: facilitating analysis of nanowire distribution on a larger scale in...
Fig. 5A: facilitating analysis of nanowire distribution on a larger scale in brightfield.
Fig. 5B: Height colour plot.
Fig. 5B: Height colour plot.
Fig. 5C: Organic solar cell architecture.
Fig. 5C: Organic solar cell architecture.


Feeding the global power grid in a sustainable fashion remains one of the biggest challenges faced by the modern world, and it’s an exciting time for research into innovative solutions. The use of widely available materials holds future promise in providing a green alternative to conventional solar cell manufacture, with such investigations driven by the latest technological developments.

From enabling accurate step measurements of the active layer with non-contact profilometry, to improving the efficiency of analysis with speed and advanced software functions, the 3C confocal laser scanning microscope has provided Dr Manuela Schiek’s research group with many advantages over stylus-based methods. As alternative energy becomes a greater focus in the coming years, the evolving light microscope technologies are likely to play a central role in the solar revolution.


This text is based on the following article: Markus Fabich: Alternative Materials for Alternative Energy, Olympus SE & CO. KG (Hamburg, Germany); https://www.olympus-ims.com/en/applications/alternative-materials-for-alternative-energy/.


[1] S. Brück, C. Krause, R. Turrisi, L. Beverina, S. Wilken, W. Saak, A. Lützen, H. Borchert, M. Schiek, J. Parisi, Structure–property relationship of anilino-squaraines in organic solar cells, Phys. Chem. Chem. Phys. 16 (2014) 1067.
[2] F. Balzer, H. H. Henrichsen, M. B. Klarskov, T. J. Booth, R. Sun, J. Parisi, M. Schiek, P. Bøggild, Directed self-assembled crystalline oligomer domains on graphene and graphite, Nanotechnology 25 (2014) 035602.