Evidence trail 01 / materials

Routes Through Transparent PV

There is no single transparent solar material. The useful distinction is how a device divides incoming light between transmission, absorption, reflection and collection.

Read alongside: optical spectraEvidence level: material → device

Transparency begins with a loss budget

A window cannot transmit and absorb the same photon at the same time. Conventional photovoltaic devices generally seek strong absorption across a broad useful spectrum. A transparent device deliberately gives up part of that opportunity to preserve a view or deliver daylight. That compromise is physical, not merely a sign that a manufacturing process needs improvement.

Start by asking what “transparent” means in the particular paper. Some authors describe a uniformly transmitting film; others describe an array of opaque cells separated by clear gaps. A third group describes a largely transparent light guide with cells hidden at its perimeter. These approaches may all produce a view through glass, but their appearance, electrical layout and scaling behaviour differ.

Selective absorption in a thin film

Wavelength-selective devices aim to harvest portions of the ultraviolet or near-infrared spectrum while transmitting much of the visible spectrum. Organic semiconductors are useful research candidates because their molecular structure can be adjusted to influence absorption. A complete organic photovoltaic device also needs charge-selective layers and electrodes, each of which introduces its own optical and electrical losses.

Richard Lunt and Vladimir Bulović described visibly transparent organic photovoltaic work in Applied Physics Letters in 2011. That paper is a useful historical entry point, not a specification for present-day windows. The Massachusetts Institute of Technology and Michigan State University are associated with important research in this area, but institutional association does not substitute for the test conditions of an individual device.

Even a selective absorber can leave a tint. Transparent electrodes may absorb light, reflect it or introduce haze. Sheet resistance also matters: a conductor that works across a small laboratory device may cause excessive resistive loss when current must travel farther across a large pane.

Primary reading: Lunt and Bulović, “Transparent, near-infrared organic photovoltaic solar cells for window and energy-scavenging applications,” Applied Physics Letters, 2011.

Thin absorbers and patterned openness

Another route reduces the thickness or coverage of an otherwise strongly absorbing photovoltaic material. Semitransparent perovskite devices can transmit light through a thin absorber, while patterned silicon or thin-film modules let light through gaps. These are not interchangeable strategies. Uniform films can change the colour of the entire view; patterned devices can produce visible geometry and non-uniform daylight.

For perovskites, the absorber composition, contacts and encapsulation influence both performance and stability. Some compositions contain lead, so material containment, damage scenarios and end-of-life handling deserve explicit attention. A laboratory efficiency result does not establish that the complete glazing assembly satisfies building requirements. Likewise, making an absorber thinner can increase transmission while reducing the number of photons available for current generation.

Edge collection changes the geometry

Luminescent solar concentrators use molecules or particles to absorb light and re-emit it at a different wavelength. Part of that emission is guided through a transparent plate to photovoltaic cells at its edges. The visible aperture can therefore remain relatively unobstructed, although colour, haze and optical losses still require measurement.

Reabsorption, escape through the plate surfaces and imperfect coupling to the edge cells all reduce collection. A short optical path in a small sample is not equivalent to the longer paths in a façade-sized pane. Reported efficiency also needs an area definition: output divided by the edge-cell area can look very different from output divided by the full window aperture.

Soft-lit three-dimensional diagram of a transparent light-guiding pane carrying re-emitted light toward photovoltaic cells at its edges
Concept illustration / edge collection moves the cells, not the need to account for losses.

Compare devices, not material names

Terms such as organic, perovskite or luminescent describe broad families. They do not specify a usable window. Ask for a transmission spectrum, an electrical measurement, an active-area definition and a photograph under controlled lighting. Then ask whether those results come from the same physical device. Combining the best transparency from one sample with the best efficiency from another creates a comparison that no actual pane achieves.

Durability should be equally specific. A material may tolerate one exposure while failing under a combination of heat, moisture, oxygen and illumination. Laboratory stability tests help identify mechanisms, but they cannot be translated into a guaranteed building service life without supporting evidence. Materials research is most informative when its boundaries remain visible.

Review context: Traverse and colleagues, “Emergence of highly transparent photovoltaics for distributed applications,” Nature Energy, 2017. Read individual device papers for current results and methods.

A practical reading sequence

  1. Identify where light is absorbed and where charge is collected.
  2. Check whether transmission and efficiency belong to the same sample.
  3. Separate aperture area from active photovoltaic area.
  4. Look for stability, scale and encapsulation evidence.

These steps do not select a winning material. They establish whether two results answer the same question. Only after that comparison does it make sense to discuss the architecture of an actual window.

Compare the trade-offs →