High-performance bifacial perovskite solar cells enabled by single-walled carbon nanotubes

Harnessing light’s dance, bifacial perovskite cells with carbon nanotube electrodes shine, boasting over 98% bifaciality and 36% power density. They promise a greener, cost-effective future with their feather-light, durable design.
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In the pursuit of harnessing albedo energy, bifacial photovoltaic (PV) devices emerge as a beacon of innovation. Perovskite solar cells (PSCs) are particularly adept in low-light conditions, displaying superior open-circuit voltage and minimal voltage loss, thus effectively capitalizing on albedo energy.

For peak bifacial performance, electrodes must be optically transparent, chemically stable, and harmonious with adjacent layers. Traditional materials like indium tin oxide (ITO) and fluorine-doped tin oxide (FTO) are hindered by their inherent brittleness, limiting their use in flexible applications. Additionally, the fabrication of transparent conducting oxides (TCOs) as back electrodes poses a significant challenge; the high-temperature deposition process risks compromising the delicate perovskite layers.

Addressing these limitations, our latest publication in Nature Communications introduces a feasible approach: employing single-walled carbon nanotubes (SWCNTs) as both front and back electrodes. This innovation not only promises enhanced transparency and conductivity but also ensures compatibility with the perovskite layer, heralding a new era for flexible, efficient bifacial PSCs.

a SEM image of the SWCNT film (scale bar = 500 nm). b TEM graph of a SWCNT film, and the average diameter of the individual tube is ~2.5 nm (scale bar = 10 nm). c Optical transmittances of the SWCNT films with various thicknesses. d Sheet resistances of SWCNT films. e Raman spectrum of the SWCNT film, and the high IG/ID ratio is illustrated.

Figure 1. Optical and electrical characterisations of SWCNTs prepared by FCCVD method. a SEM image of the SWCNT film (scale bar = 500 nm). b TEM graph of a SWCNT film, and the average diameter of the individual tube is ~2.5 nm (scale bar = 10 nm). c Optical transmittances of the SWCNT films with various thicknesses. d Sheet resistances of SWCNT films. e Raman spectrum of the SWCNT film, and the high IG/ID ratio is illustrated.

Optical and electrical characterizations (Figure 1) underscore the exceptional attributes of SWCNT films, positioning them as prime candidates for transparent electrodes in bifacial PSCs. Their remarkable optical transmittance and conductivity, coupled with a high G to D band intensity ratio (IG/ID = 162), signal high crystallinity and minimal defects, enhancing charge transport efficiency. Ultraviolet photoelectron spectroscopy reveals the SWCNT films’ work function to be approximately is about -4.70 eV, on par with ITO, underscoring their potential as a superior alternative in terms of work function, sheet resistance, and optical transmittance.

a PGD chart of bifacial PSCs under various albedo conditions. b J-V curves of an all-carbon-electrode-based PSC illuminated from the front side (100 mW cm-2) and back side (100 mW cm-2) simultaneously, and the inset picture depicts the characterization setup described in IEC TS 60904-1-2: double light source method. c Shelf storage stability records of an all-carbon-electrode-based PSC and control device under 25℃ and a relative humidity of 55% (dark, unencapsulated). d The thermal stability performance of all-carbon-electrode-based PSCs and their control counterparts were evaluated under sustained exposure to 85℃ in an N2-filled glove box, and inset pictures show that the control PSC becomes yellowish after 400hr (with orange border) whereas the all-carbon-electrode-based PSC is still black (with blue border). e Maximum power point (MPP) tracking of an all-carbon-electrode-based PSC and control device under N2 atmosphere, 1 sun continuous illumination without UV filter. (Temperature=25℃).

Figure 2. Photovoltaic performances of the all-carbon-electrode-based bifacial PSCs. a PGD chart of bifacial PSCs under various albedo conditions. b J-V curves of an all-carbon-electrode-based PSC illuminated from the front side (100 mW cm-2) and back side (100 mW cm-2) simultaneously, and the inset picture depicts the characterization setup described in IEC TS 60904-1-2: double light source method. c Shelf storage stability records of an all-carbon-electrode-based PSC and control device under 25℃ and a relative humidity of 55% (dark, unencapsulated). d The thermal stability performance of all-carbon-electrode-based PSCs and their control counterparts were evaluated under sustained exposure to 85℃ in an N2-filled glove box, and inset pictures show that the control PSC becomes yellowish after 400hr (with orange border) whereas the all-carbon-electrode-based PSC is still black (with blue border). e Maximum power point (MPP) tracking of an all-carbon-electrode-based PSC and control device under N2 atmosphere, 1 sun continuous illumination without UV filter. (Temperature=25℃).    

We then prepared bifacial devices by using SWCNT as both front and back electrodes and measured the corresponding performances (Figure 2). The resultant PSCs have demonstrated enhanced power generation density (PGD) under different albedo conditions. By removing ITO and back metal electrodes, the stability of these carbon-based devices has improved greatly. These results underscore the potential of SWCNT electrodes to create efficient and stable bifacial PSCs, promising a significant step forward in solar technology.  

Figure 5. Short-term (one year) and long-term (26 years) power output simulation of double-sided SWCNT@85% PSCs.

Figure 3. Short-term (one year) and long-term (26 years) power output simulation of double-sided SWCNT@85% PSCs. a The one-year power generation and the b power output for 26 years (from 2025 to 2050) (assuming the device area is 1m2). (Source data are provided as a Source Data file).

Power generation simulations (Figure 3) of bifacial PSCs for 2025 project a peak energy yield of 35 kWh in June, leveraging high sunlight exposure. Over a 26-year horizon, these PSCs are expected to deliver an annual output of 300 kWh. The integration of carbon materials in bifacial PSCs notably enhances energy generation, especially in urban landscapes rich in reflective glass surfaces, optimizing the harnessing of solar energy. 

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Physical Sciences > Materials Science > Materials for Energy and Catalysis > Perovskites

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