SPIE Digital Library Get updates from SPIE Newsroom
  • Newsroom Home
  • Astronomy
  • Biomedical Optics & Medical Imaging
  • Defense & Security
  • Electronic Imaging & Signal Processing
  • Illumination & Displays
  • Lasers & Sources
  • Micro/Nano Lithography
  • Nanotechnology
  • Optical Design & Engineering
  • Optoelectronics & Communications
  • Remote Sensing
  • Sensing & Measurement
  • Solar & Alternative Energy
  • Sign up for Newsroom E-Alerts
  • Information for:
    Advertisers
SPIE Photonics West 2017 | Register Today

SPIE Defense + Commercial Sensing 2017 | Call for Papers

Journal of Medical Imaging | Learn more

SPIE PRESS




Print PageEmail PageView PDF

Solar & Alternative Energy

Fluorescent borate glass enhances cadmium telluride solar cells

Using fluorescent samarium-doped borate glasses to cover cadmium telluride solar cells boosts efficiency in the UV.
11 June 2012, SPIE Newsroom. DOI: 10.1117/2.1201205.004235

The dominant solar cell technology in the photovoltaics market is based on crystalline silicon wafers. The search to lower production costs and reduce materials usage has led to the invention of thin-film solar modules that use very thin semiconductor layers to absorb and convert sunlight. Cadmium telluride (CdTe) is one of the thin-film technologies currently in use by the photovoltaics industry, but it works in only a limited range of solar frequencies (see Figure 1). We aim to improve the efficiency of conventional CdTe by converting unusable parts of the solar spectrum into usable frequencies.

Conventional CdTe solar cells cannot use IR light because these frequencies are less energetic than the bandgap of 1.45eV (855nm).1 On the other side of the spectrum, CdTe is limited because the UV and blue spectral ranges (that is, frequencies larger than 2.42eV, or 512nm) are absorbed in the cadmium sulfide buffer layer.2 The maximum short circuit current density of a CdTe solar cell, i.e. the total number of photons that lead to electron-hole pairs, is shown as the area under the blue curve in Figure 1. Our approach to improve the efficiency does not modify the solar cell itself. Instead, it alters the light-harvesting system. We replace the cover glass with a spectral converter made of fluorescent borate glass that takes photons of unusable frequencies and uses them to generate photons that CdTe can absorb.

Highly transparent, durable and inexpensive fluorescent borate glasses, such as samarium-doped barium borate (see Figure 2), convert the UV and blue part of the solar spectrum to yellow and red light, which can be more efficiently absorbed by the solar cell.3 This process, where a high-energy photon is absorbed and a photon with lower energy is subsequently emitted, is called frequency down-conversion. Borate glasses, which are additionally doped with fluorescent rare-earth ions such as trivalent samarium, have optical properties that complement the limitations in quantum efficiency of the CdTe solar cell. The chemical composition of borate glasses consists of boron oxide to form the network and metal oxides as network modifiers.


Figure 1. Photon flux density for the air mass 1.5 spectrum (black curve), external quantum efficiency of a CdTe solar cell (red curve), and the short-circuit current density (area under blue curve).4, 5

To investigate the potential of fluorescent glasses, we estimated the influence of a 3.2mm thick borate glass down-converter on the short-circuit current density. First we made cover plates for CdTe solar cells by cutting 3.2mm thick borate glass doped with samarium oxide (Sm2O3) into 20mm squares. The relative change in the short-circuit current density depends on two factors: the number of absorbed photons, which is given by the Sm2O3 doping concentration, and the number of converted photons, which depends on the Sm3+ conversion efficiency.

Figure 3 shows the relative changes in the CdTe solar cell efficiency as we change the Sm2O3 doping concentration and the Sm3+ conversion efficiency. Here, the number of emitted photons reaching the CdTe absorber is estimated to be 80%. (The number of absorbed photons was determined from absorption measurements on borate glasses with different Sm2O3 doping concentrations.) We found that a Sm3+ conversion efficiency of more than 14% leads to an efficiency increase in the short-circuit current density. Assuming a conversion efficiency of 100%, a 2% molar Sm2O3 doped glass superstrate enables a relative increase of almost 3%.


Figure 2. Fluorescent Sm3+-doped barium borate glass on a CdTe solar cell under UV excitation.

Figure 3. Relative changes in the CdTe solar cell efficiency with respect to Sm2O3doping concentration and Sm3+conversion efficiency of a 3.2mm thick barium borate cover glass.

In summary, upon excitation in the UV and blue spectral region, Sm3+-doped borate glasses show an intense fluorescence in the yellow and red spectral range. First estimates for barium borate glasses with different samarium doping concentrations reveal that relative increases of almost 3% in short-circuit current density of a CdTe solar cell can theoretically be achieved. The next step will be to determine how the Sm3+ conversion efficiency varies depending on the Sm2O3 doping concentration.


Franziska Steudel
Fraunhofer Center for Silicon Photovoltaics (CSP)
Halle (Saale), Germany
Marcel Dyrba
Fraunhofer CSP
Halle (Saale), Germany
and
Centre for Innovation Competence SiLi-nano
Martin Luther University of Halle-Wittenberg
Halle (Saale), Germany
Stefan Schweizer
Fraunhofer CSP
Halle (Saale), Germany
and
Department of Electrical Engineering
South Westphalia University of Applied Sciences
Soest, Germany

References:
1. J. J. Loferski, Optimization of II-VI based heterojunctions, Solid-State Electron. 30, p. 1205, 1987.
2. B. Cockayne, P. Wright, Metalorganic chemical vapour deposition of wide band gap II–VI compounds, J. Crys. Growth 68, p. 223, 1984.
3. M. Dyrba, P.-T. Miclea, S. Schweizer, Spectral down-conversion in Sm-doped borate glasses for photovoltaic applications, Proc SPIE 7725, p. 77251D, 2010. doi:10.1117/12.853942
4. A. S. for Testing, Materials, Reference Solar Spectral Irradiance: Air Mass 1.5, http://rredc.nrel.gov/solar/spectra/am1.5/, 2011. Accessed 4 May 2012.
5. M. Hädrich, C. Kraft, H. Metzner, U. Reislöhner, C. Löffler, W. Witthuhn, Formation of CdSxTe1 x at the p-n junction of CdS-CdTe solar cells, Physica Status Solidi C 6, p. 1257, 2009.