Abstract

Hydrogenated amorphous silicon p–i–n solar cells with a 1 × 1 cm2 active surface area were fabricated using shadow masks on the 20 × 20 cm2 glass substrate coated with a fluorine-doped tin oxide film. The intrinsic, n-type hydrogenated amorphous silicon (a-Si:H), and p-type a-SiC:H thin films were deposited using plasma-enhanced chemical vapor deposition at 13.56 MHz plasma excitation frequency and on 20 × 20 cm2 and SnO2:F covered glass substrates. Low rf-power densities (less than 0.1 W/cm2) and substrate temperatures (less than 190 °C) were used for this purpose. Raman spectra of the films are dominated by a broad peak around 480 cm−1 that is the characteristic of the amorphous silicon network for all the three types of films. Scanning electron microscopy measurements revealed that the surface of the a-Si:H films deposited on SnO2:F-coated glass substrates (Asahi-VU) replicates the texture of the SnO2:F film. Spectroscopic ellipsometry spectra were analyzed with the Tauc–Lorentz dispersion model, and the results revealed that the optical gap of the intrinsic a-Si:H films is on the order of 1.7 eV, while that of the a-SiC:H is on the order of 1.8 eV. These results were further confirmed by optical transmission measurements. The highest efficiency obtained for solar cells prepared with shadow masking under our condition is on the order of 8.83% with a Voc of 0.856 V, a short circuit current density of 15.6 mA/cm2, and a fill factor of 66.07%. The obtained efficiency is slightly lower than the record efficiency obtained in this family of cells (10.3%) prepared by laser scribing because the low short-circuit current slightly lowers the fill factor. Impedance spectroscopy measurements were performed on the cells in the dark in the frequency range of 1 kHz–100 kHz. The analysis of impedance either in the Nyquist diagram or in the Bode diagram suggests a lumped circuit consisting of resistance Rs in series with a parallel combination of resistance Rp and capacitance Cp that account for the p–i–n structure. The value of Rp changed with the applied DC bias. The value of the series resistance agrees with the value obtained from the current–voltage characteristics of the cell.

Highlights

  • INTRODUCTIONDespite their lower efficiency compared to their crystalline silicon (c-Si) counterparts, single-junction hydrogenated amorphous silicon (a-Si:H) solar cells have attracted a lot of attention for several reasons: lower temperature coefficients of power and voltage, greater absorption of diffuse radiation, and abundance

  • Spectroscopic ellipsometry spectra were analyzed with the Tauc–Lorentz dispersion model, and the results revealed that the optical gap of the intrinsic amorphous silicon (a-Si):H films is on the order of 1.7 eV, while that of the a-SiC:H is on the order of 1.8 eV

  • Despite their lower efficiency compared to their crystalline silicon (c-Si) counterparts, single-junction hydrogenated amorphous silicon (a-Si:H) solar cells have attracted a lot of attention1–9 for several reasons: lower temperature coefficients of power and voltage, greater absorption of diffuse radiation, and abundance

Read more

Summary

INTRODUCTION

Despite their lower efficiency compared to their crystalline silicon (c-Si) counterparts, single-junction hydrogenated amorphous silicon (a-Si:H) solar cells have attracted a lot of attention for several reasons: lower temperature coefficients of power and voltage, greater absorption of diffuse radiation, and abundance. Multi-junction solar cells (double or triple junctions) offer another alternative to increase the cell efficiencies and go beyond the Queisser–Shockley limit for single junctions These are obtained by associating at least two sub-cells: a higher bandgap top cell (based on a-Si:H) and a lower bandgap bottom cell where various silicon alloy (a-SiGe:H) thin films are used.. Plasma enhanced chemical vapor deposition (PECVD) is by far the most used technique for the fabrication of various types of Si-thin films and cells both at the laboratory and at industrial scales.. Plasma enhanced chemical vapor deposition (PECVD) is by far the most used technique for the fabrication of various types of Si-thin films and cells both at the laboratory and at industrial scales.1–9,17 This technique offers the advantage of an easy control of the structure and microstructure (amorphous vs microcrystalline) and, the properties of the films. In addition to the photovoltaic parameter measurements, impedance spectroscopy was used to obtain information on the electrical properties of the solar cells

Deposition techniques and conditions
Characterization techniques
Structural properties of the a-Si:H and a-SiC:H films
Microstructure of the films
Solar cells
Impedance measurements
CONCLUSION
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call