Abstract
In the photovoltaic industry, an antireflection coating consisting of three SiNx layers with different refractive indexes is generally adopted to reduce the reflectance and raise the efficiency of monocrystalline silicon PERC (passivated emitter and rear cell) solar cells. However, for SiNx, a refractive index as low as about 1.40 cannot be achieved, which is the optimal value for the third layer of a triple-layer antireflection coating. Therefore, in this report the third layer is replaced by SiOx, which possesses a more appropriate refractive index of 1.46, it and can be easily integrated into the SiNx deposition process with the plasma-enhanced chemical vapor deposition (PECVD) method. Through simulation and analysis with SunSolve, three different thicknesses were selected to construct the SiOx third layer. The replacement of 15 nm SiNx with 30 nm SiOx as the third layer of antireflection coating can bring about an efficiency gain of 0.15%, which originates from the reflectance reduction and spectral response enhancement below about 550 nm wavelength. However, because the EVA encapsulation material of the solar module absorbs light in short wavelengths, the spectral response advantage of solar cells with 30 nm SiOx is partially covered up, resulting in a slightly lower cell-to-module (CTM) ratio and an output power gain of only 0.9 W for solar module.
Highlights
Antireflection coating plays an important role in the improvement of short-circuit current density and photovoltaic conversion efficiency of silicon solar cells
An antireflection coating consisting of three SiNx layers with different refractive indexes is generally adopted to reduce the reflectance and raise the efficiency of monocrystalline silicon PERC solar cells
Because of the physical constraint of SiNx, a refractive index as low as about 1.40 cannot be achieved, which is the optimal value for the third layer of triple-layer antireflection coating
Summary
Antireflection coating plays an important role in the improvement of short-circuit current density and photovoltaic conversion efficiency of silicon solar cells. The reflectance can be greatly decreased across the whole absorption band [1]. To achieve minimum reflection of a normal incident wave of a single wavelength, the antireflection coating may consist of a single layer, which must possess (a) a refractive index equal to the square root of the refractive indices of the materials bounding the coating and (b) a thickness equal to one-quarter of the wavelength within the material of which the coating consists [1], as shown in Equations (1) and (2). When the design wavelength is 550 nm (λair ), the optimal refractive index and thickness of the single-layer antireflection. For a double-layer antireflection coating, the design can be optimized with Equations (3)
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