2013
DOI: 10.1016/j.renene.2012.12.031
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Porous silicon Bragg mirrors on single- and multi-crystalline silicon for solar cells

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Cited by 31 publications
(16 citation statements)
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“…The experimentally measured absorption coefficient AL is about 10 2 -10 3 /cm in the wavelength range 1.1 m < < 2.5 m. Let us consider the infrared light trapping scheme that provides at least 100 passes of light through the active region of a modified device. The solar cells with the improved light trapping scheme can be achieved via the application, for example, Bragg mirrors [31][32][33]. The calculation of the additional photocurrent according to (2) with = 0 gives AL ∼ 2.4-5 mA/cm 2 .…”
Section: Effect Of Additional Infrared Photogeneration In Al On the Mmentioning
confidence: 99%
“…The experimentally measured absorption coefficient AL is about 10 2 -10 3 /cm in the wavelength range 1.1 m < < 2.5 m. Let us consider the infrared light trapping scheme that provides at least 100 passes of light through the active region of a modified device. The solar cells with the improved light trapping scheme can be achieved via the application, for example, Bragg mirrors [31][32][33]. The calculation of the additional photocurrent according to (2) with = 0 gives AL ∼ 2.4-5 mA/cm 2 .…”
Section: Effect Of Additional Infrared Photogeneration In Al On the Mmentioning
confidence: 99%
“…Moreover, the PS layer serves as luminescence down converter (see handbook chapter "▶ Photoluminescence of Porous Silicon") transforming the blue solar light to red-orange light which generates additional electron-hole pairs (Svrcek et al 2004). Application of porous silicon Bragg mirrors on backside of silicon solar cells can improve the efficiency (Ivanov et al 2013). It is also important to consider the passivation and gettering properties of Si-H and Si-O bonds on pore surfaces (see handbook chapter "▶ Porous Silicon Gettering") which can increase the lifetime of minority carriers (Remache et al 2010;Weiying et al 2011).…”
Section: Porous Silicon In Solar Cellsmentioning
confidence: 99%
“…This recent change therefore forces the industry to adopt new technologies which are reliable and compatible with cost effective industrial processes. However, light trapping within the cell is necessary to obtain the light absorption in the range of 800 to 1200 nm [4,7]. Therefore, to replace the classical Al BSF, an effective back reflector structure needs to be developed and implanted successfully into the cell [5][6][7][8].…”
Section: Introductionmentioning
confidence: 99%
“…Distributed Bragg reflector is a structure composed of a multilayer stack of high and low refractive index layers. Several configurations were published: Bragg mirrors implemented with (i) amorphous silicon and silicon oxide [1], (ii) SiN x and SiO x dielectric [12] (iii) porous silicon of two alternating porosities [2,7,[13][14][15]. The design of porous silicon Bragg mirror is complex and requires appropriate control of optical parameters of its constituent layers, and it produces many losses at the interface due to the excessive stack of porous silicon layers [3,16].…”
Section: Introductionmentioning
confidence: 99%