Advanced characterization methods avoiding transient
effects in
combination with solar cell performance monitoring reveal details
of reversible light-induced perovskite degradation under vacuum. A
clear signature of related deep defects in at least the 1 ppm range
is observed by low absorptance photocurrent spectroscopy. An efficiency
drop, together with deep defects, appears after minutes-long blue
illumination and disappears after 1 h or more in the dark. Systematic
comparison of perovskite materials prepared by different methods indicates
that this behavior is caused by the lead halide residual phase inherently
present in material prepared by the two-step method. X-ray photoelectron
spectroscopy confirms that lead halide when illuminated decomposes
into metallic lead and mobile iodine, which diffuses into the perovskite
phase, likely producing interstitial defects. Single-step preparation,
as well as preventing lead halide illumination, eliminates this effect.
Thin film solar cells are one of the important candidates utilized to reduce the cost of photovoltaic production by minimizing the usage of active materials. However, low light absorption due to low absorption coefficient and/or insufficient active layer thickness can limit the performance of thin film solar cells. Increasing the absorption of light that can be converted into electrical current in thin film solar cells is crucial for enhancing the overall efficiency and in reducing the cost. Therefore, light trapping strategies play a significant role in achieving this goal. The main objectives of light trapping techniques are to decrease incident light reflection, increase the light absorption, and modify the optical response of the device for use in different applications. Nanostructures utilize key sets of approaches to achieve these objectives, including gradual refractive index matching, and coupling incident light into guided modes and localized plasmon resonances, as well as surface plasmon polariton modes. In this review, we discuss some of the recent developments in the design and implementation of nanostructures for light trapping in solar cells. These include the development of solar cells containing photonic and plasmonic nanostructures. The distinct benefits and challenges of these schemes are also explained and discussed.
TiO 2 is most commonly employed as an electron transport layer (ETL) in mesoscopic n−i−p perovskite solar cells (PSCs). However, the low electron mobility, low electrical conductivity, and high electronic trap states of TiO 2 may have negative impacts on further enhancement of PSC performance. Metal doping is an efficient way to improve the electronic properties of TiO 2 films. In this work, we investigate the concentration-dependent impact of alkali lithium metal doping of the mesoporous TiO 2 ETL on the performance of mesoscopic CH 3 NH 3 PbI 3 PSCs. It was found that Li doping results in remarkable improvement in electrical conductivity and electron mobility and reduces the number of electronic trap states arising due to the oxygen vacancies within TiO 2 lattice. Such enhancements led to an enhanced charge extraction and transport and reduced charge recombination rate at the perovskite/ mesoporous TiO 2 interface as revealed by steady-state photoluminescence (PL) and time-resolved PL (TRPL) spectra, and resulted in an increase in the V OC , J SC , and FF of the PSCs. Moreover, the J−V curve hysteresis behavior after Li doping was effectively suppressed due to the reduced charge accumulation and recombination at the TiO 2 /perovskite interface. Consequently, the device performance relies on the concentration of alkali lithium metal doping, and the power conversion efficiency (PCE) of the PSC was significantly improved from 13.64% to 17.59% with reduced the J−V curve hysteresis behavior for a Li doped mesoporous TiO 2 layer with an optimized concentration of 30 mg/mL.
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