<p>Cubic lattice of the perovskite crystal ABX<sub>3</sub>. Reproduced with permission [<a href="#B31-nanomaterials-14-01867" class="html-bibr">31</a>], Copyright (2021) by John Wiley and Sons.</p> Full article ">Figure 2
<p>Evolution of PSCs: (<b>a</b>,<b>b</b>) energy levels of PSCs and (<b>c</b>–<b>h</b>) device structures of PSCs. Reprinted from [<a href="#B37-nanomaterials-14-01867" class="html-bibr">37</a>], Copyright (2019) by Frontiers Group.</p> Full article ">Figure 3
<p>Chalcogenide perovskite lattice and chemical elements at sites A and B. Reproduced with permission [<a href="#B48-nanomaterials-14-01867" class="html-bibr">48</a>], Copyright (2019) by John Wiley and Sons.</p> Full article ">Figure 4
<p>Passivation engineering: (<b>a</b>) reducing trap states to improve performance, (<b>b</b>) removal of hysteresis, (<b>c</b>) enhancing stability, and (<b>d</b>) photosensitive molecule-assisted passivation to inhibit undesired defect-assisted recombination. (<b>a</b>) Reprinted from [<a href="#B54-nanomaterials-14-01867" class="html-bibr">54</a>], Copyright (2021) by Elsevier’s Group. (<b>b</b>) Reproduced with permission [<a href="#B55-nanomaterials-14-01867" class="html-bibr">55</a>], Copyright (2019) by American Chemical Society. (<b>c</b>) Reprinted from [<a href="#B56-nanomaterials-14-01867" class="html-bibr">56</a>], Copyright (2021) by RSC Group. (<b>d</b>) Reproduced with permission [<a href="#B57-nanomaterials-14-01867" class="html-bibr">57</a>], Copyright (2023) by American Chemical Society.</p> Full article ">Figure 5
<p>(<b>a</b>) Oxidation parameters for Spiro-OMeTAD-based PSCs. (<b>b</b>) Band structure and energy level of an inverted organic photovoltaic device that utilizes an HTL of PEDOT:PSS doped with V<sub>2</sub>O<sub>5</sub>. (<b>c</b>) Examples of PTAA used with a perovskite and the resulting efficiency. (<b>d</b>) Doped PTAA with improved charge transport properties and a lower trap density. (<b>a</b>) Reproduced with permission [<a href="#B94-nanomaterials-14-01867" class="html-bibr">94</a>], Copyright (2022) by American Chemical Society. (<b>b</b>) Reprinted [<a href="#B95-nanomaterials-14-01867" class="html-bibr">95</a>], Copyright (2021) by John Wiley and Sons. (<b>c</b>) Reproduced with permission [<a href="#B96-nanomaterials-14-01867" class="html-bibr">96</a>], Copyright (2014) by American Chemical Society. (<b>d</b>) Reproduced with permission [<a href="#B97-nanomaterials-14-01867" class="html-bibr">97</a>], Copyright (2022) by Springer Nature Group.</p> Full article ">Figure 6
<p>(<b>a</b>) Cross-sectional SEM image of PSC with M-P3HT. (<b>b</b>) Steady-state PL spectra. (<b>c</b>) TRPL spectra. (<b>d</b>) J–V curves of champion devices based on P3HT, M-P3HT, and R-P3HT. (<b>e</b>) EQE spectra and integrated photocurrent curves of device with P3HT, M-P3HT, and R-P3HT. (<b>f</b>) Steady-state <span class="html-italic">PCE</span>. Reproduced with permission [<a href="#B109-nanomaterials-14-01867" class="html-bibr">109</a>], Copyright (2022) by Springer Nature Group.</p> Full article ">Figure 7
<p>Potential approaches for the HTL to enhance PSC efficiency.</p> Full article ">Figure 8
<p>(<b>a</b>) Device structure and relationship between current density and brightness with respect to applied bias (inset: EQE curves) and (<b>b</b>) high crystallinity, conductivity, and hole-extraction properties of a PSC with high <span class="html-italic">PCE</span> of 17.74% using low-temperature-processed Cu-doped NiO<sub>x</sub> [<a href="#B114-nanomaterials-14-01867" class="html-bibr">114</a>,<a href="#B116-nanomaterials-14-01867" class="html-bibr">116</a>]. (<b>a</b>) Reproduced with permission [<a href="#B114-nanomaterials-14-01867" class="html-bibr">114</a>], Copyright (2013) by John Wiley and Sons. (<b>b</b>) Reproduced with permission [<a href="#B116-nanomaterials-14-01867" class="html-bibr">116</a>], Copyright (2015) by John Wiley and Sons.</p> Full article ">Figure 9
<p>(<b>a</b>) Current–voltage (J-V) characteristics and steady photocurrent characteristics of PSCs based on NiCo<sub>2</sub>O<sub>4</sub> tested under AM 1.5 G illumination with an intensity of 100 mW cm<sup>−2</sup>. (<b>b</b>) p-i-n and n-i-p configurations for use of metal oxides as CTLs for both electrons and holes, leading to a higher <span class="html-italic">PCE</span>. (<b>c</b>) Inverted PSCs with a <span class="html-italic">PCE</span> of 19.91%, 14.6% higher than the control device, demonstrating promise of interfacial layer carrier transport for high-performance PSCs and expanding PSC material options. (<b>d</b>) Schematic and cross-sectional FESEM image of a device containing V<sub>2</sub>O<sub>5</sub>. (<b>e</b>) Hybrid ETLs with Cr<sub>2</sub>O<sub>3</sub>@GP and Cr<sub>2</sub>O<sub>3</sub>@CNT with an improved <span class="html-italic">PCE</span> of 18.5% and 26.8% compared to a plane ETL. (<b>a</b>) Reproduced with permission [<a href="#B129-nanomaterials-14-01867" class="html-bibr">129</a>], Copyright (2018) by John Wiley and Sons. (<b>b</b>) Reproduced with permission [<a href="#B130-nanomaterials-14-01867" class="html-bibr">130</a>], Copyright (2021) by Elsevier’s Group. (<b>c</b>) Reproduced with permission [<a href="#B131-nanomaterials-14-01867" class="html-bibr">131</a>], Copyright (2023) by Elsevier’s Group. (<b>d</b>) Reproduced with permission [<a href="#B132-nanomaterials-14-01867" class="html-bibr">132</a>], Copyright (2019) by American Chemical Society. (<b>e</b>) Reprinted [<a href="#B133-nanomaterials-14-01867" class="html-bibr">133</a>], Copyright (2017) by Royal Society of Chemistry.</p> Full article ">Figure 10
<p>Use of fullerenes in PSCs as an ETL. Reproduced with permission [<a href="#B148-nanomaterials-14-01867" class="html-bibr">148</a>], Copyright (2021) by Elsevier’s Group.</p> Full article ">Figure 11
<p>(<b>a</b>) Relationship between current and voltage in a DSSC with acetonitrile and an ionic liquid as electrolyte. (<b>b</b>) Structure of an FTO/TiO<sub>2</sub> compact layer/TiO<sub>2</sub> NS layer/perovskite/Spiro-OMeTAD/Au device used for the fabrication of PSCs in ambient conditions. (<b>c</b>) High levels of SnC<sub>2</sub>O<sub>4</sub> were used to produce SnO<sub>2</sub> films with an improved <span class="html-italic">PCE</span> of 21.31%. (<b>a</b>) Reproduced with permission [<a href="#B149-nanomaterials-14-01867" class="html-bibr">149</a>], Copyright (2009) by Elsevier’s Group. (<b>b</b>) Reproduced with permission [<a href="#B150-nanomaterials-14-01867" class="html-bibr">150</a>], Copyright (2023) by Elsevier’s Group. (<b>c</b>) Reproduced with permission [<a href="#B152-nanomaterials-14-01867" class="html-bibr">152</a>], Copyright (2022) by Elsevier’s Group.</p> Full article ">Figure 12
<p><span class="html-italic">PCE</span> of a ZnSe-modified PSC. Reproduced with permission [<a href="#B159-nanomaterials-14-01867" class="html-bibr">159</a>], Copyright (2019) by Elsevier’s Group.</p> Full article ">Figure 13
<p>Development of counter electrodes for more efficient, stable, and financially feasible PSCs for solar energy market adoption.</p> Full article ">Figure 14
<p>Delocalized surface states in PSCs. Reproduced with permission [<a href="#B168-nanomaterials-14-01867" class="html-bibr">168</a>], Copyright (2019) by Elsevier’s Group.</p> Full article ">Figure 15
<p>Key strategies used to enhance the stability of PSCs.</p> Full article ">Figure 16
<p>Potential directions for PSC systems.</p> Full article ">