Introduction

In an era of photovoltaic technology, silicon is an efficient light absorber with relatively high-power conversion efficiency and best stability [1]. But high processing cost to obtain pure silicon has been remained as a challenge since its usage for photovoltaic purpose. To solve such problems, a lot of works have been done. The first application of low-cost semiconductors for photovoltaic was made using cadmium selenide (CdSe), cadmium telluride (CdTe), copper indium gallium disulfide (CIGS2), amorphous silicon, etc. [2,3,4,5]. Even if their processing cost is low, they are not able to compete with crystalline silicon in efficiency and stability. Additionally, they are criticized for toxic components and less abundance [6]. The second attempt was the development of the dye-sensitized, organic molecules and organic semiconducting polymers solar cells [7, 8]. Although they are valued by their interesting properties like flexibility, light weight, colorful appearance and low cost, they lack to fulfill the main requirements for commercial application due to their low power conversion efficiency and stability [9]. The highest record which is reported for the dye-sensitized solar cells is 14% after a long-time effort with less appreciated stability. After the dawning of semiconducting polymer [10] application of non-fullerene acceptors, the record PCE for organic solar cells is increased to 18% with undefined stability [11]. Nowadays, low-cost organic–inorganic lead halide perovskite materials which have been represented by general formula, ABX3, (A = CH3NH3+, CH(NH2)2+, Cs+, B = Pb2+, X = Cl, Br, I) are attracting the photovoltaic community due to its excellent optoelectronic properties such as high absorption coefficient [12], tunable band gaps [13], long charge carrier diffusion length [14], low exciton binding energy [15], ambipolar property and flexibility [16, 17].

The unprecedented growth in PCE of organic–inorganic perovskite solar cells (OIPSCs) from 3.9% in 2009 [12] to 25.5% in 2020 [18] is another factor that motivates researchers and the industry. The rate of publications in the area is highly increased and over 13,200 publications have been published since 2019 [19, 20]. Even though all evidences have been supporting its unprecedented growth in the history of photovoltaic devices, instability towards chemical and physical stresses are profoundly lagging their scalability and commercialization. Thus, unparalleled growth of PCE and long-term stability has been lasting as an assignment for researchers in the area. Large grain boundaries, pinholes, residuals, and current density–voltage (J–V) hysteresis which are resulted from formation of deep and shallow defects in addition to under-coordinated ions or atoms at the surface and/ or interfaces are well-thought-out for unmatched PCE and stability [21,22,23,24]. Octahedral tilting, rotations and deformations of corner sharing PbI62− octahedra are also suggested for lowering of the performance of the OIPSCs [25,26,27,28]. Besides, the chemical, photochemical and thermal instability, organic–inorganic perovskite (OIP) thin films are sensitive to moisture, O2, heat and UV light [29,30,31,32,33,34].These strengths that incomplete surface coverage of OIP films attributes the formation of non-uniform and rough surface, which scrutinized as deep-trap-density states centers at the grain boundaries (GBs) across the surface or interface of the OIP layer [35]. Defects formation across the interface of HOIP and hole transport layers is considered as a major cause for instability. For example, high PCE devices reported with Spiro-OMeTAD hole transport layer are facing different challenges from instability in ambient air. Even if the active layer is good, oxidative doped Spiro-OMeTAD layer induces leakage of air and moisture towards photoactive layer [36, 37]. As a result, the overall performance of the OIPSCs is abated because of recombination of charge carriers at the surface and/ or across interfaces. The degradation of HOIP in the presence of moisture has been analyzed and may result in the formation of PbX2, HX, and X—where X = Cl, Br and I [38,39,40]. To support this, T.P. Gujar and co-workers [41] studied the role of PbI2 in CH3NH3PbI3 perovskite stability, solar cell parameters and device degradation. XRD patterns show residual PbI2 formation on the surface of CH3NH3PbI3 films. The results prove that the PbI2 peak intensity increases as annealing time increases, while CH3NH3PbI3 peak intensity decreases. This indicates residual PbI2 formation is favored during annealing which lowers the quality of CH3NH3PbI3 film. Accordingly, the non-radiative recombination can occur due to the defected surface. To retard the crystallization of PbX2, researchers are working on the effect of chelation or coordination of Pb2+ with ligands. In this regard, addition of ligands or organic salts into OIP solution has shown to improve the PCE and/ or stability of the devices in the ambient air. This approach is mainly based on retarding the crystallization of PbX2 or increasing the crystallization of OIP. Research results show that uniform and smooth morphology of the OIP thin films are obtained by incorporating some appropriate additives [42,43,44]. Moreover, large grain size or small grain boundaries have been found to slow down deep-trap states, which cause charge recombination on the surface of OIP thin films. In this regard, formation of ionic or covalent or non-covalent bonds between ions or atoms in OIP and additives or passivators is very important to suppress dissociation of OIP films due to physical and chemical stresses [45].

To improve both the PCE and long stability of OIPSCs, researchers are exhaustively working on several mechanisms to reduce high trap-density states in OIP polycrystalline thin films. Compositional engineering, incorporation of additives, interface and surface passivation of light absorber layer, careful selection of charge transport layers, solvent engineering, and use of proper electrode layers get huge attention to minimize barriers towards commercialization of OIPSCs [46,47,48,49,50,51,52,53,54,55]. Structural engineering of 3D or 2D configurations is also investigated to get stable and reproducible OIPSCs [56]. The role of deposition techniques on whole performance is also studied as one of the mechanisms to fabricate stable OIP devices [57].

Recently, high-performance devices with significant stability were reported for large-area cells. Such findings inspire scholars in the area to look for different engineering strategies of additives, and surface passivation’s to champion OIPSCs in the future. Incorporation of additives into the precursor solutions, and surface passivation of the film has been repeatedly done to inhibit degradation and form defect-free OIP polycrystalline thin films [58,59,60]. In this mini-review, we are attempting to introduce the efficacies of additives and surface passivation on light absorber and charge transport layers. Additives are compounds which are added to precursors of photoactive film or charge transporting layers in order to improve surface and/or interface optoelectrical properties [61]. Passivation is the process of deactivating (healing) the effect of under-coordinated ions, residual, defects at the grain boundaries and pin holes at the surface or interfaces.

Photoactive layer additives and passivation

Photoactive layer additives

Additives are species which are incorporated into targeted material to improve morphological properties for desirable applications. In the history of the photovoltaics technology, additives have been applied to enhance the PCE and stability of dye-sensitized, and organic solar cells [62,63,64,65,66,67,68,69]. Nowadays, this approach is extensively used for surface and/or interface treatment of defects of different layers of OIPSCs [70, 71]. Its application has been driven from acid–base adduct formation principle between Pb2+ ions and lone pair electrons of the nitrogen, oxygen or sulfur atoms of additives. Hydrogen bonding between methyl ammonium or formamidinium and additives is also responsible for the immobility of the ions in the structure of OIP [72].

Solvent additives

Nowadays, solvent engineering has been widely used in the area of OIP photovoltaic to control the crystallization and grain growth during OIP film formation [73, 74]. On the other hand, the interaction of solvent with precursor solution of OIP plays a crucial role in improving the crystal growth of OIP thin film via retarding crystallization of precursors. The effect of weak and strong interaction of solvents with Pb2+ in controlling crystallinity of the targeted OIP was studied [75]. Under this study, the coordinating ability of the processing solvents with the Pb2+ center of the lead halide precursor is reported using Gutmann’s donating number, DN. As a consequence, the solvents which have high DN are reported as best solvents, which are strongly interacting with Pb2+. In other words, strong interactions of Pb2+ with solvent keep at the formation of precursor solution and decelerate the crystal growth rate, which is responsible for formation of large-grained crystals of OIP film by decreasing immediate crystallization of lead halides. This indicates that the strength of acid–base interactions between solvent and precursor is very important in the selection of solvents to increase solubility of precursors. Based on this, interactions of two organic solvent molecules, acetonitrile (ACN) and N-methyl-2-pyrrolidone (NMP) with PbBr2 to produce CsPbBr3 films are demonstrated by Y. Wu and co-workers [76]. The ACN is reported as the solvent which has weak interactions and NMP as the solvent which has strong interactions with Pb2+. This proves that strong coordination of NMP has resulted in the formation of a uniform and smooth surface of CsPbBr3 film. Consequently, greater PCE and stability are reported for NMP under high relative humidity. Solvent engineering to tune the adduct phase of mixed-cation perovskite precursor film was investigated by M. Wang and co-workers [77]. The XRD patterns (Fig. 1) before and after annealing demonstrate the appearance and disappearance of the adduct phase of mixed-cation precursor film, respectively. It also validates that the quality of precursor film is improved when the volume of DMSO is increased due to the disappearance of unwanted δ-perovskite.

Fig. 1
figure 1

Copyright 2019 published by Elsevier Ltd

XRD patterns of perovskite films with different DMF/DMSO volume ratios a before and b after annealing. Reproduced with permission from [77],

Their work verified that exceeding DMF:DMSO volume ratio beyond 3:5 is decreasing the quality of film due to excess DMSO interaction with PbI2 which results in residual PbI2 after removal of DMSO. These findings are also supported by SEM images of their work (Fig. 2). They suggested that the formation of defect-free and large grain-size crystals of mixed-cation perovskite films from Lewis acid–base adduct by solvent engineering attributes for enhanced PCE and stability.

Fig. 2
figure 2

Copyright 2019 published by Elsevier Ltd

SEM images of perovskite films based on different DMF/DMSO volume ratios: a 3:1, b 3:3, c 3:5, d 3:7. Reproduced with permission from [77],

Currently, OIPSCs technology calls for the fabrication of ambient air-stable devices with optimum PCE to compete with silicon solar cells using additives. It is well known that OIPSCs with the highest PCEs are fabricated in the glove box to minimize the effect of moisture and O2. Even though they have shown promising performance in the indoor environment, their performance declines due to degradation of photoactive or transport layers in the outdoor environment. Recently, researchers in the area are scrutinizing the achievement of improved PCE and stable OIPSCs in ambient air for commercialization [29, 52, 78, 79]. Different techniques have been attempted to fabricate efficient and stable OIPSCs in ambient air conditions. In very recent years, introduction of additives into precursor solution of photoactive layers of OIPSCs is widely applied and helps to improve the device performance in the ambient air. G. Wang et al. [80] used N-methyl pyrrolidone (NMP) as an active layer solvent additive to inhibit the formation of non-perovskite polymorph (δ-FAPbI3) in open air. This is because NMP is strongly interacted with Pb2+ to provide ameliorative nucleation for FAI.Pb2.NMP intermediate phase. The co-formation of non-perovskite polymorph (δ-FAPbI3) in the presence of dimethyl sulfoxide (DMSO) is occurred in ambient air. But good solubility of PbI2 in NMP offers a defect-free surface for (α-FAPbI3) in ambient air. Better PCE and stability from NMP suggests that there is a probability of scalable fabrication in open air. Bekele et al. used the tendency of acetylacetone solvent additive to solvate Pb2+ and form coordination via two keto-oxygen ligands and demonstrated its dual role to improve the device performance and stability. It has shown to be a promising approach to fabricate a large-area and stable devices with high reproducibility in the ambient environment [81].

Halogenated solvent additives get attention in improving PCE and stability of OIPSCs. P.W. Liang and co-workers [82] reported that the increased coverage and smoothness of the bidentate halogenated solvent additive, 1,8-diiodooctane (DIO) assisted film might be due to improved solubility of PbCl2 in mixed solvent DIO/DMF. They justified the incorporation of DIO with DMF induces fast nucleation and slow rate crystal growth during the film formation. As a result, the whole performance of the device is drastically enhanced.

Organic additives

The formation of pinholes, small grain sizes, and non-perovskite phases in OIP film bottlenecks the stability and scalability of OIPSCs to date. Researchers in the area are intensively working on different mechanisms and strategies that enhances the performance of OIPSCs. Li et al. [83] applied acetic acid as the additive in an anti-solvent chlorobenzene, to reduce the formation of residual PbI2 on the surface of OIP films. This is supported by results which are obtained from XPS data, shift of peaks for Pb 4f, C = O, O 1 s. This indicates the presence of interaction between the carbonyl group and Pb2+ ions. Accordingly, the results justify the interaction of Pb2+ with Pb2+ sensitive functional groups has better potential to produce defect-free surfaces which facilitate the charge carrier mobility with long diffusion length. This effect not only improves the surface quality but also it advances the interface quality.

Currently, this strategy is commonly deployed to form large grains which are expedient for charge carrier mobility on the surface of a light absorbing layer. For instance, C. Cui and his co-workers [84] mentioned that the device performance is slow down due to small grains which are associated with abundant grain boundaries. They used the volatile Lewis base, thioacetamide (TAA) as an additive to fabricate uniform films, smooth and high crystalline methylammonium lead iodide films with large grains. Scanning electron microscopy (SEM) images that prove the formation of large grains CH3NH3PbI3 films with 1.0% TAA are shown in Fig. 3. The large grains film formation is verified by the FTIR spectra, which verifies the strong interactions of Pb2+ with TAA and DMSO. Stoichiometric optimization with 1.0% TAA results in less trap state density and shows a superior PCE of 18.9%. They have also tested that the device with 1.0% TAA retains 88.9% of its initial performance after aging for 816 h in ambient conditions with 25–35% relative humidity (RH).

Fig. 3
figure 3

Copyright 2020 Published by Elsevier B.V

ad Top view SEM images of perovskite films with various TAA contents (0, 0.5, 1.0 and 2.0%). e Cross-sectional SEM image and the schematic structure of the perovskite solar cell device with 1.0% TAA. Reproduced with permission from [84],

Ionic additives

Charge carriers need smooth and uniform surfaces to offer good electrical conductivity. The contribution of organic salts such as ammonium acetate (NH4Ac) and zinc acetate (ZnAc2) in smoothing the surface of hole conductor-free carbon electrode-based perovskite solar cell is worked out by Zhang et al. [85]. Volatile NH4Ac gives better smooth surface than non-volatile ZnAc2, which forms pin holes and PbI2 residual on the surface of perovskite films (Fig. 4a). In addition, as shown in the schematic (Fig. 4b, c) Zn2+ undergoes doping to replace Pb2+, resulting in losing original properties of MAPbI3. XRD patterns also support the findings of SEM images and the crystal structure of MAPbI3 in the presence of the salts. This suggests that using suitable salts may mitigate defect induced recombination in low-cost carbon-based perovskite films. Accordingly, ammonium salts such as NH4Cl and NH4SCN additives in Spiro-OMeTAD hole conductor for CH3NH3PbI3-x(SCN)x-based planar PSCs yields better results in ambient air [86].

Fig. 4
figure 4

Copyright 2019 Published by Elsevier B.V

a Top view SEM images of the three types of films deposited on FTO/TiO2 substrates by one-step method (without carbon layer). The circular marks correspond to PbI2. b, c Schematic diagram of the crystal structure of MAPbI3 and MAPbI3:NH4Ac, MAPbI3 and MAPbI3:ZnAc2. Reproduced with permission from [85],

Cationic compositional engineering in perovskite solar cells has shown a blooming effect in improving both PCE and stability [87,88,89]. Studies related to cationic engineering shows that the interchange or mixing of cations induces change in optical properties, whereas partial or full substitution of Pb ions or halide ions results in tuning of the electrical properties of the OIPs. M. Kim et al. [90] investigated that the incorporation of methylammonium chloride (MACl) builds an intermediate phase which is transformed into the high quality pure α-phase FAPbI3 film. Disappearing of δ-FAPbI3 and PbI2 during annealing of the film in the presence of MACl, and the formation of high quality pure α-phase FAPbI3 film is justified by experimental results as shown in Fig. 5. X-ray diffraction (XRD) spectra (Fig. 5A), reciprocal full width at half maximum (FWHM) (Fig. 5B), time-resolved photoluminescence (TRPL) (Fig. 5E) and steady state photoluminescence spectra (Fig. 5F) measurements for pristine, 10%, 20%, 30%, 40% and 50% of MACl were reported by the group. But films with 40% MACl at 150 °C show large grains size. The corresponding device yield of PCE is exceeding 24% with significant thermal stability from pure α-phase FAPbI3.

Fig. 5
figure 5

Copyright 2019 published by Elsevier Inc

A, B, E, F XRD spectra, reciprocal FWHM at the diffraction peak 13.9̊ and photoluminescence data of perovskite films, respectively. C XRD data obtained from perovskite films prepared without MACl before and after annealing at 150 °C for 10 min. D XRD data obtained from perovskite films prepared with MA-40 before and after annealing at 150 °C for 10 min. Reproduced with permission from [90],

The role of surfactant-based additives in improving the PCE and stability of perovskite solar cells gives the room to use and look for them [91, 92]. J. Hong et al. [93] used poly(ethylene glycol) tridecyl ether (PTE) as a non-volatile polymer additive. Introducing ultra-small amount (less than 0.1 wt%) of PTE into the perovskite precursor solution controls the kinetics of crystallization. This facilitates the charge carrier mobility at the surface and interface of inverted OIPSCs.

Passivation of photoactive layer

Nowadays, passivation approach becomes the most popular strategy to minimize the recombination centers in either photoactive layer or interfaces between light absorber and charge transport layers [22, 94,95,96]. Different molecules have been developed to avoid and stabilize different types of defects, which are triggering non-radiative recombination at the surface and/ or interfaces of the perovskite layer in different structures of OIPSCs [43, 97]. Passivation of the surface or interface can occur by either chemical or physical processes. Chemical passivating agents undergo reaction with charged or neutral species at the surface and/ or interface before the generation of charge carriers. Physical passivating agents treat grain boundary defects and pin holes via physical interaction and improve surface coverage. To support this, M.S. Lee and co-workers [98] used a simple bidentate organic molecule, pyrazine (Pyr), which is undergoing both chemical and physical passivation. Pyr forms bidentate coordination with Pb2+ to prevent electrons reaction. This indicates that chemical passivation inhibits the reduction or oxidation of ions at the surface or interface of photoactive layer to produce neutral atoms or molecules. They reported that insertion of Pyr boosts the PCE of the device. One of the problems on the surface during operation is the chemical reaction which changes the optoelectronic properties of OIP film. Using co-passivating additives reduces the chemical reactions which are taking place on the surface. Guo and co-workers [99] applied 1H, 1H-Perfluorooctylamine (PFA) as a co-passivating agent. The comparative results between films with and without PEA show the importance of co-passivating agents for better performance of OIPSCs. Consequently, it helped to achieve promising results which motivate to design and synthesis other efficient co-passivating agents to fabricate large-area OIPSCs. PEA via chlorobenzene (antisolvent) was introduced as co-passivating agent which simultaneously lowers the surface and grain boundary defects.

The existence of defects or impurities in semiconductors has potential to change the optical and electrical properties of the semiconductors in both negative and positive aspects [100,101,102]. For example, impurities in silicon increase electrical conductivity. But in OIPSCs, the presence of bulk defects and impurities reduces the electrical conductivity due to non-radiative recombination of charge carries [103,104,105]. Accordingly, they beget current–voltage (IV) hysteresis, reduced PCE and instability for the device. D. Aidarkhanov et al. [106] showed that the defects at the interface of SnO2/mixed perovskite layers is passivated by introduction of optimal amount of organic cross linker, 2,2ʹ-(ethylenedioxy)bis(ethylammonium iodide) (EDAI) at the interface. The study shows that problems which are created because of defects can be solved by using suitable additives at the interface. IV hysteresis that may be rooted due to ion migration [107], or charge trap states [108] across interfaces is significantly reduced and the PCE of the device is increased with better stability. Dissolution of OIPs in a humid environment, which has some ionic and covalent characteristics [109], may cause loss of optoelectronic properties. This attributes to the formation of hydrated phases and lead halides on the surface of OIPs films [110, 111]. Based on this, different hydrophobic additives have been developed to mitigate the impact of moisture. C.F. Arias-Ramos et al. [112] applied a mixture of ethyl acetate (EA) and 4-tertbutyl-pyridine (tBP) as hydrophobic anti-solvent additive to extract the primary solvent from the precursor solution. The results suggested that using appropriate hydrophobic anti-solvent with proper optimization may give room to fabricate highly stable OIPSCs outside glovebox atmosphere. Liu et al. [113] demonstrated that polymethyl methacrylate (PMMA) passivate the interface of cesium formamidinium methyl ammonium lead triiodide (CsFAMAPbI3)/Spiro-OMeTAD and methyl ammonium lead triiodide (MAPbI3)/Spiro-OMeTAD in planar perovskite solar cells. Though doped Spiro-OMeTAD is appreciated for achievement of the highest PCE, it is reproached for oxidation at high temperature and infiltration of water through it to the photoactive layer. The insertion of hydrophobic PMMA between light absorbing and hole transport layer boosts both PCE and stability in outdoor because it reduces percolation of water. It is also acknowledged for having higher VOC and FF and less hysteresis compared to corresponding reference devices. Incorporation of polymethyl methacrylate (PMMA) into the PTAA hole transport layer is also reported and it provides high hydrophobic nature for the layer [114]. On the other hand, it improves the crystallinity of the OIP films by preventing moisture. Carbonyl groups of the PMAA contribute large grain formation. This helps to yield better PCE and stability for inverted structure.

Li et al. [115] reported that addition of quinolone to CH3NH3PbI3 precursor solution effectively suppresses the non-radiative recombination of carriers by co-passivating the defects at surface and grain boundaries. The XRD patterns prove the interaction between Pb2+ and lone pair electrons in quinolone, which confirms the formation of Lewis acid–base adduct. The optimized device with less hysteresis, improved stability and high PCE indicates that quinolone and compounds from the quinolone family can be applied as effective OIP additives. The high cost and less stable states of some hole transport materials forces to manufacture hole-free OIPSCs. Adding most favorable polyethylene glycol (PEG) concentration into MAPbI3 precursor solution produced high surface coverage and large grain size [116]. However, it behaves hygroscopic; it prevents OIP film from moisture and delivers interesting stability for the device. This is because it is preventing water molecules from reaching the surface of OIP films. Y.H. Lin et al. [117] reported the effect of additives on the thermal stability of mixed OIPSCs. It has been shown that the incorporation of organic–inorganic ionic salt additive 1-butyl-1-methylpiperidinium tetrafluoroborate ([BMP]+[BF4]) into the perovskite absorber minified deep-trap states. They justified that defects in Cs 0.17FA0.83Pb (I0.77Br0.23) based perovskite solar cells have been passivated through reaction between ([BMP]+[BF4]) and photogenerated superoxide and peroxide species from the surface of Cs 0.17FA0.83Pb (I0.77Br0.23) film [57]. This effect improves the performance and enhances the operational thermal stability of mixed OIPSCs which is stressed under full-spectrum sunlight at elevated temperatures up to 85 °C. In another study the impacts of lead halide residual are removed by adding an optimum amount of tetrabutyl ammonium bromide (TBAB) salt into pristine OIP films [118]. The role of TBAB is measured in terms of crystal growth kinetics alteration [119, 120]. As a result, it improved the PCE, stability and negative impact of the hysteresis.

Mixed dimensional structure is another approach to improve stability of OIPSCs [56, 121,122,123,124]. Studies show that, however, two-dimensional (2D) OIPs are more stable than three-dimensional (3D), their low PCE is not yet attractive [125]. To surpass the whole performance of the 2D OIPSCs, introduction of organic additives resulting in good quality of OIP crystal structure [126]. Zheng et al. [127], studied the synergistic effect of additives on 2D OIP films. N,N-dimethyl sulfoxide (DMSO) and thio-semicarbazide (TSC) were introduced as additives into the precursor solution. Consequently, trap state density of 2D OIP film is reduced and evidently about 93% increment of PCE and improved stability were achieved after the addition of additives. These results clearly magnify the positive impacts of additives on the whole performance of 2D OIPSCs. Other studies affirm that formation of the mixed 3D/2D structure yields efficient and stable perovskite solar cells in the presence of additives [128, 129]. D. Yao et al. demonstrated the capability of long-chain alkylamine organic compounds in hindering moisture permeation towards light absorbing layer [130]. As discussed in preceding part, the work proves that post-device treatment with vapor of diethyltriamine (DETA) and triethylenetetraamine (TETA), transformed 3D OIPs to lower dimensional (LD) crystals on account of partial substitution of cation by either DETA or TETA. Accordingly, the LD perovskite crystals are passivating 3D layers from moisture and deep-trap states across the interface.

Current studies are focusing on zwitterion molecules, which can bind with negatively and positively charged defects. These defects are intrinsic in nature, and they are supposed to be vacancies and ions at the surface and/ or interfaces. Thus, zwitterion type molecular passivators help to solve such problems by binding to two sites simultaneously. The comparative study between pyridine treated and pyridinium iodide, zwitterion molecule, was conducted by Y. Du and co-workers to indicate the role of zwitterion molecule in boosting the whole performance of the mixed-cation perovskite solar cells [131]. To suppress cationic and anionic defects from the surface and interface of OIP, low-cost ammonium chloride was used [132]. It passivates negatively charged cation vacancy defects by NH4+ and positively charged vacancy defects by Cl. As a result, imperfection of polycrystalline OIP film was improved and PCE of 21.38% was achieved.

Inverted architecture in perovskite solar cells has been widely used to solve the stability problems which are incorporated with mesoporous and planar devices [133, 134]. Emerging inverted perovskite solar cells which have used moisture sensitive and highly acidic poly (3, 4-ethylenedioxythiophene) polystyrene sulfonate) PEDOT:PSS as a hole transport layer are not stable enough and are less efficient [135]. J–V hysteresis are common problems in PEDOT:PSS integrated PSCs. To resolve this effect, inorganic hole transport materials are applied in inverted PSCs [136, 137]. Even if stability of inverted PSCs is upgraded due to incorporation of inorganic hole transport materials, their efficiency is not sufficient for scalability of OIPSCs. In recent times, different groups show interest to resolve the negative impacts of PEDOT:PSS by adding efficient additives at ITO/PEDOT:PSS or PEDOT:PSS/ perovskite interface or light absorber or charge transport layer surfaces [138,139,140]. Zhou and co-workers [141] studied on synergetic effects of multiple functional ionic liquid, EMIC (1-Ethyl-3-methylimidazolium chloride) treated PEDOT:PSS and S-acetylthiocholinechloride passivated perovskite surface. The result show improvement in PCE as well as stability of ITO/PEDOT:PSS(EMIC)/CH3NH3PbI3/S-acetylthiocholinechloride/C60/BCP/Ag configuration for a large area. An increase in electrical conductivities for the mentioned device is explained by an increase in the amount of PEDOT in the bipolaron states because of doping and the formation of defect-free OIP surface. Attempt to augment the performance of inverted PSCs has motivated the group of Zheng [142] to explore the role of n-butylamine (BA), phenethylamine (PEA), octylamine (OA) and oleylamine (OAm) in modifying grain boundaries and interface of the light absorber. They have found that long-chain alkylamine ligands (AALs) have potential to subdue deep-trap densities at the surface and/ or interfaces. This method enables them to achieve an inverted champion device with a PCE of 23% with significantly improved operational stability. It is well known that under-coordinated ions in OIPs are responsible for I–V hysteresis in the presence of mobile ions in the crystal. To prevent this issue, researchers are dedicated in looking for efficient passivation of ions migration. Luo et al. [138] demonstrated the effectiveness of ionic liquid, 1-methyl-3-propylimidazolium bromide (MPIB), in passivating under-coordinated Pb2+ in the perovskite film. The formation of PbI2 residual during OIP film annealing in pristine and disappearance of under-coordinated Pb2+ in the presence of MPIB was proved using X-ray diffraction (XRD) (Fig. 6). This affects the quality of crystal growth for OIP film with enhanced thermal stability. Hence, improved PCE with negligible IV hysteresis was reported from passivation of under-coordinated Pb2+ using MPIB. On other hands, ionic or hydrogen bond interactions could be favored when additives are purposefully added to precursors of OIP or OIP solution. Group of Choi [143] worked on the role of functional additives in performance of inverted planar OIPSCs. They found that OH functional groups in 2-hydroxyethyl acrylate (HEA) is strongly interacted with organic cation (CH3NH3+ or HC(NH2)2+. They proved that the crystallinity and grain sizes of OIP are improved and rate of non-radiative recombination is decreased. As a result, they achieved the highest PCE of 20.40% for a large-area (1.08 cm2) inverted planar OIPSCs. Under this study, the long-term stability is also reported for OIP with HEA.

Fig. 6
figure 6

Copyright 2020 Royal Society of Chemistry

X-ray diffraction (XRD) of the pristine perovskite and MPIB-perovskite (0.5) films. Reproduced with permission from [138],

Morphology improvement in crystalline semiconducting materials is very crucial to increase electrical conductivity. Kinetics of crystallization justifies that slow crystallization process attributes for large grains size of crystal. This effect is modifying the surface and interface optoelectronic properties of the materials. During OIP film formation, unreacted lead halides or cation halides in a solution contribute for incomplete surface coverage of the film. In 2019, Su et al. [144] engaged in the fabrication of defect-free OIP film using a two-step solution method in the presence of trimesic acid (TMA) as an additive in the lead precursor solution. It is reported that coordination of oxygen atoms in TMA with Pb2+ in lead precursor solution to form an intermediate which slows down fast crystallization to control the course of crystallization. Furthermore, the existence of hydrogen bonding between hydroxyl group of TMA and iodide in perovskite is depicted (Scheme 1) under this study. The cumulative effect of hydrogen bonding interactions with perovskite and oxygen atoms interactions with Pb2+ in the precursor solution is able to produce stable and pinholes-free large grain-sized perovskite film.

Scheme 1
scheme 1

Copyright 2019 Published by Elsevier B.V

Schematic representation of the interaction between perovskite and TMA. Reproduced with permission from [144],

Mechanical instability is the major challenge to fabricate flexible solar cells which is also common issue in flexible perovskite solar cells. It is believed that the addition of polymer additives can resolve such problems [140]. Based on this, Yao and co-workers reported the effectiveness of polymer additives in improving the morphological quality and mechanical instability of flexible perovskite solar cells [145]. By doing this, they obtained mechanically stable device. This shows that the addition of the optimum amount of polymer alloy additives has great potential to fabricate wearable electronics which are flexible. Similarly, S. Ma et al. [146] introduced N,Nˈ-bis-(1-naphthalenyl)-N,Nʹ-bis-phenyl-(1,1ʹ-biphenyl)-4,4ʹ-diamine (NPB), to fabricate uniform and pin holes-free OIP films. In addition to that, they mentioned that NPB offers good communication between PEDOT:PSS and OIP film due to its ability to adjust the energy level mismatch between PEDOT:PSS and OIP layers. The valence band energy of MAPbI3 and the HOMO energy level of PEDOT:PSS are − 5.43 eV and − 4.92 eV, respectively. But the HOMO energy level of NPB is − 5.40, which is able to adjust the mismatch between the two layers. This bestows enhanced performance for inverted flexible MAPbI3 solar cells under a humid atmosphere and UV light.

Additives which have ion migration blocking effect in perovskite solar cells are highly effective in eliminating I–V hysteresis. In addition to this, such additives contribute to reduce recombination centers by providing large grain-sized crystallinity for OIP films. In this regard, K. Zhu et al. [147] investigated the role of ethylamine alcohol chloride (EA.HCl) which contains hydroxyl (-OH) and ammonium cation (–NH3+) as the additive to reduce ion migration in the perovskite film. They verified that halide ion interactions in perovskite through hydrogen bonds of –OH or coordination of –NH3+ passivate defects and avoid ion migrations. The introduction of the optimal amount of EA.HCl enables to fabricate devices with improved PCE and negligible IV hysteresis (Fig. 7).

Fig. 7
figure 7

Copyright 2019 Published by Elsevier B.V

Current density–voltage (J–V) curves of devices with 1 wt% EA⋅HCl additive for reverse and forward scans. Reproduced with permission from [147],

Researchers use different organic compound additives containing carbonyl group to investigate its role to improve the PCE and stability of perovskite devices. Lately, Wang et al. [148] studied that strong interaction of C=O groups in caffeine with Pb2+ increases the activation energy of nucleation, which delays crystal growth to improve crystallinity of the OIP films. The finding suggests that caffeine and related alkaloids can improve the electrical conductivity and operational stability in ambient air. Inspiring results from biomaterial, betulin, which contains hydroxyl (–OH) functional groups and give a chance to use biologically active materials to passivate under-coordinated ions defects at the surface or interfaces of OIP [149]. Thus, the experimental and theoretical results show that the hydrogen bonds of betulin lock methylamine and halogen ion along the grain boundaries. This work reports the highest PCE, 21.15%, with remarkable chemical and thermal stability.

The effect of electrostatic force to avoid the surface and interface drawbacks is inspected. Zhang et al. [150] observed that the addition of chenodeoxycholic acid (CDCA) stabilizes the FAPbI3 film by electrostatic interaction between FAI and CDCA in which CDCA passivated the surface and interfaces of FAPbI3. Moreover, the effect of passivation is justified by shift of HOMO and LUMO energy levels after treatment which forms better communication at the interface of pristine and CDCA treated OPI films (Fig. 8). Other study by Xin et al. [151] also assures that the electrostatic interactions of molecules with positively and negatively charged point defects are declining the number of charge trapping centers from the surface by adding 2-amino-5-cyanopyridine (ACP), which contains electron-withdrawing (cyano) and electron donating (amine) groups into OIP film. The study suggested that similar features of ACP molecule with the zwitterion to bind with negatively and positively charged point defects of the film decreases the charge recombination rate across the surface or interface of the film. The result indicates that incorporation of ACP imparts good mechanical stability besides improving the PCE for regular flexible OIPSCs.

Fig. 8
figure 8

Copyright 2020 Published by Elsevier B.V

Energy levels and band structure diagram of functional layers for PVSC. Reproduced with permission from [150],

Even though mesoporous configurations of OIPSCs are noted in their highest PCE at this time, they are known for their fast degradation [152]. To maintain the PCE of mesoporous structure and improve the stability of devices, Xie et al. [153] applied three amides viz; formamide (FAM), acetoamide (AAM) and propionamide (PAM) to passivate the surface and regulate crystallographic structures. The result shows that 5% of AAM yields over 20% of PCE with better stability for meso-configured OIPSCs. They rationalized that strong interaction between AAM-5% and Pb2+ is responsible for formation of smooth and uniform crystalline film for the enhancement of the performance. The formation of residual of PbI2 is one of the common problems as a surface defect of perovskite films. Nishihara et al. [154] used formamidinium bromide (FABr) to react excess PbI2 to form FAPbBr3−xIx. The strategy is effective in passivating the surface of the film and facilitates the charge transport process.

Challenges in the case of the PCE and long-term stability of OIPSCs are mainly dealt with defects across of the HTL/light absorber layers interface. But defects at the interface of ETL/OIP layers have been causing immense problems, which are altering the optoelectronic properties of the interface. Amphoteric imidazole as passivator in inverted OIPSCs structure was tested [155]. It improves the quality of crystals as well as it reduces defects at the surface and grain boundaries. Consequently, imidazole treated OIP yields devices with promising PCE and stability. The derivative of imidazole, 2-methylbenzimidazole was introduced at the interface of SnO2/OIP film to solve defects-related anomalies [156]. Binding of the under-coordinated Pb2+ with lone pairs of 2-methylbenzimidazole to form acid–base adduct decreases the number of charge trapping centers. This approach yields devices with PCE of 21.6% having better humidity and thermal stability. Similarly, imidazolium iodide is used as auto-passivator to produce MAPbI3 and imidazole iodide [157]

Li et al. [158] studied organophosphorous ligands (trioctylphosphine oxide (TOPO) and triphenylphosphine oxide (TPPO)) as passivators. The results affirm that TPPO is more effective than TOPO. This is because benzene rings are facilitating charge transfer across the interface of HTM and photoactive layer in addition to oxygen atom which is an electron-rich center to bind with under-coordinated Pb2+. Dual advantages of TPPO result in the improved PCE and stability of the device. The group of Wu reported the potential of applying other organophosphorous compounds like tributyl phosphine (TBUP), triphenyl phosphine (PPh3), and trioctylphosphine (TOP) in reducing and oxidizing iodine (Io) and lead (Pbo) atoms defects [159]. TBUP is found to be more effective in reducing volatile Io and an oxidized form of TBUP is oxidizing Pbo to Pb2+. The studies show that the catalytic TBUP, which is passivating the defects, is integrated with tributyl phosphine oxide, which is binding with under-coordinated Pb2+, to subdue recombination impacts. So, it offers long-term operational thermal stability with attractive PCE for doped Spiro-OMeTAD containing perovskite solar cell.

Triphenyl(9-ethyl-9H-carbazol- 3-yl)-phosphonium bromide (TCPBr) and iodide (TCPI) were also applied as passivator of the OIP film [160]. The films which are without and with TCPBr and TCPI treatment are characterized by XRD. Results indicate that the amount of PbI2 is increasing after one month for pristine because of moisture but it is very low after two months in case of treated OIP films. This ascertains the great capability of TCPBr and TCPI in improving PCE and stability of Spiro-OMeTAD HTL-based perovskite solar cell.

N, N′-bis-(1, 1, 1, 2, 2, 3, 3, 4, 4-nonafluorodo- decan-6-yl)-perylenediimide (F-PDI), which is conductive, and hydrophobic organic molecule is analyzed for its competency in improving PCE and stability [161]. Its carbonyl groups which bind with under-coordinated Pb2+ passivate the surface. Besides that fluoro groups which are interacted with methyl ammonium cation to form hydrogen bonding provide immobility for monovalent cation. This strategy is crucial to ward off the phase transition of the cubic structure of OIP during annealing [162, 163].

Wu et al. [164] have revealed the potential of three kinds of large alkylammonium iodides viz. phenylethylammonium iodide, (PEAI), 1,4- butanediammonium iodide (BDAI), and guanidinium iodide (GAI) as passivating interlayer between hole transport layer and OIP layer in inverted structure. Their integration as an interlayer suppressed non-radiative recombination processes, which indicate their passivating role. Moreover, they enhanced charge selectivity from OIP to HTL. BDAI interlayer increased the open circuit voltage (Voc) of the device without affecting short-circuit current density (Jsc) and fill factor (FF). These features helped to yield a competitor PCE for inverted OIPSCs with negligible hysteresis.

Charge transporting layers additives and passivators

It is well known that the total number of charge carriers which are transported via charge transporting layers is critical to harvest maximum PCE. But different defects in charge transporting layers are acting as trapping centers of charge carriers and lowering the performance of the OIPSCs. For example, mesoporous TiO2 as an electron and doped Spiro-OMeTAD as hole transport layers are widely deployed in OIPSCs technologies [165]. Devices with mesoporous TiO2 are showing better PCE than devices based on dense TiO2 which is due to an increase in surface area of the light absorber [166]. But both mesoporous scaffolds of TiO2 and dense TiO2 suffers from a large number of oxygen vacancies, which are deliberated as trapping centers for electrons. The commonly used additives are infused to charge transporting layers to form uniform and smooth surface morphology. Not only that, they helped to have good communication between the interface of charge transporting and other layers in OIPSCs by reducing charge carriers trapping centers, but they can also adjust energy level alignments [167, 168]. Lose in the original properties of charge transporting layers in the presence of moisture, O2, and UV–Vis light has been lowering PCE and stability of perovskite solar cells. For this reason, different surface or interface properties modifiers have been emerged to manage such problems.

Solvent-based additives

Organic halides or lead halide crystalline aggregates formation on the surface during OIP film fabrication investigated as a contributor for charge carriers recombination. Recent works point out that some charge transport materials which are suspicious towards the formation of aggregates [46, 169, 170]. Solvent additive engineering is used to minimize the causes which are responsible for formation of aggregates due to charge transporting layers. Ye et al. [171] worked on engineering of a series of solvent additives (1,8-diiodoctane, 1-chloronaphthalene, 1-phenylnaphtha-lene, 1-methylnaphthalene) to improve the influence of electron transport layer, perylene diimide derivatives (PDIs) in the film morphology and transport process. They found that 1-methylnaphthalene (MN) was the best solvent additive to control the effect of aggregates in 1,1ʹ-bis(2-methoxyethoxyl)-7,7ʹ-(2,5-thienyl)bis-(BIS-PDI-EG) films. In general, addition of 1-methylnaphthalene into perylenediimide derivatives (PDIs) was effective in improving both PCE and stability of the OIPSCs.

Organic compounds-based additives

Hygroscopic dopant, lithium bis(trifluoromethanesulfonyl)imide (Li-TFSI), in Spiro-OMeTAD-based perovskite solar cells is responsible for fast decay of the device performance as a result of aggregate formation. Searching for hydrophobic dopants which will substitute Li-TFSI is very crucial to increase the electrical conductivity of Spiro-OMeTAD layer in ambient air condition. Hydrophobic alkaline-earth bis(trifluoromethanesulfonyl)imide additives such as Mg-TFSI2 and Ca-TFSI2 were developed by N.D. Pham and co-workers to increase moisture resistivity of the Spiro-OMeTAD [172]. Comparative study of Li-TFSI, Mg-TFSI2 and Ca-TFSI2 by using different methods reveals that alkaline-earth bis(trifluoromethanesulfonyl)imide additives have better potential than Li-TFSI. For instance, the calculated hole mobilities for Mg-TFSI2 and Ca-TFSI2 are greater than Li-TFSI. Consequently, they obtained noteworthy PCE and stability from Spiro-OMeTAD-based OIPSC.

The main purpose of dopants in Spiro-OMeTAD is to oxidize the HTL. Consequently, thionyl chloride (SOCl2) dopant which is capable of generating more oxidized states of spiro-OMetAD was developed by the group of Li [173]. The experimental findings prove that the optimum amount of SOCl2 increases the concentration of holes as well as its mobility to achieve better PCE. The instability which is criticized in the presence Li-TFSI is upgraded by inclusion of SOCl2 because of suppression of density of defect states from the interface. Moreover, Hu et al. [174] studied the effectiveness of fullerene and its derivatives as OIP additives to improve the PCE and stability of OIPSCs in ambient conditions. They observed that addition of these materials to OIP solution improves the crystal quality, enlarges grain size and reduces grain boundaries. Consequently, the electron extraction and transport have been increased in OIP films. The FTIR spectra prove that the formation of Lewis acid–base adduct from Pb2+ and C60 derivatives and weakening of dissolution of PbI2 in the presence of moisture. As a result, they reported improved stability from nitrogen containing C60 derivatives in ambient environment. The development of naphthalene imide dimer (2FBT2NDI) by group of H. Wang [175] resulted in achieving maximum PCE of inverted OIPSCs. They affirmed the effectiveness of it in passivating the surface and interface of OIP layer. The same forward and reverse current scans indicate, defects and ions which are causing hysteresis are negligible in the device. Furthermore, it facilitates electron extraction across the interface of OIP/PCBM. So, the summative qualities of 2FBT2NDI integration offer the maximum PCE for inverted OIPSC. Poly (2,2ʹ-bithiazolothienyl-4,4ʹ,10,10ʹ-tetracarboxydiimide) (PDTzTI) which contains sulfur, nitrogen and oxygen functional groups was also used as ETL in inverted OIPSCs [176]. In addition to charge selectivity, it is passivating the interface of OIP due to possible interactions between Pb2+ and the functional groups (Fig. 9). The synergistic effect of this polymer yields greater PCE (20.86%) than 2FBT2NDI, which is the highest for inverted structure to date. Hydrophobic nature of PDTzTI is also benefiting to improve the long-term operational stability of OIPSCs.

Fig. 9
figure 9

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Schematic illustration of the perovskite/PDTzTI interfaces. The enlarged area describes the possible interactions between unsaturated Pb ions (likely Pb trap/defect sites) and functional group (N, S, O) presented in the PDTzTI ETLs. Reproduced with permission from [176],

Similarly, 4ʹ,4ʹʹʹ-(1,3,4-oxadiazole-2,5-diyl)bis(N,N-bis(4-methoxyphenyl)-[1,1ʹ-biphenyl]-4-amine) was designed and synthesized as HTL to transport holes and passivate the Pb2+ by Lee et al. [177]. They found that methoxy functional groups in the HTL are very important in adjusting energy alignment of HOMO of HTL with OIP.

Alkoxy-PTEG HTM with multifunctional groups was designed and synthesized by Lee et al. [178]. The presence of alkoxy groups in it offers multipurpose advantages. For example; (1) it increases solubility of alkoxy-PTEG in nonaromatic green solvent (3-methyl cyclohexanone) which is occurring naturally, (2) it prevents the leakage of lead ions by chelating with it, (3) it enhances the electrical conductivity of alkoxy-PTEG, which is comparable with doped Spiro-OMeTAD and (4) it exhibits improved Voc and FF. Alkoxy-PTEG HTM which is processed in nonaromatic green solvent exhibits inviting PCE (19.9%) from SnO2 planar OIPSCs. On the other hand, dopant-free alkoxy-PTEG HTM which is processed in 2-methyl anisole (2-MA) which is an aromatic solvent with low toxicity potential shows 21.2% of PCE which is reported as the highest value. Besides these, it improves chemical and thermal stability of OIP films.

Ionic-based additives

Oxygen vacancies in commonly used ETL, TiO2 are considered as trapping centers for electrons, which are causing non-radiative recombinations in regular OIPSCs [179,180,181]. Unstability due to TiO2 demands several approaches which can reduce side effects in regular planar perovskite solar cells. NaCl-assisted defect passivation study has been done to empower electrons extraction of TiO2 by Li et al. [182]. They reported that Na+ ions-doped TiO2 improved the wettability of OIP films. As a result, 5% Na-doped TiO2 shows the remarkable change in average grain size and grain boundaries of the perovskite layer (Fig. 10).

Fig. 10
figure 10

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SEM images of the perovskite layer fabricated on a the pristine and b 2%, c 5%, d 10%, and e 20% Na-doped TiO2 films, respectively. The insets are the statistic distributions of grain size analyzed from individual images. Reproduced with permission from [182],

In addition, oxygen vacancies in TiO2 which are scavenging electrons are deactivated by incorporation of NaCl salt. Thus, electron transporting potential of TiO2 is enhanced. Also the measured higher recombination resistance owing to NaCl has contributed significant change in long-term stability and hysteresis in n-i-p perovskite solar cells. Also, Sun et al. [183] asserted the role of optimum Na2S to passivate TiO2 and OIP surfaces. Herein, Na+ ions are doping the TiO2, while S2− ions are interacting with Pb2+ ions to form covalent bonds, which are ruled out by soft acid–base principle. Na+ ions-doped TiO2 increased wettability degree of OIP films as mentioned by Li et al. [182]. As a result, experimental results verify that incorporation of Na2S passivated the interface and improved the crystallinity of OIP films. Significant change has been observed in current density and Voc of planar OIPSCs fabricated after incorporation of Na2S into TiO2 ETLs. The other study (Fig. 11) on inverted perovskite solar cells using surfactant additives has been reported by Wang et al. [184].

Fig. 11
figure 11

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The contact angle of water on the NiOx/SDBS film with different concentrations (mg mL−1) of SDBS: a 0, b 0.05, c 0.20, d 1 and e 10. Top view SEM and AFM images of perovskite films deposited on NiOx/SDBS film with different concentrations (mg mL−1) of SDBS: 0 (f, k), 0.05 (g, l), 0.20 (h, m), 1 (i, n) and 10 (j, o). p Statistics of grain size and surface roughness of perovskite films deposited on NiOx/SDBS film with different concentrations of SDBS solution. Cross-sectional SEM images of perovskite layers grown on NiOx film q without and r with SDBS layer. Reproduced with permission from [184],

They coated an ultrathin sodium dodecyl benzene sulfonate (SDBS) on the surface of nickel oxide (NiOx) HTL, that is between HTL and light absorber layer. They explained that the reason for good communication at the interface of NiOx/perovskite surface is surface wettability potential of SDBS. Thus, the SDBS is adjusting the surface wettability of NiOx to form a fully covered perovskite film, which provides high quality crystalline perovskite film.

In general, the role of some additives and passivators in improving PCE, Jsc, Voc, and FF of the different perovskite solar cells since 2019 is summarized in Table 1. Their role in improving the chemical, mechanical and thermal stability of the device is also noticed as the foremost merit.

Table 1 Comparative summary of OIPSCs in the presence of additives/passivators and the reference cells

Conclusions and outlooks

Even though the power conversion efficiency of OIPSCs has been promising to go over the Shockley limitation of silicon solar cells, still their instability has been remained as a gap. Managing the factors which are causing degradation of layers, charge recombination across the interface and surface and hysteresis of OIPSCs is very crucial. Different approaches like compositional engineering, optimizing deposition techniques, solvent engineering, anti-solvent engineering, and additives/passivators engineering have been applied to abate the common problems in these devices.

Nowadays, different additives are fruitful in ameliorating poor crystallinity of the photoactive layer. They have been also applied in adjusting energy alignment between photoactive and charge transporting layers. Even if hydrophobic approaches have been leading to prevent moisture interaction, hydrophilic surface passivation which is paradoxical approach has been becoming efficient in improving moisture instability as well as PCE due to hydrogen bonding.

Degree of intra- or inter-molecular interactions between additives/passivators and photoactive or charge transporting layers or defects is determining the status of OMHPSCs stability. Accordingly, studies show that the binding energy of the atoms or ions can be used to relevant technique to determine stability of the materials or devices. Thus, detailed study on the binding energy of the different additives/passivators atoms or ions with organo-metal halide perovskites or charge transporting layers or surface defects is vital to select worthy additive to obtain homogenized and well-ordered surfaces for ease transportation of charge carriers and stable state of materials. In general, additives/passivators engineering has becoming promising strategy to look for different additives to alleviate either extrinsic or intrinsic negative impacts in OIPSCs.