CsPbI 3 has recently received tremendous attention as a possible absorber of perovskite solar cells (PSCs). However, CsPbI 3 -based PSCs have yet to achieve the high performance of the hybrid PSCs. In this work, we performed a density functional theory (DFT) study using the Cambridge Serial Total Energy Package (CASTEP) code for the cubic CsPbI 3 absorber to compare and evaluate its structural, electronic, and optical properties. The calculated electronic band gap ( E g ) using the GGA-PBE approach of CASTEP was 1.483 eV for this CsPbI 3 absorber. Moreover, the computed density of states (DOS) exhibited the dominant contribution from the Pb-5d orbital, and most charges also accumulated for the Pb atom as seen from the electronic charge density map. Fermi surface calculation showed multiband character, and optical properties were computed to investigate the optical response of CsPbI 3 . Furthermore, we used IGZO, SnO 2 , WS 2 , CeO 2 , PCBM, TiO 2 , ZnO, and C 60 as the electron transport layers (ETLs) and Cu 2 O, CuSCN, CuSbS 2 , Spiro-MeOTAD, V 2 O 5 , CBTS, CFTS, P3HT, PEDOT:PSS, NiO, CuO, and CuI as the hole transport layers (HTLs) to identify the best HTL/CsPbI 3 /ETL combinations using the SCAPS-1D solar cell simulation software. Among 96 device structures, the best-optimized device structure, ITO/TiO 2 /CsPbI 3 /CBTS/Au, was identified, which exhibited an efficiency of 17.9%. The effect of the absorber and ETL thickness, series resistance, shunt resistance, and operating temperature was also evaluated for the six best devices along with their corresponding generation rate, recombination rate, capacitance–voltage, current density–voltage, and quantum efficiency characteristics. The obtained results from SCAPS-1D were also compared with wxAMPS simulation results.
Different from conventional nonionic poly(oxyethylene) surfactants, poly(oxyethylene) cholesteryl ethers, ChEO n , possess a bulky and nonflexible hydrophobic part and form a variety of self-organized structures in water. We investigated the phase behavior and the micellar structures in the water/ChEO15 and water/ChEO10 systems by means of visual observation, rheometry, small-angle X-ray scattering (SAXS), dynamic light scattering (DLS), dielectric relaxation spectroscopy (DRS), and densimetry. We found that in the water/ChEO15 system, aqueous micellar (Wm), discontinuous micellar cubic (I1) with Fd3m space group, hexagonal (H1), rectangular ribbon (R1), and lamellar (Lα) phases are formed, whereas Wm, unknown, R1, defected lamellar ( ), and Lα phases are produced in the water/ChEO10 system at ambient temperatures. Compared with a conventional aqueous nonionic surfactant system, the intermediate R1 phase region is incredibly wide. As for the water/ChEO15 system, with increasing water content, the packing parameter, P, in the R1 region is gradually decreased, finally converging to 1/2 at W s ∼ 0.58, indicative of the formation of the H1 phase. The R1 phase acts as a “distorted” hexagonal phase in the system. However, in the water/ChEO10 system, upon reduction of W S, P shows a steplike increase and the maximum value ∼0.67 at W S ∼ 0.7, just corresponding to the threshold of discontinuous and bicontinuous structures. After that, P is decreased with decreasing W S and unknown phase that cannot be indexed to any known space group for liquid crystalline phases emerges at W S ∼ 0.5. The GIFT analysis of the SAXS data for the Wm solution indicates that spherical micelles are present in the water/ChEO15 system in an ambient temperature range, but ChEO10 forms a short-rod micelle in water. With increasing temperature, rodlike micelles appear to be grown and a viscoelastic micellar phase is formed in water/ChEO10 system. The hydration number for each oxyethylene unit is evaluated as ∼4 by DRS, which gives a consistent explanation for the concentration dependence of the apparent hydrodynamic radius in the Wm phase obtained by DLS. Hydrated water molecules should be regarded as a constituent of the micelles. The majority of these features of novel phase behavior in the water/ChEO n systems are based on a nonflexible and bulky hydrophobic part of ChEO n .
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