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Abstract:

The copper–silver–bismuth–iodide compound Cu2AgBiI6 has emerged as a promising lead-free and environmentally friendly alternative to wide-bandgap lead-halide perovskites for applications in multijunction solar cells. Despite its promising optoelectronic properties, the efficiency of Cu2AgBiI6 is still severely limited by poor charge collection. Here, we investigate the impact of commonly used charge transport layers (CTLs), including poly­[bis­(4-phenyl)­(2,4,6-trimethylphenyl)­amine] (PTAA), CuI, [6,6]-phenyl-C61-butyric acid methyl ester (PCBM), and SnO2, on the structural and optoelectronic properties of coevaporated Cu2AgBiI6 thin films. We reveal that while organic transport layers, such as PTAA and PCBM, form a relatively benign interface, inorganic transport layers, such as CuI and SnO2, induce the formation of unintended impurity phases within the CuI–AgI–BiI3 solid solution space, significantly influencing structural and optoelectronic properties. We demonstrate that identification of these impurity phases requires careful cross-validation combining absorption, X-ray diffraction and THz photoconductivity spectroscopy because their structural and optoelectronic properties are very similar to those of Cu2AgBiI6. Our findings highlight the critical role of CTLs in determining the structural and optoelectronic properties of coevaporated copper–silver–bismuth–iodide thin films and underscore the need for advanced interface engineering to optimize device efficiency and reproducibility.

Abstract:

The rise of metal halide perovskites has prompted a revolution in optoelectronics research [1]. Yet a comprehensive understanding of the vertical charge transport that underlies the soaring efficiencies of perovskite-based solar cells has remained challenging owing to the materials' nanocrystalline structure [2] and competing crystal phases [3]. Here, we simultaneously probe the intrinsic out-of-plane charge-carrier diffusion and the nanoscale morphology by pushing depth-sensitive terahertz near- field nano-spectroscopy [4] to extreme subcycle timescales [5]. Evanescent terahertz fields at the apex of a metallic tip probe ultrafast dynamics of photocarriers in $\text{FA}_{0}.{}_{83}\text{Cs}_{0.17}\text{Pb}(\mathrm{I}_{1}{}_{-\mathrm{x}}\mathrm{C}1_{\mathrm{x}})_{3}$ films with nanoscale spatial resolution (Fig. 1 a). By analysing characteristic phonon signatures in the spectral response, we distinguish domains of the photo active cubic $\alpha$ -phase from the trigonal δ-phase and $\text{PbI}_{2}$ nano-islands (Fig. 1 b). To examine the impact of these nanoscale inhomogeneities on carrier dynamics, we monitor the peak pump-induced signal as a function of pump delay time $t_{\mathrm{p}}$ (Fig. 1c). Notably, the full pump-induced waveforms at different $t_{\mathrm{p}}$ (Fig. 1d) show a deeply subcycle time shift $\Delta t$, which can be microscopically linked to a diffusion-driven change in the vertical carrier distribution with $t_{\mathrm{r}}$ (Fig. 1e, inset). Com-bining a straightforward rate equation model with the finite-dipole model, we extract the evolution of the out-of-plane carrier density profile from $\Delta t$ (Fig. 1e). Mapping the out-of-plane diffusion coefficient $D$ along a line across different grains, including $\alpha$ -phase grains and $\text{PbI}_{2}$ contaminations, we find a homogeneous value of $D=(0.2\pm 0.1)\ \text{cm}^{2}\mathrm{s}^{-1}$, which is surprisingly immune to compositional and structural variations (Fig. 1 f). This robustness of vertical diffusion may contribute to the exceptional performance of perovskite-based devices. Linking in situ carrier transport with nanoscale morphology and chemical composition could introduce a paradigm shift for the analysis and optimization of next-generation optoelectronics that are based on nanocrystalline materials.

Abstract:

Copper is one of the most extensively studied materials for energy conversion and catalytic systems, with a wide range of other applications, from nanophotonics to biotechnology. However, existing synthesis methods are limited with many undesirable byproducts and poorly defined morphologies. Here, we report an on-substrate wet synthesis approach that yields purely metallic and monocrystalline Cu microflakes with an exposed (111) crystalline surface. By systematically studying the growth mechanism, we achieve unprecedented sizes of more than 130 mu m, which is 2 orders of magnitude larger than reported in most previous studies, along with high aspect ratios of over 400. Furthermore, we show significantly higher stability against oxidation provided by the halide adlayer, which also eliminates the need for any organic surfactants in the synthesis. Overall, our facile synthesis approach delivers an exciting avenue for the emerging fields of catalysis and nanophotonics.LNE

Abstract:

The perovskite semiconductor, CsPbI3, holds excellent promise for solar cell applications due to its suitable bandgap. However, achieving phase‐stable CsPbI3 solar cells with high power conversion efficiency remains a major challenge. Ruddlesden–Popper (RP) defects have been identified in a range of perovskite semiconductors, including CsPbI3. However, there is limited understanding as to why they form or their impact on stability and photophysical properties. Here, the prevalence of RP defects is increased with increased Cs‐excess in vapor‐deposited CsPbI3 thin films while superior structural stability but inferior photophysical properties are observed. Significantly, using electron microscopy, it is found that the atomic positions at the planar defect are comparable to those of a free surface, revealing their role in phase stabilization. Density functional theory (DFT) calculations reveal the RP planes are electronically benign, however, antisites observed at RP turning points are likely to be malign. Therefore it is proposed that increasing RP planes while reducing RP turning points offers a breakthrough for improving both phase stability and photophysical performance. The formation mechanism revealed here can apply more generally to RP structures in other perovskite systems.