Spatial positioning of nanocrystal building blocks on a solid surface is a prerequisite for assembling individual nanoparticles into functional devices. Here, we report on the graphoepitaxial liquid-solid growth of nanowires of the photovoltaic compound CH3NH3PbI3 in open nanofluidic channels. The guided growth, visualized in real-time with a simple optical microscope, undergoes through a metastable solvatomorph formation in polar aprotic solvents. The presently discovered crystallization leads to the fabrication of mm2-sized surfaces composed of perovskite nanowires having controlled sizes, cross-sectional shapes, aspect ratios and orientation which have not been achieved thus far by other deposition methods. The automation of this general strategy paves the way towards fabrication of wafer-scale perovskite nanowire thin films well-suited for various optoelectronic devices, e.g. solar cells, lasers, light-emitting diodes and photodetectors.
One-dimensional nanostructures, such as nanowires and nanotubes, represent the smallest dimension for efficient transport of electrons and excitons1. In particular, organic or solid-state nanowires, due to their unique properties as compared to their bulk counterparts, are attractive building blocks in a wide range of applications, including sensors2,3, nanoelectronics4,5, photonics6,7 and renewable energy8. Recently, a solvatomorph-mediated synthesis of hybrid halide perovskite in nanowire form, specifically methylammonium lead iodide, CH3NH3PbI3 (hereafter MAPbI3), a material that has attracted overwhelming attention, was discovered9,10,11,12. Even if very little is known concerning their liquid phase growth mechanism or their structural and photo-physical properties, elongated lead halide perovskite particles9,13 have already been successfully integrated into perovskite-based solar cells14 and ultrasensitive, micro-fabricated photodetectors15. Recently, exceptional lasing properties of solution-grown perovskite thin films16,17; and nanowires18 have been reported.
Solution-based low-temperature processes are generally recognized to be cost-effective and easy to scale-up fabrication methods. Therefore, the forecasted low fabrication cost is one of the main arguments of researchers and investors for considering organometallic halide perovskites as a promising material for the development of next-generation photovoltaics19. Despite numerous successful reports on record-breaking efficiencies it remains a major challenge to attain device-to-device reproducibility of the performance parameters, even in case of lab-scale (~20 mm2 surface area) prototypes20. Currently, the major hurdle to overcome is related to the lack of precise control of the crystal parameters, such as the crystal habit, crystallite size, crystallinity and the quality of grain boundaries on small and large scale surfaces. For instance, in polycrystalline nanoparticle-based perovskite films, the most important parameters to achieve outstanding optoelectronic performances are strongly linked to both the size and the orientation of the crystalline domains, likewise affecting the film homogeneity, area coverage, pinholes and roughness21. Similarly, the slip-coating method, i.e. our previously reported single-step approach, produces perovskite nanowires in dandelion-like organization on a flat surface.
The liquid phase growth pattern is determined by the formation of nucleation centers randomly distributed over the substrate, therefore there is little control on the area coverage, pinholes, aspect ratio and orientation of the nanowires9,15. Recently, however, we found a fairly simple approach to overcome the spatially-random surface nucleation. Therefore, here, we report on the guided growth of extremely high aspect-ratio perovskite crystalline nanowires in the arrays of open nanofluidic channels. An important feature of the observed “solvatomorph-graphoepitaxy” is that the crystallization of MAPbI3 solvatomorphs proceeds exclusively in polar aprotic solvents such as dimethylformamide (DMF), dimethylacetamide (DMAc) and dimethyl sulfoxide (DMSO), at near room temperature. Moreover, for the first time, the kinetics of the nanowire growth was visualized with a simple optical microscope in real-time. We envision that standardization of this general strategy will allow the reproducible fabrication of wafer-scale perovskite nanowire thin films with highly controlled crystallite dimensions and crystallinity. Their integration into various optoelectronic devices could help in further boosting their performances.
We show that slip-coating of saturated solution of MAPbI3 in polar aprotic solvents (i.e. DMF, DMSO and DMAc) results in the formation of perovskite nanowires organized in dandelion-like arrangement on a silicon surface. As can be seen from the optical microscopy and scanning electron microscopy (SEM) images in Fig. 1, the liquid phase growth pattern is inherently determined by the formation of nucleation centers, which are randomly distributed on the surface. Therefore, there is little control over the aspect ratio and the orientation of the nanowires. Only a very slight, shear-force-induced guidance was observed with respect to the sliding direction of the top glass plate.
MAPbI3 has been reported to be unstable in the majority of ordinary solvents, including water and to decompose at moderate temperatures (~400 K) in addition22,23. Therefore, processing and precise patterning by post-growth assembly techniques such as dielectrophoresis24, Langmuir-Blodgett self-assembly25 and mechanical shear1 seems to be a challenging task. Unlike the above mentioned multi-step post-growth assembly techniques, here, we combine a bottom-up nanofluidic alignment with a top-down surface patterning technique to achieve both the synthesis and oriented assembly of elongated MAPbI3 crystallites in a single step. The nanowires were crystallized in the arrays of nanofabricated channels owing to the strong guiding effect of the nano-grooves26. Similar guiding effects have already been observed for chemical vapor deposited (vapor-liquid-solid grown, VLS) grown gallium nitride (GaN) nanowires27. The phenomenon of the alignment induced by the intimate epitaxial relationship has been discovered four decades ago and it has been named “graphoepitaxy”28,29,30. In a typical experiment, we dropped a supersaturated solution of MAPbI3 dissolved in DMF onto the arrays of nanostructured trenches etched in a SiO2 substrate (Fig. 2a). Next, capillary forces drove the liquid inside the channels with a speed proportional to the channel width31 (Fig. 2b). At this point, the first defects and etching-induced crystallographic imperfections of the channel wall triggered the heterogeneous nucleation of a yellow, so far barely studied clathrate phase of MAPbI3-DMF. This crystalline, translucent-yellow precipitate contained the mother liquor, that is a polar aprotic solvent (e.g. DMF, DMSO and DMAc). Therefore, it can be regarded as a solvatomorph phase (i.e. metastable precursor phase) of the MAPbI3 perovskite. Unlike MAPbI3 itself, this solvatomorph phase does not show the characteristic photo-luminescence under excitation with the green monochromatic incoherent light (λex = 546 nm) (Fig. S4). Interestingly, neither the solvatomorph formation nor the guided growth was observed with gamma-Butyrolactone (GBL), another commonly used solvent in solution based perovskite thin films preparation. This partially explains the enigma of the highly-anisotropic crystallization of cubic or tetragonal phases of the perovskite. Actually, the anisotropic crystal growth is specific to the metastable translucent-yellow colored solvatomorph phase, formed by the host-guest interaction (solvatomorph formation) of MAPbI3 with polar aprotic solvents (MAPbI3-DMF, MAPbI3-DMSO and MAPbI3-DMAc). It is important to realize, that these are metastable precursor compounds, hence the final MAPbI3 perovskite phase is formed by a subsequent solvent evaporation-induced recrystallization of the solvatomorph phase, which is equivalent to the dehydration processes observed for instance in many oxo-hydroxo compounds (Fig. 2g,h). The analysis of the time-lapse videos recorded in an optical microscope provided insight into the nanowire formation mechanism and also added another simple tool to study the kinetics of growth and dissolution (Fig. 2, Fig. S6, video S1). We have found, that the crystallization follows the classical solvent evaporation-induced supersaturation-driven crystallization. The most important parameters controlling the growth rate are the surface-normalized concentration of the MAPbI3 solution, as well as the temperature and the surface tension of the solvent. In the first approximation, stable clusters and nuclei of MAPbI3-DMF solvatomorph form in the channel entrances, thus acting as foreign particles (Fig. 2e). The subsequent nanowire growth, dilutes the liquid, hence shifts the solution to an undersaturated condition (Fig. 2f). This is expected to slow down the kinetics and ultimately stop the precipitation of the solute. However, the solvent evaporation from the open nanofluidic channel acts on the opposite way, it concentrates the solution, maintaining the supersaturation condition in equilibrium (Fig. 2g). Furthermore, the capillary forces as well as the concentration difference-induced diffusion of the solute toward the growing crystal plane, i.e. the growing end of the wire, play a fundamental role in crystal growth. When the continuous supply of the solute and/or the mother liquor is blocked the supersaturation is exhausted, the nanowire growth stops (Fig. 2c). The synthesis process ends when all the mother liquor escapes from the metastable clathrate phase (MAPbI3-DMF) formed by the polar aprotic solvent. Nanoscale crystallite dimensions allow the solvent to escape without inducing significant shrinkage-induced cracks or damage in the crystal habit. Ultimately, the precursor phase transforms to the final, grey-silver MAPbI3 phase and maintaining the elongated crystal shape (Fig. 2d).
The process yields nanowires with well-defined sizes, cross-sections and spatial distributions. With this fairly simple technique, extremely long (up to few mm) and narrow (down to 10 nm) V-shaped (Fig. S2a) and rectangular-shaped cross section (Fig. S2b) nanowires have been realized along predefined nanofluidic channels. Examination of the growth process on larger length scales shows that the growth extends over millimeter length scales and seems to be limited by the length of the fluidic channel. We have carried out several experiments in order to understand the parameters controlling the crystal habit.
We have found that whereas wider, micrometer-sized channels were mostly filled with bundles of nanowires (Fig. S2d), individual nanowires tend to grow in narrower channels. This can be explained by the stochastic nature of the heterogeneous nucleation process. Narrow channels are comparable in size to the first nucleus formed, hence there is a higher probability that they contain less nucleation centers, resulting in individual elongated single crystallites (Fig. S1). In contrast, wider channels (>1 μm) contain more imperfections, where multiple nuclei can be formed, resulting in the formation of crystallographically-fused parallel aggregates of perovskite nanowires (Fig. S2d, Video S4). The crystal growth of the elongated solvatomorphs is likewise feasible in curved or zig-zag shaped nanofluidic channels (Fig. 3a). The graphoepitaxial growth is not limited to a particular inorganic substrate, hence the guided growth was similarly observed in metallic (e.g Au) as well as in organic resin (e.g. ZEP520A) based nanofluidic channels. This compositional versatility enables the fabrication of numerous patterned substrate/nanowire material combinations i.e. p-i-n lateral interdigital configurations (Fig. 3). The possible advantage of these non-conventional p-i-n architectures over the state-of-the-art planar or mesoscopic configurations is yet to be determined (Fig. S7). Interestingly, we observed guiding effects even in between non- continuous -walled channels, e.g. arrays of rectangular pillars of SiO2 or organic resin of ZEP520A (Fig. 3d,e). This implicates that the most important parameter determining the nanowire diameter might be the size of the nucleation center. Once the nanowire growth starts, the cross-section remains constant over ~cm length scales (Fig. 3g, Video S3, Video S4). This allowed us to create controlled ‘wire-to-wire’ connections by launching the wire growth on the pillar-pattered silicon surface from two directions (90o degree angle) simultaneously (Fig. 3e). In addition, the surface coverage and the film thickness can be similarly controlled by the nanofluidic channel dimensions. Importantly, all the wires were spatially confined and the minimum separation of the aligned nanowires depends solely on the resolution and precision of the applied lithographical process. By using recent electron-beam tools, this can easily be reduced below 50 nm. Accordingly, the channel width and its periodicity will control the area coverage of a given film, with the film thickness being linearly proportional to the channel height.
As an example, we fabricated series of perovskite nanowire based photodetector devices using e-beam lithography (Fig. 4e). The longitudinal composite devices were composed of lithographically patterned graphene sensitized by a perovskite nanowire active layer (Fig. 4a,b). Recently we have reported on the fabrication of similar devices attaining remarkable responsivities (2.6 × 106 AW−1) under pW light intensities. Here, the hybrid devices prepared by the graphoepitaxial liquid-solid growth of aligned, millimeter-long nanowires of MAPbI3 in open nanofluidic channels showed similar linearI-V characteristics, with characteristic response times of 2–5 seconds (Fig. 4d). The best devices reached responsivities as high as 6 × 106 AW−1 (Fig. 4e). The drastic enhancement of the responsivity at very low light intensities (pW) could enable MAPbI3 nanowire/graphene devices for use as low-light imaging sensors and single photon detectors. We attribute these very high device performances mainly to the controlled growth of perovskite nanowires in predefined positions. Our results demonstrate an important step in the integration of perovskite nanowires in arrays of microfabricated optoelectronic devices with high reproducibility. The process allows the synthesis of extremely long (~cm) and thin (~few nm) nanowires with a morphology defined by the shape of nanostructured open fluidic channels. Moreover, optimized spacing, shape and size in the periodic pattern may result in large-area, wafer-scale superstructures with advantageous optical properties for photonic, optoelectronic, radio-frequency and non-linear optic applications. Ultimately, the graphoepitaxial nanowire growth enables well-engineered angular restriction designs, which can improve the photon reabsorption process and thus maximize the performance of perovskite nanowire based optoelectronic device32. This low temperature solution growth method, unique in its gender opens an entirely new spectrum of architectural design of organometal halide perovskite based optoelectronic devices.
How to cite this article: Spina, M. et al. Controlled growth of CH3NH3PbI3 nanowires in arrays of open nanofluidic channels. Sci. Rep.6, 19834; doi: 10.1038/srep19834 (2016).
Huang, Y., Duan, X., Wei, Q. & Lieber, C. M. Directed Assembly of One-Dimensional Nanostructures into Functional Networks. Science 291, 630–633 (2001).
McAlpine, M. C., Ahmad, H., Wang, D. & Heath, J. R. Highly ordered nanowire arrays on plastic substrates for ultrasensitive flexible chemical sensors. Nat. Mater. 6, 379–384 (2007).
Yang, D., Kang, K., Kim, D., Li, Z. & Park, I. Fabrication of heterogeneous nanomaterial array by programmable heating and chemical supply within microfluidic platform towards multiplexed gas sensing application. Sci. Rep. 5, 8149 (2015).
Yan, H. et al. Programmable nanowire circuits for nanoprocessors. Nature 470, 240–244 (2011).
Shulaker, M. M. et al. Carbon nanotube computer. Nature 501, 526–530 (2013).
Yan, R., Gargas, D. & Yang, P. Nanowire photonics. Nat. Photonics 3, 569–576 (2009).
Johnson, J. C. et al. Single gallium nitride nanowire lasers. Nat. Mater. 1, 106–110 (2002).
Tétreault, N. et al. High-Efficiency Solid-State Dye-Sensitized Solar Cells: Fast Charge Extraction through Self-Assembled 3D Fibrous Network of Crystalline TiO2 Nanowires. ACS Nano 4, 7644–7650 (2010).
Horváth, E. et al. Nanowires of Methylammonium Lead Iodide (CH3NH3PbI3) Prepared by Low Temperature Solution-Mediated Crystallization. Nano Lett. 14, 6761–6766 (2014).
Kojima, A., Teshima, K., Shirai, Y. & Miyasaka, T. Organometal Halide Perovskites as Visible-Light Sensitizers for Photovoltaic Cells. J. Am. Chem. Soc. 131, 6050–6051 (2009).
Im, J.-H., Lee, C.-R., Lee, J.-W., Park, S.-W. & Park, N.-G. 6.5% efficient perovskite quantum-dot-sensitized solar cell. Nanoscale 3, 4088–4093 (2011).
Kim, H.-S. et al. Lead Iodide Perovskite Sensitized All-Solid-State Submicron Thin Film Mesoscopic Solar Cell with Efficiency Exceeding 9%. Sci. Rep. 2, 591 (2012).
Zhang, D., Eaton, S. W., Yu, Y., Dou, L. & Yang, P. Solution-Phase Synthesis of Cesium Lead Halide Perovskite Nanowires. J. Am. Chem. Soc. 137, 9230–9233 (2015).
Im, J.-H. et al. Nanowire Perovskite Solar Cell. Nano Lett. 15, 2120–2126 (2015).
Spina, M. et al. Microengineered CH3NH3PbI3 Nanowire/Graphene Phototransistor for Low-Intensity Light Detection at Room Temperature. Small 11, 4824–4828 (2015).
Saba, M. et al. Correlated electron–hole plasma in organometal perovskites. Nat. Commun. 5, 5049 (2014).
Sutherland, B. R., Hoogland, S., Adachi, M. M., Wong, C. T. O. & Sargent, E. H. Conformal Organohalide Perovskites Enable Lasing on Spherical Resonators. ACS Nano 8, 10947–10952 (2014).
Zhu, H. et al. Lead halide perovskite nanowire lasers with low lasing thresholds and high quality factors. Nat. Mater. 14, 636–642 (2015).
Antonietta Loi, M. & Hummelen, J. C. Hybrid solar cells: Perovskites under the Sun. Nat. Mater. 12, 1087–1089 (2013).
Jeon, Y.-J. et al. Planar heterojunction perovskite solar cells with superior reproducibility. Sci. Rep. 4, 6953 (2014).
Stranks, S. D., Nayak, P. K., Zhang, W., Stergiopoulos, T. & Snaith, H. J. Formation of Thin Films of Organic–Inorganic Perovskites for High-Efficiency Solar Cells. Angew. Chem. Int. Ed. 54, 3240–3248 (2015).
Leguy, A. M. A. et al. Reversible Hydration of CH3NH3PbI3 in Films, Single Crystals and Solar Cells. Chem. Mater. 27, 3397–3407 (2015).
Han, Y. et al. Degradation observations of encapsulated planar CH3NH3PbI3 perovskite solar cells at high temperatures and humidity. J. Mater. Chem. A 3, 8139–8147 (2015).
Sarker, B. K., Shekhar, S. & Khondaker, S. I. Semiconducting Enriched Carbon Nanotube Aligned Arrays of Tunable Density and Their Electrical Transport Properties. ACS Nano 5, 6297–6305 (2011).
Whang, D., Jin, S., Wu, Y. & Lieber, C. M. Large-Scale Hierarchical Organization of Nanowire Arrays for Integrated Nanosystems. Nano Lett. 3, 1255–1259 (2003).
Hellgren, N. et al. Electronic structure of carbon nitride thin films studied by X-ray spectroscopy techniques. Thin Solid Films 471, 19–34 (2005).
Ma, Z. et al. Vapor–liquid–solid growth of serrated GaN nanowires: shape selection driven by kinetic frustration. J. Mater. Chem. C 1, 7294–7302 (2013).
Geis, M. W., Tsaur, B.-Y. & Flanders, D. C. Graphoepitaxy of germanium on gratings with square‐wave and sawtooth profiles. Appl. Phys. Lett. 41, 526–529 (1982).
Givargizov, E. I. Graphoepitaxy as an approach to oriented crystallization on amorphous substrates. J. Cryst. Growth 310, 1686–1690 (2008).
Geis, M. W., Flanders, D. C. & Smith, H. I. Crystallographic orientation of silicon on an amorphous substrate using an artificial surface‐relief grating and laser crystallization. Appl. Phys. Lett. 35, 71–74 (1979).
Yang, D., Krasowska, M., Priest, C. & Ralston, J. Dynamics of capillary-driven liquid–liquid displacement in open microchannels. Phys. Chem. Chem. Phys. 16, 24473–24478 (2014).
Sha, W. E. I., Ren, X., Chen, L. & Choy, W. C. H. The efficiency limit of CH3NH3PbI3 perovskite solar cells. Appl. Phys. Lett. 106, 221104 (2015).
This work was partially supported by the Swiss National Science Foundation and ERC ADVANCED GRANT (PICOPROP#670918). Device fabrication was carried out in part in the EPFL Center for Micro/Nanotechnology (CMI).
The authors declare no competing financial interests.
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Spina, M., Bonvin, E., Sienkiewicz, A. et al. Controlled growth of CH3NH3PbI3 nanowires in arrays of open nanofluidic channels. Sci Rep 6, 19834 (2016). https://doi.org/10.1038/srep19834
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