Rheological Tunability of Perovskite Precursor Solutions: From Spin Coating to Inkjet Printing Process

The high efficiencies (>22%) reached by perovskite-based optoelectronic devices in a very short period, demonstrates the great potential and tunability of this material. The current challenge lies in translating such efficiencies to commercially feasible forms produced through industrial fabrication methods. Herein, a novel first step towards the processability of starch-perovskite inks, developed in our previous work, is investigated, by using inkjet printing technology. The tunability of the viscosity of the starch-perovskite-based inks allows the selection of suitable concentrations to be used as printable inks. After exploration of several printing parameters, thick and opaque starch-perovskite nanocomposite films were obtained, showing interesting morphological and optical properties. The results obtained in this work underline the potential and versatility of our approach, opening the possibility to explore and optimize, in the future, further large-scale deposition methods towards fully printed and stable perovskite devices.


Introduction
Inkjet printing, traditionally used in the graphics and publishing industries, has proven to be an effective digital manufacturing technique for printed solar cells [1]. In this direction, the emergence of organic-inorganic hybrid perovskite solar cells has represented a breakthrough technology, combining solution-based deposition techniques with greater efficiencies than organic solar cells [1].
However, one of the most important challenges now for perovskite-based materials is improving stability and reproducibility during fabrication, particularly by translating the high performance obtained at laboratory scale to industrial fabrication methods [2][3][4].
Among the different potential techniques for depositing perovskite-based materials and other functional layers of a solar energy device, inkjet printing is one of the most frequently used on a laboratory scale due to its versatility and selectivity in the fabrication of functional layers from solutions Nanomaterials 2019, 9, 582 3 of 12

Poly-TPD Solution Preparation
The solution of poly-TPD (1.5 mg/mL in chlorobenzene) was prepared by stirring at 40 • C for 2 h.

Starch-Perovskite Solution Preparation
The perovskite precursor solution containing an equimolar precursor stoichiometry, i.e., MAI:PbI 2 = 1:1, was prepared by mixing MAI with PbI 2 in DMSO with varying precursor weight concentrations in DMSO, i.e., 10-20-30 wt%, as reported in Table 1. The solutions were stirred on a hot plate at 80 • C for 30 min. After precursor solubilization, different starch/precursor ratios were added to each solution, i.e., 1, 5, 10, and 15 wt%, and were stirred at 80 • C for 5 h in order to obtain a clear solution after starch solubilization. The identification name (ID) of each sample with the correspondent precursors and starch concentrations are reported in Table 1.

Rheological Characterization of Perovskite Precursors Solutions
The viscosity of the perovskite precursor solutions by varying the precursor concentrations in DMSO from 5 to 30 wt% and with a starch/precursor ratio from 1 to 15 wt%, was carried out in a strain controlled rheometer (Malvern Kinexus Pro+, Malvern, UK) equipped by parallel plate geometry (radius = 12.5 mm) in steady state mode with a shear rate ranging from 1-1000 s −1 at 23 • C. All the liquid formulations were tested after stirring at 80 • C for 5 h and cooled to ambient temperature. This was in order to better understand the influence of precursor and starch concentrations on the viscosity of the as-prepared perovskite solutions before deposition. The rheological experiments were repeated three times to check the repeatability of the results.

Surface Tension
The surface tension of the inks was measured by Krüss DSA100 (Bristol, UK) using the pendant drop method.

Inkjet Printing Process
Patterns of 5 mm × 5 mm with various print resolutions were designed using the open source software, GIMP (The General Image Manipulation Program, Spencer Kimball, Peter Mattis, 2.10.8 version, Berkeley, CA, USA). The files were saved as bitmap (.bmp) image file format and opened with Dimatix drop manager (Fujifilm, Santa Clara, CA, USA) in order to be loaded by the printer software.
The printing frequency was set at 5.0 kHz and a customized waveform was used. The voltage and the temperature of the cartridge were optimized based on the ink explored. The printing process was carried out in air with a humidity of 20-30%. The temperature of the substrate was optimized during the process through print platform heating. The diameters of the printed drops were analyzed to optimize the drop spacing of each explored ink.
The substrate was prepared by washing the glass slide with isopropanol. Then, the poly-TPD solution (1.5 mg/mL in clorobenzene) was printed at room temperature by using the same customized waveform with a drop spacing of 60 µm (distance between droplets center to center) and a voltage of 23 V. Printed poly-TPD was annealed in air at 140 • C for 30 min, followed by UV treatment of 30 min in order to improve the wettability, as already demonstrated in our previous paper [2].

Morphological Characterization
The surface morphology of the single droplets printed and of the printed starch-perovskite composite samples was analyzed by an optical microscope (Nikon Eclipse-LV100ND, Tokyo, Japan). Scanning electron microscopy (SEM) images of the printed starch-perovskite composite samples, deposited on a glass/printed poly-TPD substrate, were collected by using Carl Zeiss Auriga 40 Crossbeam instrument (Oberkochen, Germany), in high vacuum and high-resolution acquisition mode, equipped with Gemini column and an integrated high efficiency in-lens detector. The applied acceleration voltage was 5 kV.

XRD Measurements
Wide-angle X-ray diffraction (XRD) patterns were obtained in reflection geometry by an automated Bruker D8 Advance diffractometer (Billerica, MA, USA), equipped with nickel-filtered Cu Kα radiation (1.5418 Å) as the X-ray source that was operated at 35 kV and 40 mA.

UV-vis Absorption
UV-visible optical absorption spectra were recorded on Varian Cary 500 spectrophotometer (Agilent, Santa Clara, CA, USA) in the 200-800 nm wavelength range at room temperature. Steady state and time resolved photoluminescence (PL) was measured by an Edinburgh FLS920 spectrometer (Livingstone, UK) equipped with a Peltier-cooled Hamamatsu R928 photomultiplier tube (185-850 nm). An Edinburgh Xe900 450 W Xenon arc lamp (Livingstone, UK) was used as exciting light source. Corrected spectra were obtained via a calibration curve supplied with the instrument (lamp power in the steady state PL experiments~0.6 mW cm −2 , spot area 0.5 cm 2 ). Emission lifetimes were determined with the single photon counting technique by means of the same Edinburgh FLS980 spectrometer (Livingstone, UK), using a laser diode as excitation source (1 MHz, λ exc = 635 nm, 67 ps pulse width, and about 30 ps time resolution after deconvolution) and a Hamamatsu MCP R3809U-50 (time resolution 20 ps) as detector (laser power in the time resolution photoluminescence (TRPL) experiment~1.6 W cm -2 , spot area 0.3 mm 2 ) [15].

Results and Discussion
The printability of the starch-perovskite-based inks [2] was explored with the aim to evaluate the possibility to deposit them through large scale methods. The printability of a solution can be defined by the Z parameter that is directly dependent on viscosity, surface tension, and density of the ink [16][17][18]. Therefore, these properties were, firstly, evaluated in order to select the solutions more suitable for ink jet printing technology. Figure 1 showed the steady state viscosity of the different solutions investigated, including a wide range of perovskite precursor concentrations from 5 to 30 wt% and starch/precursor concentrations from 0 to 15 wt%. All the perovskite precursor formulations, without starch, showed a Newtonian behavior with almost constant viscosity ranges from~0.002 to~0.007 Pa s by increasing the precursors content. By increasing the starch content, at lower perovskite precursor concentrations, i.e., 5 and 10 wt%, the solutions still showed a Newtonian behavior, with an increased viscosity up to~0.01 Pa s. By increasing the perovskite precursors ratio to 20 and 30 wt%, a pseudoplastic behavior was observed in the presence of starch content higher than 5 wt%. Nanomaterials 2019, 9, x FOR PEER REVIEW 5 of 13

Photoluminescence (PL) Experiments
Steady state and time resolved photoluminescence (PL) was measured by an Edinburgh FLS920 spectrometer (Livingstone, UK) equipped with a Peltier-cooled Hamamatsu R928 photomultiplier tube (185-850 nm). An Edinburgh Xe900 450 W Xenon arc lamp (Livingstone, UK) was used as exciting light source. Corrected spectra were obtained via a calibration curve supplied with the instrument (lamp power in the steady state PL experiments ~0.6 mW cm −2 , spot area 0.5 cm 2 ). Emission lifetimes were determined with the single photon counting technique by means of the same Edinburgh FLS980 spectrometer (Livingstone, UK), using a laser diode as excitation source (1 MHz, λexc = 635 nm, 67 ps pulse width, and about 30 ps time resolution after deconvolution) and a Hamamatsu MCP R3809U-50 (city, country, time resolution 20 ps) as detector (laser power in the time resolution photoluminescence (TRPL) experiment ~1.6 W cm -2 , spot area 0.3 mm 2 ) [15].

Results and Discussion
The printability of the starch-perovskite-based inks [2] was explored with the aim to evaluate the possibility to deposit them through large scale methods. The printability of a solution can be defined by the Z parameter that is directly dependent on viscosity, surface tension, and density of the ink [16][17][18]. Therefore, these properties were, firstly, evaluated in order to select the solutions more suitable for ink jet printing technology. Figure 1 showed the steady state viscosity of the different solutions investigated, including a wide range of perovskite precursor concentrations from 5 to 30 wt% and starch/precursor concentrations from 0 to 15 wt%. All the perovskite precursor formulations, without starch, showed a Newtonian behavior with almost constant viscosity ranges from ~0.002 to ~0.007 Pa s by increasing the precursors content. By increasing the starch content, at lower perovskite precursor concentrations, i.e., 5 and 10 wt%, the solutions still showed a Newtonian behavior, with an increased viscosity up to ~0.01 Pa s. By increasing the perovskite precursors ratio to 20 and 30 wt%, a pseudoplastic behavior was observed in the presence of starch content higher than 5 wt%. The starch used for the solutions was widely characterized in our previous work [14], as well as its role as a rheological modifier [2], with the interesting discovery that the gelatinization process of the starch into DMSO together with the interaction between the OH groups of the starch and the perovskite precursors highly influences the rheological behavior of the solutions. Interestingly, the results of the rheological characterization showed that by tuning the concentration of the precursors and of the starch, it is possible to obtain a solution with rheological properties suitable to the The starch used for the solutions was widely characterized in our previous work [14], as well as its role as a rheological modifier [2], with the interesting discovery that the gelatinization process of the starch into DMSO together with the interaction between the OH groups of the starch and the perovskite precursors highly influences the rheological behavior of the solutions. Interestingly, the results of the rheological characterization showed that by tuning the concentration of the precursors and of the starch, it is possible to obtain a solution with rheological properties suitable to the deposition technology used. By decreasing the perovskite precursor ratio down to 5-10 wt%, we were able to move from spin coating to ink jet printing of perovskite-starch deposition. Together with the viscosity, the surface tension and the density of the inks are key parameters to investigate the "ejectability" of a solution. In general, values between 20-40 mN/m are considered more suitable for ink jet printing processes, lower than the surface tension values reported in Table 2 for the solutions with varying perovskite precursors, from 5 to 10 wt%, and starch content from 0 to 10 wt%. The respective densities, calculated by weighing a known volume of each solution, were reported in Table 2, together with the Z value calculated by Equation (1).
where η is the dynamic viscosity, ρ is the density, γ is the surface tension, a is the characteristic length (usually the nozzle diameter) of the ink. The solution containing the 5 wt% of perovskite precursor in solvent showed a surface tension of 44.24 ± 0.15 mN/m, close to the solvent used for the solution, DMSO (45.25 ± 0.47 mN/m). In the presence of starch, as well as with a higher precursor concentration, the surface tension increases up to about 53 mN/m. As reported in Table 2, Z values decreased by increasing the starch content, driven by the increased viscosity, and were much lower for the ink containing 10 wt% of precursors, showing a good influence of the presence of the starch on the ink ejectability calculated from Z. Indeed, Z values between 1 and 10 are more suitable for ink jet printing technology, even though the value of a printable Z number is still under investigation [19][20][21].
Subsequently, the ejectability of the inks was experimentally investigated by applying several customized waveforms to the nozzle of the cartridge and by optimizing the voltage and the temperature applied to obtain a drop ejected from the nozzle, as shown in Figure 2.
After optimization of the previous parameters, interesting results were obtained for most of the inks reported in Table 1, by setting the voltage of the piezoelectric driven print-heads at each nozzle at 23 V and the temperature of the print-head at 23 • C. On the other hand, for the formulations containing higher starch concentration, 5MAPbI 3 -10S, 10MAPbI 3 -5S, and 10MAPbI 3 -10S, higher voltage and temperature were necessary to allow the ejection of the ink from the nozzle, i.e., 30 V and 40 • C, and 40 V and 45 • C, respectively. This latter result was probably due to the combination of higher surface tension and viscosity, despite the lower Z parameter calculated. It is interesting to observe that the shape and the length of the drop were highly influenced by the concentration of starch. In detail, increasing starch molecular concentration lead to a longer drop tail due to greater long chain content, typical of polymers with high molecular weight-based solutions [22].
showing a good influence of the presence of the starch on the ink ejectability calculated from Z. Indeed, Z values between 1 and 10 are more suitable for ink jet printing technology, even though the value of a printable Z number is still under investigation [19][20][21].
Subsequently, the ejectability of the inks was experimentally investigated by applying several customized waveforms to the nozzle of the cartridge and by optimizing the voltage and the temperature applied to obtain a drop ejected from the nozzle, as shown in Figure 2.  Figure 3 shows single droplets of the perovskite inks deposited on printed and annealed poly-TPD by varying perovskite precursors and starch concentrations, before thermal treatment. It is evident that the size of the drops increases from about 48.9 ± 4.9 µm for 5 wt% and 52.8 ± 1.3 µm for 10 wt%, in absence of starch, up to 61.2 ± 0.4 µm and 66.2 ± 1.3 µm, respectively, after adding 10 wt% of the biopolymer. Moreover, the presence of the starch allows for a more compact and homogeneous drop on the substrate to be obtained, which is a key aspect in order to realize a good photoactive film. After optimization of the previous parameters, interesting results were obtained for most of the inks reported in Table 1, by setting the voltage of the piezoelectric driven print-heads at each nozzle at 23 V and the temperature of the print-head at 23 °C. On the other hand, for the formulations containing higher starch concentration, 5MAPbI3-10S, 10MAPbI3-5S, and 10MAPbI3-10S, higher voltage and temperature were necessary to allow the ejection of the ink from the nozzle, i.e., 30 V and 40 °C, and 40 V and 45 °C, respectively. This latter result was probably due to the combination of higher surface tension and viscosity, despite the lower Z parameter calculated. It is interesting to observe that the shape and the length of the drop were highly influenced by the concentration of starch. In detail, increasing starch molecular concentration lead to a longer drop tail due to greater long chain content, typical of polymers with high molecular weight-based solutions [22]. Figure 3 shows single droplets of the perovskite inks deposited on printed and annealed poly-TPD by varying perovskite precursors and starch concentrations, before thermal treatment. It is evident that the size of the drops increases from about 48.9 ± 4.9 μm for 5 wt% and 52.8 ± 1.3 μm for 10 wt%, in absence of starch, up to 61.2 ± 0.4 μm and 66.2 ± 1.3 μm, respectively, after adding 10 wt% of the biopolymer. Moreover, the presence of the starch allows for a more compact and homogeneous drop on the substrate to be obtained, which is a key aspect in order to realize a good photoactive film. From droplet to pattern printing, there are several aspects to consider; first, the choice of a proper drop space, in order to have the appropriate overlapping of the droplets, which is essential to obtain a continuous pattern. Hence, drop size is a crucial parameter and depends on the ink, wettability of the substrate, and surface temperature as well. As the diameter of the print head nozzle is fixed, the droplet overlap is controlled by increasing or decreasing the resolution of the image (dpi) of the pattern [23].
By considering the average drop size of the different inks tested, a drop space of 30 μm was firstly selected to be used for printing continuous patterns. In addition, several annealing temperatures, from 80 to 110 °C, were explored for printed perovskite precursor films and shown in From droplet to pattern printing, there are several aspects to consider; first, the choice of a proper drop space, in order to have the appropriate overlapping of the droplets, which is essential to obtain a continuous pattern. Hence, drop size is a crucial parameter and depends on the ink, wettability of the substrate, and surface temperature as well. As the diameter of the print head nozzle is fixed, the droplet overlap is controlled by increasing or decreasing the resolution of the image (dpi) of the pattern [23].
By considering the average drop size of the different inks tested, a drop space of 30 µm was firstly selected to be used for printing continuous patterns. In addition, several annealing temperatures, from 80 to 110 • C, were explored for printed perovskite precursor films and shown in Figure 4a.  All of the films annealed at 80 and 100 °C resulted in a needle-like morphology organized in smaller islands, by increasing the temperature and the starch content (at fixed temperature). After annealing at 110 °C, a more compact morphology was observed, irrespective of the starch content, suggesting that the rate of the solvent evaporation is a key point during perovskite film formation; by increasing the annealing temperature, then the rate of DMSO evaporation, a better perovskite grain morphology could be obtained. However, a "shift" of the drops was observed during thermal annealing, leading to a non-homogeneous perovskite film, as shown in the pictures in Figure 4b, which was more evident as the starch content decreased.
Furthermore, with the aim to overcome the crystallization issue by increasing the solvent evaporation rate, and to better control the uniformity of the printed pattern, the perovskite precursor-based inks containing 5 and 10 wt% of precursors and 5 wt% of starch were printed on a hot substrate at 90 and 100 °C. As shown in the optical images reported in Figure 5, for both of the concentrations explored, a higher temperature of the substrate enabled a morphology characterized by perovskite grains, whereas a needles-like structure was observed by depositing the 5 wt% of starch perovskite at 90 °C. Therefore, 100 °C was selected as the best printing temperature. Moreover, a well-defined 5 × 5 mm 2 printed pattern was obtained, as shown in the inset of Figure 5. All of the films annealed at 80 and 100 • C resulted in a needle-like morphology organized in smaller islands, by increasing the temperature and the starch content (at fixed temperature). After annealing at 110 • C, a more compact morphology was observed, irrespective of the starch content, suggesting that the rate of the solvent evaporation is a key point during perovskite film formation; by increasing the annealing temperature, then the rate of DMSO evaporation, a better perovskite grain morphology could be obtained. However, a "shift" of the drops was observed during thermal annealing, leading to a non-homogeneous perovskite film, as shown in the pictures in Figure 4b, which was more evident as the starch content decreased.
Furthermore, with the aim to overcome the crystallization issue by increasing the solvent evaporation rate, and to better control the uniformity of the printed pattern, the perovskite precursor-based inks containing 5 and 10 wt% of precursors and 5 wt% of starch were printed on a hot substrate at 90 and 100 • C. As shown in the optical images reported in Figure 5, for both of the concentrations explored, a higher temperature of the substrate enabled a morphology characterized by perovskite grains, whereas a needles-like structure was observed by depositing the 5 wt% of starch perovskite at 90 • C. Therefore, 100 • C was selected as the best printing temperature. Moreover, a well-defined 5 × 5 mm 2 printed pattern was obtained, as shown in the inset of Figure 5. With the aim to improve the coverage of the substrate, the drop space was decreased from 30 to 15 μm, leading to a more compact and homogeneous film, as shown in Figure 6 for 10MAPbI3-5S perovskite ink. Therefore, in the following experiment, 5MAPbI3-5S and 10MAPbI3-5S were printed according to the optimized parameters and the respective films were accurately characterized and compared.
The SEM images in Figure 7a,b show a morphology characterized by large grains of about 5 μm in both samples. However, slightly larger and more compact grains were observed for 10MAPbI3-5S, combined with a smaller quantity of gaps than 5Mapi-5S film. The X-ray diffraction patterns on 5MAPbI3-5S and 10MAPbI3-5S printed film in Figure 7c display a strong peak at 14.2° of the MAPbI3 crystal. However, the presence of a small peak at 12.7°, in both of the samples, suggested the presence of unreacted PbI2 in the film, maybe due to the deposition conditions (in air, in presence of humidity). The characteristic absorption spectra of perovskite were shown for both of the concentrations explored in Figure 7d, with higher absorption intensity by increasing the precursor concentration due to the increasing thickness of the film from about 1 μm (5MAPbI3-5S) to 1.7 μm (10MAPbI3-5S). It is interesting to observe that thicker and more opaque films were achieved by With the aim to improve the coverage of the substrate, the drop space was decreased from 30 to 15 µm, leading to a more compact and homogeneous film, as shown in Figure 6 for 10MAPbI 3 -5S perovskite ink. With the aim to improve the coverage of the substrate, the drop space was decreased from 30 to 15 μm, leading to a more compact and homogeneous film, as shown in Figure 6 for 10MAPbI3-5S perovskite ink. Therefore, in the following experiment, 5MAPbI3-5S and 10MAPbI3-5S were printed according to the optimized parameters and the respective films were accurately characterized and compared.
The SEM images in Figure 7a,b show a morphology characterized by large grains of about 5 μm in both samples. However, slightly larger and more compact grains were observed for 10MAPbI3-5S, combined with a smaller quantity of gaps than 5Mapi-5S film. The X-ray diffraction patterns on 5MAPbI3-5S and 10MAPbI3-5S printed film in Figure 7c display a strong peak at 14.2° of the MAPbI3 crystal. However, the presence of a small peak at 12.7°, in both of the samples, suggested the presence of unreacted PbI2 in the film, maybe due to the deposition conditions (in air, in presence of humidity). The characteristic absorption spectra of perovskite were shown for both of the concentrations explored in Figure 7d, with higher absorption intensity by increasing the precursor concentration due to the increasing thickness of the film from about 1 μm (5MAPbI3-5S) to 1.7 μm (10MAPbI3-5S). It is interesting to observe that thicker and more opaque films were achieved by Therefore, in the following experiment, 5MAPbI 3 -5S and 10MAPbI 3 -5S were printed according to the optimized parameters and the respective films were accurately characterized and compared.
The SEM images in Figure 7a,b show a morphology characterized by large grains of about 5 µm in both samples. However, slightly larger and more compact grains were observed for 10MAPbI 3 -5S, combined with a smaller quantity of gaps than 5Mapi-5S film. The X-ray diffraction patterns on 5MAPbI 3 -5S and 10MAPbI 3 -5S printed film in Figure 7c display a strong peak at 14.2 • of the MAPbI 3 crystal. However, the presence of a small peak at 12.7 • , in both of the samples, suggested the presence of unreacted PbI 2 in the film, maybe due to the deposition conditions (in air, in presence of humidity). The characteristic absorption spectra of perovskite were shown for both of the concentrations explored in Figure 7d, with higher absorption intensity by increasing the precursor concentration due to the increasing thickness of the film from about 1 µm (5MAPbI 3 -5S) to 1.7 µm (10MAPbI 3 -5S). It is interesting to observe that thicker and more opaque films were achieved by inkjet depositing perovskite inks at low precursor concentrations of 5 and 10 wt%, when compared to conventional spin-coating [2]. Moreover, despite the high thickness, printed perovskite films are highly converted, as demonstrated by XRD patterns, which did not evidence the presence of peaks related to MAI-DMSO-PbI 2 intermediate complex (6.6 • , 7.2 • , and 9.2 • ) [24]. Nanomaterials 2019, 9, x FOR PEER REVIEW 10 of 13 inkjet depositing perovskite inks at low precursor concentrations of 5 and 10 wt%, when compared to conventional spin-coating [2]. Moreover, despite the high thickness, printed perovskite films are highly converted, as demonstrated by XRD patterns, which did not evidence the presence of peaks related to MAI-DMSO-PbI2 intermediate complex (6.6°, 7.2°, and 9.2°) [24]. Aiming at future optoelectronic applications, the optical properties of the printed films were investigated by steady-state PL measurements, as shown in Figure 8. The intense PL emission band of 10MAPbI3-5S peaks at 795 nm, and it is slightly blue, shifting to 790 nm for 5MAPbI3-5S. The emission band position and intensities are in line with what was previously reported for these composites, and suggests good optoelectronic properties for the perovskite component of the ink [25].
The time-resolved PL experiment (Figure 8b) further supports the claim of good optoelectronic properties, as the lifetimes are reasonably long (9, 52 ns for 5MAPbI3-5S; and 5, 124 ns for 10MAPbI3-5S) and suggest reduced parasite traps mediated the carrier's recombination. The role of the starch has already been proven to positively affect the optoelectronic properties of perovskite materials. Herein, the increase of the lifetime associated to a higher precursor concentration suggests better optoelectronic properties for 10MAPbI3-5S film, which could be due to an increase of the perovksite grain dimensions. Aiming at future optoelectronic applications, the optical properties of the printed films were investigated by steady-state PL measurements, as shown in Figure 8. The intense PL emission band of 10MAPbI 3 -5S peaks at 795 nm, and it is slightly blue, shifting to 790 nm for 5MAPbI 3 -5S. The emission band position and intensities are in line with what was previously reported for these composites, and suggests good optoelectronic properties for the perovskite component of the ink [25].

Conclusions
In this work, the possibility to print the starch-perovskite inks, developed in our previous work, was explored by using ink jet printing as a first step towards a more scalable deposition process of perovskite-based devices. The tunability of the viscosity of the starch-perovskite-based inks allowed us to select the suitable concentration to be used as printable inks. Through the investigation of the The time-resolved PL experiment (Figure 8b) further supports the claim of good optoelectronic properties, as the lifetimes are reasonably long (9, 52 ns for 5MAPbI 3 -5S; and 5, 124 ns for 10MAPbI 3 -5S) and suggest reduced parasite traps mediated the carrier's recombination. The role of the starch has already been proven to positively affect the optoelectronic properties of perovskite materials. Herein, the increase of the lifetime associated to a higher precursor concentration suggests better optoelectronic properties for 10MAPbI 3 -5S film, which could be due to an increase of the perovksite grain dimensions.

Conclusions
In this work, the possibility to print the starch-perovskite inks, developed in our previous work, was explored by using ink jet printing as a first step towards a more scalable deposition process of perovskite-based devices. The tunability of the viscosity of the starch-perovskite-based inks allowed us to select the suitable concentration to be used as printable inks. Through the investigation of the printing parameters, such as waveform, voltage, and temperature of piezoelectric driven print heads from one side, and drop space, substrate temperature from the other, printed perovskite films with good morphological, crystalline, and optical properties were realized. These results represent the first demonstration of the versatility of the perovskite deposition approach developed during this work, and open the possibility for further investigations towards upscaling of perovskite deposition.