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At least 19 records

The Role of SnO2 Processing on Ionic Distribution in Double-Cation-Double Halide Perovskites

Moving toward a future of efficient, accessible, and less carbon-reliant energy devices has been at the forefront of energy research innovations for the past 30 years. Metal-halide perovskite (MHP) thin films have gained significant attention due to their flexibility of device applications and tunable capabilities for improving power conversion efficiency. Serving as a gateway to optimize device performance, consideration must be given to chemical synthesis processing techniques. Therefore, how does common substrate processing techniques influence the behavior of MHP phenomena such as ion migration and strain? Here, we demonstrate how a hybrid approach of chemical bath deposition (CBD) and nanoparticle SnO2 substrate processing significantly improves the performance of (FAPbI3)0.97(MAPbBr3)0.03 by reducing micro-strain in the SnO2 lattice, allowing distribution of K+ from K-Cl treatment of substrates to passivate defects formed at the interface and produce higher current in light and dark environments. X-ray diffraction reveals differences in lattice strain behavior with respect to SnO2 substrate processing methods. Through use of conductive atomic force microscopy (c-AFM), conductivity is measured spatially with MHP morphology, showing higher generation of current in both light and dark conditions for films with hybrid processing. Additionally, time-of-flight secondary ionization mass spectrometry (ToF-SIMS) observed the distribution of K+ at the perovskite/SnO2 interface, indicating K+ passivation of defects to improve the power conversion efficiency (PCE) and device stability. We show how understanding the role of ion distribution at the SnO2 and perovskite interface can help reduce the creating of defects and promote a more efficient MHP device.

conductive atomic force microscopy↗

High Performing Inverted Flexible Perovskite Solar Cells via Solution Phase Deposition of Yttrium-Doped SnO 2 Directly on Perovskite

Solution processing of flexible perovskite solar cells (f-PSCs) provides an avenue for scalable, high-throughput printing of lightweight, scalable, and cost-effective flexible solar cells. However, the deposition of fully solution-processed metal oxide charge transport layers on perovskites has been limited by solvent incompatibilities and high processing temperatures for metal oxide nanoparticles. In this study, we present high-performance, inverted f-PSCs from the direct deposition of yttrium doped SnO 2 nanoparticles functionalized with acetate on top of perovskite as an ink in anhydrous ethanol via blade coating. Yttrium doping improved device performance by improving the charge extraction leading with a decreased series resistance leading to improvements in the open-circuit voltage and fill factor. Furthermore, the champion power conversion efficiency for 0.1 cm 2 devices increased from 14.3% for undoped SnO 2 to 18.2% with 2% Y:SnO 2 doping, which is unprecedented for f-PSCs on ITO-PET substrate employing SnO 2 as an ETL.

14 SOLAR ENERGY↗

A compendium and meta-analysis of flatband potentials for TiO2, ZnO, and SnO2 semiconductors in aqueous media

Semiconductor/electrolyte interfaces are of great interest to numerous scientific fields including renewable energy, (photo)electrochemistry, and energy storage. The semiconductor flatband potential is a key parameter in locating the conduction band minimum or valence band maximum of the semiconductor material in electrolyte. Despite its importance for quantifying the energetic location of the semiconductor bands, literature reports for the same material demonstrate significant variability in the flatband potential. In this compendium and meta-analysis, reported flatband potentials of the common semiconductor materials TiO2, SnO2, and ZnO in aqueous electrolyte were compiled and assessed to quantify the spread in literature flatband potentials as well as determine the factors that lead to the significant spread. For TiO2, SnO2, and ZnO, literature flatband potentials referenced to the reversible hydrogen electrode span a range of nearly 2 V each. Flatband potential tabulations were separated by variables such as the solution pH, the crystalline polymorph, the crystal facet, the morphology, and the dimensions or combinations of these variables to assess the factors that contribute to the observed spread. Important and surprising findings from these categorizations are summarized: (1) Even for the narrowest categorizations, the spread in flatband potential is still large. (2) Flatband potentials of TiO2 and SnO2 follow the expected Nernstian dependence with solution pH. ZnO materials deviate from this Nernstian dependence. (3) In the aggregate, there is no statistically significant difference in the reported flatband potentials of anatase and rutile TiO2. Single crystal tabulations were the only distributions to have statistically significant differences in the flatband potential between anatase and rutile TiO2. (4) Anatase TiO2 materials with a nanotube morphology appear to have a +400 mV difference in mean flatband potential compared to all other morphologies, but we argue that this is likely due to widespread misuse of the Mott–Schottky analysis. Other interesting findings are revealed within the spread of literature flatband potentials, and possible explanations are provided to generate discussion. We also briefly review and discuss common techniques that were used to determine the flatband potential and the pitfalls/criticisms of these techniques. Last, we discuss some ways in which future research on the determination of the flatband potential can be performed to improve the reliability of reported values and the quality of the work. In total, the results from this meta-analysis suggest multiple factors can affect the measured flatband potential and that an abundance of caution should be applied when attempting to quantify the flatband potential of complex or nanostructured systems.

Patel, Milan Y. (ORCID:0000000291948141)↗

Materials Data on SnO2 by Materials Project

SnO2 is Hydrophilite-like structured and crystallizes in the orthorhombic Pbcn space group. The structure is three-dimensional. Sn4+ is bonded to six equivalent O2- atoms to form a mixture of corner and edge-sharing SnO6 octahedra. The corner-sharing octahedra tilt angles range from 52–54°. There are a spread of Sn–O bond distances ranging from 2.07–2.14 Å. O2- is bonded in a distorted trigonal planar geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Fluorite structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sn4+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Sn–O bond lengths are 2.23 Å. O2- is bonded to four equivalent Sn4+ atoms to form a mixture of corner and edge-sharing OSn4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Hydrophilite structured and crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. Sn4+ is bonded to six equivalent O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are four shorter (2.09 Å) and two longer (2.10 Å) Sn–O bond lengths. O2- is bonded in a trigonal planar geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Hydrophilite-like structured and crystallizes in the orthorhombic Pbcn space group. The structure is three-dimensional. there are two inequivalent Sn4+ sites. In the first Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedra tilt angles range from 51–53°. There are three shorter (2.09 Å) and three longer (2.10 Å) Sn–O bond lengths. In the second Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedra tilt angles range from 51–53°. There are a spread of Sn–O bond distances ranging from 2.06–2.13 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Sn4+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the third O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Rutile structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Sn4+ is bonded to six equivalent O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 51°. All Sn–O bond lengths are 2.09 Å. O2- is bonded in a trigonal planar geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 crystallizes in the cubic Pa-3 space group. The structure is three-dimensional. Sn4+ is bonded to six equivalent O2- atoms to form corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 60°. All Sn–O bond lengths are 2.11 Å. O2- is bonded in a trigonal planar geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is beta Vanadium nitride-like structured and crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Sn4+ is bonded to six equivalent O2- atoms to form a mixture of distorted corner and edge-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 27°. There are four shorter (2.09 Å) and two longer (2.10 Å) Sn–O bond lengths. O2- is bonded in a distorted T-shaped geometry to three equivalent Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Na(SnO2)2 by Materials Project

Na(SnO2)2 is Spinel structured and crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Na1+ is bonded to four equivalent O2- atoms to form NaO4 tetrahedra that share corners with twelve equivalent SnO6 octahedra. The corner-sharing octahedral tilt angles are 61°. All Na–O bond lengths are 2.35 Å. Sn+3.50+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent NaO4 tetrahedra and edges with six equivalent SnO6 octahedra. All Sn–O bond lengths are 2.20 Å. O2- is bonded to one Na1+ and three equivalent Sn+3.50+ atoms to form a mixture of distorted edge and corner-sharing ONaSn3 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Cyanogen Chloride-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is zero-dimensional and consists of two tin;dihydrate molecules. Sn4+ is bonded in a linear geometry to two equivalent O2- atoms. Both Sn–O bond lengths are 1.83 Å. O2- is bonded in a single-bond geometry to one Sn4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 is Hydrophilite-like structured and crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are four inequivalent Sn4+ sites. In the first Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are a spread of Sn–O bond distances ranging from 2.06–2.14 Å. In the second Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are a spread of Sn–O bond distances ranging from 2.07–2.15 Å. In the third Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are a spread of Sn–O bond distances ranging from 2.06–2.15 Å. In the fourth Sn4+ site, Sn4+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing SnO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are a spread of Sn–O bond distances ranging from 2.07–2.15 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the sixth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the seventh O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the eighth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y(SnO2)2 by Materials Project

Y(SnO2)2 is Spinel structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Y3+ is bonded to four O2- atoms to form YO4 tetrahedra that share corners with twelve SnO6 octahedra. The corner-sharing octahedra tilt angles range from 52–61°. There are one shorter (2.09 Å) and three longer (2.23 Å) Y–O bond lengths. There are two inequivalent Sn+2.50+ sites. In the first Sn+2.50+ site, Sn+2.50+ is bonded to six O2- atoms to form SnO6 octahedra that share corners with six equivalent YO4 tetrahedra and edges with six SnO6 octahedra. There are two shorter (2.45 Å) and four longer (2.55 Å) Sn–O bond lengths. In the second Sn+2.50+ site, Sn+2.50+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent YO4 tetrahedra and edges with six equivalent SnO6 octahedra. All Sn–O bond lengths are 2.15 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Y3+ and three Sn+2.50+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Y3+ and three equivalent Sn+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Al(SnO2)2 by Materials Project

Al(SnO2)2 is Spinel structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with twelve SnO6 octahedra. The corner-sharing octahedra tilt angles range from 46–54°. There is one shorter (1.76 Å) and three longer (1.86 Å) Al–O bond length. There are two inequivalent Sn+2.50+ sites. In the first Sn+2.50+ site, Sn+2.50+ is bonded to six O2- atoms to form distorted SnO6 octahedra that share corners with six equivalent AlO4 tetrahedra and edges with six SnO6 octahedra. There are two shorter (2.45 Å) and four longer (2.51 Å) Sn–O bond lengths. In the second Sn+2.50+ site, Sn+2.50+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent AlO4 tetrahedra and edges with six equivalent SnO6 octahedra. All Sn–O bond lengths are 2.16 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Al3+ and three Sn+2.50+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Al3+ and three equivalent Sn+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Al(SnO2)2 by Materials Project

Al(SnO2)2 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Al3+ is bonded in a square co-planar geometry to four O2- atoms. All Al–O bond lengths are 1.85 Å. There are two inequivalent Sn+2.50+ sites. In the first Sn+2.50+ site, Sn+2.50+ is bonded in a square co-planar geometry to four O2- atoms. There are two shorter (2.18 Å) and two longer (2.29 Å) Sn–O bond lengths. In the second Sn+2.50+ site, Sn+2.50+ is bonded in a square co-planar geometry to four O2- atoms. There are two shorter (2.09 Å) and two longer (2.22 Å) Sn–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Al3+ and two Sn+2.50+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Al3+ and two Sn+2.50+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Ca(SnO2)2 by Materials Project

Ca(SnO2)2 is Spinel structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Ca2+ is bonded to four equivalent O2- atoms to form CaO4 tetrahedra that share corners with twelve equivalent SnO6 octahedra. The corner-sharing octahedral tilt angles are 59°. All Ca–O bond lengths are 2.31 Å. Sn3+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent CaO4 tetrahedra and edges with six equivalent SnO6 octahedra. All Sn–O bond lengths are 2.30 Å. O2- is bonded to one Ca2+ and three equivalent Sn3+ atoms to form a mixture of distorted edge and corner-sharing OCaSn3 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on SnO2 by Materials Project

SnO2 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are twelve inequivalent Sn4+ sites. In the first Sn4+ site, Sn4+ is bonded to six O2- atoms to form edge-sharing SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.10–2.15 Å. In the second Sn4+ site, Sn4+ is bonded to six O2- atoms to form edge-sharing SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.10–2.15 Å. In the third Sn4+ site, Sn4+ is bonded to four O2- atoms to form corner-sharing SnO4 tetrahedra. The corner-sharing octahedra tilt angles range from 55–61°. There are a spread of Sn–O bond distances ranging from 1.96–2.03 Å. In the fourth Sn4+ site, Sn4+ is bonded to six O2- atoms to form SnO6 octahedra that share corners with three SnO4 tetrahedra and edges with four SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.01–2.18 Å. In the fifth Sn4+ site, Sn4+ is bonded to six O2- atoms to form edge-sharing SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.10–2.15 Å. In the sixth Sn4+ site, Sn4+ is bonded to four O2- atoms to form corner-sharing SnO4 tetrahedra. The corner-sharing octahedra tilt angles range from 54–62°. There are a spread of Sn–O bond distances ranging from 1.95–2.03 Å. In the seventh Sn4+ site, Sn4+ is bonded to six O2- atoms to form SnO6 octahedra that share corners with six SnO4 tetrahedra and edges with two equivalent SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.03–2.16 Å. In the eighth Sn4+ site, Sn4+ is bonded to four O2- atoms to form corner-sharing SnO4 tetrahedra. The corner-sharing octahedra tilt angles range from 53–61°. There are a spread of Sn–O bond distances ranging from 1.95–2.03 Å. In the ninth Sn4+ site, Sn4+ is bonded to six O2- atoms to form SnO6 octahedra that share corners with three SnO4 tetrahedra and edges with four SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.01–2.17 Å. In the tenth Sn4+ site, Sn4+ is bonded to four O2- atoms to form corner-sharing SnO4 tetrahedra. The corner-sharing octahedra tilt angles range from 55–62°. There is two shorter (1.96 Å) and two longer (2.02 Å) Sn–O bond length. In the eleventh Sn4+ site, Sn4+ is bonded to six O2- atoms to form edge-sharing SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.10–2.15 Å. In the twelfth Sn4+ site, Sn4+ is bonded to six O2- atoms to form edge-sharing SnO6 octahedra. There are a spread of Sn–O bond distances ranging from 2.10–2.14 Å. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the sixth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the seventh O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the eighth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the ninth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the tenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Sn4+ atoms. In the eleventh O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the twelfth O2- site, O2- is bonded in a bent 120 degrees geometry to two Sn4+ atoms. In the thirteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the fourteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the fifteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the sixteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the seventeenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Sn4+ atoms. In the eighteenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Sn4+ atoms. In the nineteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the twentieth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the twenty-first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms. In the twenty-second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the twenty-third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Sn4+ atoms. In the twenty-fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Sn4+ atoms.

36 MATERIALS SCIENCE↗