Dec 5, 2024
8:00pm - 10:00pm
Hynes, Level 1, Hall A
Kyle McCall1,Kulatheepan Thanabalasingam1,2,Mihir Singh1,2
The University of Texas at Dallas1,University of Texas at Dallas2
Halide perovskites are next-generation photovoltaic candidates due to their remarkable properties, such as defect tolerance, low thermal conductivity, and efficient light emission, which arise in part from the structural dynamics and disorder of the crystal lattice. However, the limits of this disorder are unclear – that is, how far can the perovskite structure be stretched while maintaining similar properties? The 2D Ruddlesden-Popper perovskites (RPs), A
n+1B
nX
3n+1, are quasi-2D <100> structure variants of 3D perovskites where B
+ ion occupies in corner-connected octahedra in
ab plane, while A
+ ions space out the layers. Here, we study inorganic and hybrid mixed-anion 2D RP materials to understand the structure-property relationship and gain insights into the origin of their optical properties. In this presentation, we report the synthesis, crystal structure, and optical properties of two novel RPs, Cs
2CdI
2Cl
2 and MA
2CdI
2Cl
2 (MA = methylammonium).
All-inorganic Cs
2CdI
2Cl
2 crystals were grown using a solvothermal reaction in a 1:1 HCl and HI mixture, while the hybrid MA
2CdI
2Cl
2 was grown using a hydrothermal reaction in distilled water with a few drops of hypophosphorous acid and followed by slow evaporation crystallization. Powder X-ray diffraction of Cs
2CdI
2Cl
2 and Rietveld refinement confirm that the material crystallizes in the tetragonal
I4/
mmm space group. This is the highest allowable symmetry for Ruddlesden-Popper perovskites, and is isostructural with Rb
2CdI
2Cl
2, Cs
2SnI
2Cl
2, and Cs
2PbI
2Cl
2 analogues. This series is thus ideal for probing the impact of A and B site variation in these mixed-anion compounds, which host heteroleptic coordination of the B site with both I and Cl ions. On the other hand, MA
2CdI
2Cl
2 crystallizes in the orthorhombic
Fmm2 space group, confirmed by single crystal X-ray diffraction. The octahedral units of this structure are tilted due to the orientation of the MA cation in the void, causing the reduction in symmetry. Photoluminescence of Cs
2CdI
2Cl
2 shows a broad yellow emission centered at 570 nm with 340 nm excitation. Comparison of these new 2D RPs with the known compounds Rb
2CdI
2Cl
2 and Cs
2PbI
2Cl
2, which have exhibited broadband emission and photoconductivity, respectively, will enable us to connect structural features, including the presence or absence of a lone pair, with optical properties to close the structure-property relationship loop. In this presentation, we will discuss the synthesis and crystal growth of these materials, their crystal structures, and their optical properties measured by photoluminescence and UV-Vis absorption spectra.