14488-45-0Relevant academic research and scientific papers
Structure and function relationships in alkylammonium lead(II) iodide solar cells
Safdari, Majid,Fischer, Andreas,Xu, Bo,Kloo, Lars,Gardner, James M.
, p. 9201 - 9207 (2015)
Alkylammonium lead(ii) iodide materials (APbI3), based on the general formula of CH3-(CH2)n-NH3PbI3, may lead to a monumental leap in developing affordable photovoltaics. Herein, we correlate the structure and function relationships of alkylammonium lead(ii) iodide in solar cells. We investigated changes in the structure of APbI3 materials by varying the alkylammonium cations in their structure. As the size of the alkylammonium cation increased, the crystallographic unit cell increased in size and yielded lower symmetry crystals. High symmetry materials, those with cubic symmetry, showed the highest conductivity, the smallest bandgap, and produced the best performing solar cells. Structural changes were investigated by X-ray crystallography, X-ray powder diffraction, and Raman scattering.
From 2D to 1D Electronic Dimensionality in Halide Perovskites with Stepped and Flat Layers Using Propylammonium as a Spacer
Hoffman, Justin M.,Che, Xiaoyang,Sidhik, Siraj,Li, Xiaotong,Hadar, Ido,Blancon, Jean-Christophe,Yamaguchi, Hisato,Kepenekian, Mika?l,Katan, Claudine,Even, Jacky,Stoumpos, Constantinos C.,Mohite, Aditya D.,Kanatzidis, Mercouri G.
, p. 10661 - 10676 (2019)
Two-dimensional (2D) hybrid halide perovskites are promising in optoelectronic applications, particularly solar cells and light-emitting devices (LEDs), and for their increased stability as compared to 3D perovskites. Here, we report a new series of structures using propylammonium (PA+), which results in a series of Ruddlesden-Popper (RP) structures with the formula (PA)2(MA)n-1PbnI3n+1 (n = 3, 4) and a new homologous series of step-like (SL) structures where the PbI6 octahedra connect in a corner- and face-sharing motif with the general formula (PA)2m+4(MA)m-2Pb2m+1I7m+4 (m = 2, 3, 4). The RP structures show a blue-shift in bandgap for decreasing n (1.90 eV for n = 4 and 2.03 eV for n = 3), while the SL structures have an even greater blue-shift (2.53 eV for m = 4, 2.74 eV for m = 3, and 2.93 eV for m = 2). DFT calculations show that, while the RP structures are electronically 2D quantum wells, the SL structures are electronically 1D quantum wires with chains of corner-sharing octahedra insulated by blocks of face-sharing octahedra. Dark measurements for RP crystals show high resistivity perpendicular to the layers (1011 ω cm) but a lower resistivity parallel to them (107 ω cm). The SL crystals have varying resistivity in all three directions, confirming both RP and SL crystals' utility as anisotropic electronic materials. The RP structures show strong photoresponse, whereas the SL materials exhibit resistivity trends that are dominated by ionic transport and no photoresponse. Solar cells were made with n = 3 giving an efficiency of 7.04% (average 6.28 ± 0.65%) with negligible hysteresis.
PHOTOELECTRIC CONVERSION ELEMENT, SOLAR CELL, AND COMPOSITION
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Paragraph 0304; 0306, (2018/04/26)
Provided are a photoelectric conversion element, a solar cell using the photoelectric conversion element, and a composition. The photoelectric conversion element includes a first electrode including a photosensitive layer, which includes a light absorbing agent, on a conductive support. The light absorbing agent includes a compound having a perovskite-type crystal structure that includes organic cations represented by the following Formulae (1) and (2), a cation of a metal atom, and an anion. [in-line-formulae]R1—N(R1a)3+??Formula (1)[/in-line-formulae] [in-line-formulae]R2—N(R2a)3+??Formula (2)[/in-line-formulae] In Formulae (1) and (2), R1 represents a specific group such as an alkyl group (including a specific substituent group in a case where the number of carbons is 1 or 2), and a cycloalkyl group. R2 represents a methyl group, an ethyl group, and the like. R1a and R2a represent a specific group such as a hydrogen atom and an alkyl group.
