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Perovskite (structure)

About: Perovskite (structure) is a research topic. Over the lifetime, 51482 publications have been published within this topic receiving 1541750 citations.


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TL;DR: The self-powered, flexible, 360 ° omnidirectional perovskite PD, featuring high detectivity and responsivity along with real-world sensing capability, suggests a new direction for next-generation optical communications, sensing, and imaging applications.
Abstract: Flexible and self-powered photodetectors (PDs) are highly desirable for applications in image sensing, smart building, and optical communications. In this paper, a self-powered and flexible PD based on the methylammonium lead iodide (CH3 NH3 PBI3 ) perovskite is demonstrated. Such a self-powered PD can operate even with irregular motion such as human finger tapping, which enables it to work without a bulky external power source. In addition, with high-quality CH3 NH3 PBI3 perovskite thin film fabricated with solvent engineering, the PD exhibits an impressive detectivity of 1.22 × 1013 Jones. In the self-powered voltage detection mode, it achieves a large responsivity of up to 79.4 V mW-1 cm-2 and a voltage response of up to ≈90%. Moreover, as the PD is made of flexible and transparent polymer films, it can operate under bending and functions at 360 ° of illumination. As a result, the self-powered, flexible, 360 ° omnidirectional perovskite PD, featuring high detectivity and responsivity along with real-world sensing capability, suggests a new direction for next-generation optical communications, sensing, and imaging applications.

305 citations

Journal ArticleDOI
TL;DR: Room temperature optical absorption spectra for thermally ablated films of the perovskites (AEQT)PbX(4) exhibit an exciton peak arising from the lead(II) halide sheets, along with absorption from the quaterthiophene moiety, and no evidence of the inorganic sheet excitonic transition is observed in the photoluminescence spectra.
Abstract: A quaterthiophene derivative, 5,5‘ ‘‘-bis(aminoethyl)-2,2‘:5‘,2‘ ‘:5‘ ‘,2‘ ‘‘-quaterthiophene (AEQT), has been selected for incorporation within the layered organic−inorganic perovskite structure. In addition to having an appropriate molecular shape and two tethering aminoethyl groups to bond to the inorganic framework, AEQT is also a dye and can influence the optical properties of lead(II) halide-based perovskites. Crystals of C20H22S4N2PbBr4 were grown from a slowly cooled aqueous solution containing lead(II) bromide and quaterthiophene derivative (AEQT·2HBr) salts. The new layered perovskite adopts a monoclinic (C2/c) subcell with the lattice parameters a = 39.741(2) A, b = 5.8420(3) A, c = 11.5734(6) A, β = 92.360(1)°, and Z = 4. Broad superstructure peaks are observed in the X-ray diffraction data, indicative of a poorly ordered, doubled supercell along both the a and b axes. The quaterthiophene segment of AEQT2+ is nearly planar, with a syn−anti−syn relationship between adjacent thiophene rings. Eac...

305 citations

Journal ArticleDOI
05 Mar 2009-Nature
TL;DR: Unexpected temperature-induced valence changes at the A and B sites in the A-site-ordered double perovskite LaCu3Fe4O12 are reported; the underlying intersite charge transfer is accompanied by considerable changes in the material’s structural, magnetic and transport properties.
Abstract: The introduction of 'foreign' elements into transition-metal oxides (called chemical doping) can change the valence state of the metal's cations and hence modify the physical properties of the material as a whole. These changes can be dramatic, for example causing high-temperature superconductivity in copper oxides and colossal magnetoresistance in manganese oxides. Youwen Long et al. have identified an oxide system, the perovskite LaCu3Fe4O12, in which changes in valence state occur when charge is shuffled between different cations (iron and copper) in the host structure, rather than via doping. As a result, the material can be reversibly transformed from one possessing iron in an unusually high Fe3.75+ state (partnered with fairly common Cu2+ ions) to one possessing rare Cu3+ ions. These changes are reflected in the magnetic and electronic properties of the material and, intriguingly, the material contracts slightly on being warmed through the transition. The temperature sensitivity of this effect makes it a strong candidate for technological applications. This paper identifies an oxide system where changes in valence state occur as a result of charge being shuffled between different cations in the host structure, rather than via doping, this charge transfer being sensitive to temperature. As a result, the material can be reversibly transformed from one possessing iron in an unusually high Fe3.75+ state to one possessing rare Cu3+ ions. These changes are reflected in the magnetic and electronic properties of the material and, intriguingly, are accompanied by negative thermal expansion. Changes of valence states in transition-metal oxides often cause significant changes in their structural and physical properties1,2. Chemical doping is the conventional way of modulating these valence states. In ABO3 perovskite and/or perovskite-like oxides, chemical doping at the A site can introduce holes or electrons at the B site, giving rise to exotic physical properties like high-transition-temperature superconductivity and colossal magnetoresistance3,4. When valence-variable transition metals at two different atomic sites are involved simultaneously, we expect to be able to induce charge transfer—and, hence, valence changes—by using a small external stimulus rather than by introducing a doping element. Materials showing this type of charge transfer are very rare, however, and such externally induced valence changes have been observed only under extreme conditions like high pressure5,6. Here we report unusual temperature-induced valence changes at the A and B sites in the A-site-ordered double perovskite LaCu3Fe4O12; the underlying intersite charge transfer is accompanied by considerable changes in the material’s structural, magnetic and transport properties. When cooled, the compound shows a first-order, reversible transition at 393 K from LaCu2+3Fe3.75+4O12 with Fe3.75+ ions at the B site to LaCu3+3Fe3+4O12 with rare Cu3+ ions at the A site. Intersite charge transfer between the A-site Cu and B-site Fe ions leads to paramagnetism-to-antiferromagnetism and metal-to-insulator isostructural phase transitions. What is more interesting in relation to technological applications is that this above-room-temperature transition is associated with a large negative thermal expansion.

305 citations

Journal ArticleDOI
TL;DR: In this paper, the perovskite-type oxides SrCo0.8B'0.2O3−σ (with B'=Cr, Fe, Co and Cu) and La0.6Sr0.4CoO3 −δ are presented.

304 citations

Journal ArticleDOI
TL;DR: In this article, the open circuit voltages are modulated by chemical doping of CsSnI3 with Br leading to formation of CsnI3-xBrx (0 ≤ x ≤ 3) perovskites.
Abstract: Replacement of lead in the hybrid organic–inorganic perovskite solar cells invokes the need for non-toxic materials such as Sn. Although solution processed CsSnI3 has been demonstrated as a lead-free halide perovskite which can function as a light absorber with high photocurrent densities, the power conversion efficiencies were bottlenecked by low open circuit voltages. In this work, the open circuit voltages are modulated by chemical doping of CsSnI3 with Br leading to formation of CsSnI3-xBrx (0 ≤ x ≤ 3) perovskites. The beneficial effect of Br incorporation for Voc improvement is evident for CsSnI3 system even without the addition of SnF2. There is an evolution of the crystal structure of CsSnI3 from orthorhombic to cubic for CsSnBr3 accompanied by changes in its optical properties with a blue shift of the absorption and IPCE onset, as the Br– doping is increased. The Voc enhancement is attributed to the decrease in Sn vacancies which is reflected by the lower charge carrier densities of 1015 cm–3 and ...

304 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
20235,193
20229,857
20216,144
20205,859
20195,498
20184,741