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SCAPS-1D Simulation of Various Hole Transport Layers' Impact on CsPbI₂Br Perovskite Solar Cells Under Indoor Low-Light Conditions
Chih-Hsi Peng,
Yi-Cheng Lin
Posted: 13 May 2025
Photosensitization of TiO2 with Copper for the Photodegradation of Organic Pollutants in Water
Dafne Rubi Porras-Herrera,
Debany Yulissa Rincón-Salazar,
María Teresa Maldonado-Sada,
José Adalberto Castillo-Robles,
Carlos Adrián Calles-Arriaga,
Enrique Rocha-Rangel
Posted: 12 May 2025
DFT Study of Hydrostatic Pressure Effects up to 1.0 GPa on the Electronic and Magnetic Properties of Laves Phases ErAl₂ and ErNi2
T. López-Solenzal,
J.L. Sanchez Llamazares,
J.L. Enríquez-Carrejo,
C.F. Sánchez-Valdés
Posted: 12 May 2025
Design and Energy Spectrum Performance Optimization of a Portable Gamma Detector Based on Perovskite Materials
Yuanxiang Feng
Posted: 12 May 2025
Probing Phase Transitions and Interfacial Reorganization in Tapc/Cbp/BPhen OLED Stacks by In Situ Ellipsometry
Ilze Aulika,
Patricija Paulsone,
Sven Oras,
Jelena Butikova,
Margarita Anna Zommere,
Elina Laizane,
Aivars Vembris
Posted: 15 April 2025
Advances in the Fabrication and Magnetic Properties of Heusler Alloy Glass-Coated Microwires with high Curie Temperature
Mohamed Salaheldeen,
Valentina Zhukova,
Juan Mari Blanco,
Julian Gonzalez,
Arcady Zhukov
Posted: 15 April 2025
Fano Resonance Sensing with Ultra-High Q Based on Bound States in the Continuum in All-Dielectric Metasurface
Haoning Sun,
Hui Deng,
Jiawei Zhang,
Tongsheng Xia,
Xiangfen Wang
Posted: 11 April 2025
Chiral-Plasmonic Hybrid Nanostructures for Sensing and Optical Computing Applications Based on Controlled Optical Binding
Ada John
Posted: 03 April 2025
Enhancing Optical Repulsion in Nano-Dimers Through Tailored Background Media and Wave Engineering
Billy Elly
Posted: 02 April 2025
A Facile Microwave-Assisted Hydrothermal (MAH) Method of CdWO4/CdMoO4 Heterostructures and Their Photocatalytic Properties
Nivaldo Freire Andrade Neto,
Onecima B.M. Ramalho,
Marcio D. Teodoro,
Mauricio R. D. Bomio,
Fabiana V. Motta
Posted: 28 March 2025
Flexible Glass: Myth and Photonic Technology
Giancarlo C. Righini,
Maurizio Ferrari,
Anna Lukowiak,
Guglielmo Macrelli
Posted: 04 March 2025
Towards Machine Learning Assisted Discovery of Organic Topological Materials
Muhammad Usman
Posted: 03 March 2025
Recent Developments of Advanced Broadband Photodetectors Based on 2D Materials
Yan Tian,
Hao Liu,
Jing Li,
Fei Liu,
Baodan Liu
Posted: 12 February 2025
The Promise of Lead-free Perovskites: Can They Replace Toxic Alternatives in Solar Cells and Lead the Future?
Dilshod Nematov,
Iskandar Raufov,
Anushervon Ashurov,
Sakhidod Sattorzoda,
Tehron Najmiddinov,
Saidjon Nazriddinzoda,
Mufazala Umarzoda,
Khonumgul Yusupova
Posted: 12 February 2025
Multipurpose X-Ray Stage and Its Application for In-Situ Poling Studies
Antonio Iacomini,
Davide Sanna,
Marzia Mureddu,
Laura Caggiu,
Costantino Cau,
Stefano Enzo,
Edgar Eduardo Villalobos-Portillo,
Lorena Pardo,
Sebastiano Garroni
Posted: 06 February 2025
Fullerene-Passivated Methylammonium Lead Iodide Perovskite Absorber for High-Performance Self-Powered Photodetectors with Ultrafast Response and Broadband Detectivity
Lakshmi Praba,
Yoseob Chung,
Dong Han Kim,
Jae Woong Jung
We herein report enhanced electrical properties of the self-powered perovskite-based photodetectors with high sensitivity and responsivity by applying surface passivation strategy using C60 (fullerene) as a surface passivating agent. The perovskite (CH3NH3PbI3) thin film passivated with the fullerene achieves highly uniform and compact surface, showing reduced leakage current and higher photon-to-current conversion capability. As a result, the improved film quality of the peorvksite layer allows excellent photon-detecting properties including high values of external quantum efficiency (> 95%), responsivity ( > 5 A W−1), and specific detectivity (> 1013 Jones) at zero bias voltage, which surpasses those of the pristine perovskite-based device. Furthermore, the passivated device showed fast rise (0.18 μs) and decay times (17 μs), demonstrating high performance and ultrafast light-detecting capability of the self-powered perovskite-based photodetectors.
We herein report enhanced electrical properties of the self-powered perovskite-based photodetectors with high sensitivity and responsivity by applying surface passivation strategy using C60 (fullerene) as a surface passivating agent. The perovskite (CH3NH3PbI3) thin film passivated with the fullerene achieves highly uniform and compact surface, showing reduced leakage current and higher photon-to-current conversion capability. As a result, the improved film quality of the peorvksite layer allows excellent photon-detecting properties including high values of external quantum efficiency (> 95%), responsivity ( > 5 A W−1), and specific detectivity (> 1013 Jones) at zero bias voltage, which surpasses those of the pristine perovskite-based device. Furthermore, the passivated device showed fast rise (0.18 μs) and decay times (17 μs), demonstrating high performance and ultrafast light-detecting capability of the self-powered perovskite-based photodetectors.
Posted: 04 February 2025
Potentials-Based Computer Modelling of Lanthanide Doped Mixed Metal Fluorides and Oxides for Optical Applications
Robert Adam Jackson
Posted: 15 January 2025
Effects of CH3NH3PbI3 Perovskite Films Crystal Structure on Solar Cell Performances
Qian Wang,
Molang Cai,
Jianfei Gao,
Xiaoxu Sun,
Haokai Zhao,
Wenjun Wang,
John Bell,
Songyuan Dai
Posted: 10 January 2025
Effect of the Position of a Phenyl Group on the Luminescent and TNP-Sensing Properties of Cationic Iridium(III) Complexes
Xiaoran Yang,
Jiahao Du,
Rui Cai,
Chun Liu
Three cationic Ir(III) complexes 1, 2, and 3 were successfully synthesized and characterized by tuning the position of a phenyl group at the pyridyl moiety in 2-phenylpyridine. All three complexes exhibit typical aggregation-induced phosphorescence emission (AIPE) properties in CH3CN/H2O. The AIPE property was further utilized to achieve highly sensitive detection of 2,4,6-trinitrophenol (TNP) in aqueous media with low limits of detection (LOD) of 164, 176, and 331 nM, respectively. This suggests that the different positions of the phenyl group influence the effectiveness of 1, 2, and 3 in the detection of TNP. In addition, 1, 2, and 3 showed superior selectivity and anti-interference for the detection of TNP and the potential to detect TNP in practical applications. Taking 1 as an example, the changes in the luminescent lifetime and UV-Vis absorption spectra of 1 before and after the addition of TNP, indicate that the quenching process is a combination of static and dynamic quenching. Additionally, the proton nuclear magnetic resonance spectra and spectral studies show that the detection mechanism is photo-induced electron transfer (PET).
Three cationic Ir(III) complexes 1, 2, and 3 were successfully synthesized and characterized by tuning the position of a phenyl group at the pyridyl moiety in 2-phenylpyridine. All three complexes exhibit typical aggregation-induced phosphorescence emission (AIPE) properties in CH3CN/H2O. The AIPE property was further utilized to achieve highly sensitive detection of 2,4,6-trinitrophenol (TNP) in aqueous media with low limits of detection (LOD) of 164, 176, and 331 nM, respectively. This suggests that the different positions of the phenyl group influence the effectiveness of 1, 2, and 3 in the detection of TNP. In addition, 1, 2, and 3 showed superior selectivity and anti-interference for the detection of TNP and the potential to detect TNP in practical applications. Taking 1 as an example, the changes in the luminescent lifetime and UV-Vis absorption spectra of 1 before and after the addition of TNP, indicate that the quenching process is a combination of static and dynamic quenching. Additionally, the proton nuclear magnetic resonance spectra and spectral studies show that the detection mechanism is photo-induced electron transfer (PET).
Posted: 19 December 2024
Straightforward Determination of the Average Electron-Hole Distance in Charge-Transfer States Organic Photovoltaic Donor/Acceptor Composites from Out-of-Phase Electron Spin Echo Data
Anna G. Matveeve,
Victoria N. Syryamina,
Vyacheslav N. Nekrasov,
Ekaterina A. Lukina,
Ivan A. Molchanov,
Vitalii I. Sysoev,
Leonid V. Kulik
Photoinduced charge separation at donor-acceptor composites (active layer material of organic solar cells) is an important step of photoelectric energy conversion. It results in formation of the interfacial charge-transfer state (CTS), which is Coulombically bound electron-hole pair. We developed the mathematical procedure of direct quantification of the electron-hole distance on the basis of time-domain pulse electron paramagnetic resonance data, obtained in electron spin echo (ESE) experiment. For an ensemble of CTSs characterized by distribution of electron-hole distance this procedure derives the average electron-hole distance without numerical simulation of the experimental data, which is a superposition of the oscillating functions, corresponding to CTSs with the certain electron-hole distance. This procedure was tested on model distance distributions, yielding very accurate results. The data for highly efficient organic photovoltaic composite PM6/Y6 were also analyzed; the average electron-hole distance within the CTS and its dependence on temperature were determined. This procedure can be useful for tracing small changes in CTS structure during optimization of the donor-acceptor composite morphology, which is tightly related to photovoltaic efficiency of the composite.
Photoinduced charge separation at donor-acceptor composites (active layer material of organic solar cells) is an important step of photoelectric energy conversion. It results in formation of the interfacial charge-transfer state (CTS), which is Coulombically bound electron-hole pair. We developed the mathematical procedure of direct quantification of the electron-hole distance on the basis of time-domain pulse electron paramagnetic resonance data, obtained in electron spin echo (ESE) experiment. For an ensemble of CTSs characterized by distribution of electron-hole distance this procedure derives the average electron-hole distance without numerical simulation of the experimental data, which is a superposition of the oscillating functions, corresponding to CTSs with the certain electron-hole distance. This procedure was tested on model distance distributions, yielding very accurate results. The data for highly efficient organic photovoltaic composite PM6/Y6 were also analyzed; the average electron-hole distance within the CTS and its dependence on temperature were determined. This procedure can be useful for tracing small changes in CTS structure during optimization of the donor-acceptor composite morphology, which is tightly related to photovoltaic efficiency of the composite.
Posted: 06 December 2024
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