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Representation of THz spectroscopy of a metamaterial with a Nanowire THz sensor

Representation of THz spectroscopy of a metamaterial with a Nanowire THz sensor

Credit: Rendering by Dimitars Jevtics

Prof Michael Johnston

Professor of Physics

Research theme

  • Photovoltaics and nanoscience

Sub department

  • Condensed Matter Physics

Research groups

  • Terahertz photonics
  • Advanced Device Concepts for Next-Generation Photovoltaics
michael.johnston@physics.ox.ac.uk
Johnston Group Website
  • About
  • Publications

Coated Spintronic Emitters for Improved THz Time-domain Spectroscopy

Institute of Electrical and Electronics Engineers (IEEE) 00 (2023) 1-2

Authors:

Ford M Wagner, Simas Melnikas, Joel Cramer, Djamshid A Damry, Chelsea Q Xia, Kun Peng, Gerhard Jakob, Mathias Kläui, Simonas Kičas, Michael B Johnston
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Nanowire-based THz polarimetry

Institute of Electrical and Electronics Engineers (IEEE) 00 (2023) 1-2
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Nanowires in Terahertz Photonics: Harder, Better, Stronger, Faster

Institute of Electrical and Electronics Engineers (IEEE) 00 (2023) 1-1

Authors:

Hannah J Joyce, Stephanie O Adeyemo, Srabani Kar, Jamie D Lake, Chawit Uswachoke, Chennupati Jagadish, H Hoe Tan, Yunyan Zhang, Huiyun Liu, Jessica L Boland, Djamshid Damry, Michael B Johnston
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Synergistic surface modification of tin-lead perovskite solar cells

Advanced Materials Wiley 35:9 (2023) 2208320

Authors:

Shuaifeng Hu, Pei Zhao, Kyohei Nakano, Robert DJ Oliver, Jorge Pascual, Joel A Smith, Takumi Yamada, Minh Anh Truong, Richard Murdey, Nobutaka Shioya, Takeshi Hasegawa, Masahiro Ehara, Michael B Johnston, Keisuke Tajima, Yoshihiko Kanemitsu, Henry J Snaith, Atsushi Wakamiya

Abstract:

Interfaces in thin-film photovoltaics play a pivotal role in determining device efficiency and longevity. Herein, we study the top surface treatment of mixed tin-lead (∼1.26 eV) halide perovskite films for p-i-n solar cells. We are able to promote charge extraction by treating the perovskite surface with piperazine. This compound reacts with the organic cations at the perovskite surface, modifying the surface structure and tuning the interfacial energy level alignment. In addition, the combined treatment with C<sub>60</sub> pyrrolidine tris-acid (CPTA) reduces hysteresis and leads to efficiencies up to 22.7%, with open-circuit voltage values reaching 0.90 V, ∼92% of the radiative limit for the band gap of this material. The modified cells also show superior stability, with unencapsulated cells retaining 96% of their initial efficiency after >2000 hours of storage in N<sub>2</sub> and encapsulated cells retaining 90% efficiency after >450 hours of storage in air. Intriguingly, CPTA preferentially binds to Sn<sup>2+</sup> sites at film surface over Pb<sup>2+</sup> due to the energetically favoured exposure of the former, according to first-principles calculations. This work provides new insights into the surface chemistry of perovskite films in terms of their structural, electronic, and defect characteristics and we use this knowledge to fabricate state-of-the-art solar cells.
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Thermally stable perovskite solar cells by all-vacuum deposition

ACS Applied Materials and Interfaces American Chemical Society 15:1 (2022) 772-781

Abstract:

Vacuum deposition is a solvent-free method suitable for growing thin films of metal halide perovskite (MHP) semiconductors. However, most reports of high-efficiency solar cells based on such vacuum-deposited MHP films incorporate solution-processed hole transport layers (HTLs), thereby complicating prospects of industrial upscaling and potentially affecting the overall device stability. In this work, we investigate organometallic copper phthalocyanine (CuPc) and zinc phthalocyanine (ZnPc) as alternative, low-cost, and durable HTLs in all-vacuum-deposited solvent-free formamidinium-cesium lead triodide [CH(NH2)2]0.83Cs0.17PbI3 (FACsPbI3) perovskite solar cells. We elucidate that the CuPc HTL, when employed in an “inverted” p–i–n solar cell configuration, attains a solar-to-electrical power conversion efficiency of up to 13.9%. Importantly, unencapsulated devices as large as 1 cm2 exhibited excellent long-term stability, demonstrating no observable degradation in efficiency after more than 5000 h in storage and 3700 h under 85 °C thermal stressing in N2 atmosphere.

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