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CMP
Credit: Jack Hobhouse

Prof Henry Snaith FRS

Professor of Physics

Sub department

  • Condensed Matter Physics

Research groups

  • Snaith group
  • Advanced Device Concepts for Next-Generation Photovoltaics
Henry.Snaith@physics.ox.ac.uk
Robert Hooke Building, room G21
  • About
  • Publications

Ethylenediamine Addition Improves Performance and Suppresses Phase Instabilities in Mixed-Halide Perovskites

(2022)

Authors:

Margherita Taddei, Joel A Smith, Benjamin M Gallant, Suer Zhou, Robert JE Westbrook, Yangwei Shi, Jian Wang, James N Drysdale, Declan P McCarthy, Stephen Barlow, Seth R Marder, Henry J Snaith, David S Ginger
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Impact of hole-transport layer and interface passivation on halide segregation in mixed-halide perovskites

Advanced Functional Materials Wiley 32:41 (2022) 2204825

Authors:

Vincent JY Lim, Alexander J Knight, Robert DJ Oliver, Henry J Snaith, Michael B Johnston, Laura M Herz

Abstract:

Mixed-halide perovskites offer ideal bandgaps for tandem solar cells, but photoinduced halide segregation compromises photovoltaic device performance. This study explores the influence of a hole-transport layer, necessary for a full device, by monitoring halide segregation through in situ, concurrent X-ray diffraction and photoluminescence measurements to disentangle compositional and optoelectronic changes. This work demonstrates that top coating FA0.83Cs0.17Pb(Br0.4I0.6)3 perovskite films with a poly(triaryl)amine (PTAA) hole-extraction layer surprisingly leads to suppression of halide segregation because photogenerated charge carriers are rapidly trapped at interfacial defects that do not drive halide segregation. However, the generation of iodide-enriched regions near the perovskite/PTAA interface enhances hole back-transfer from the PTAA layer through improved energy level offsets, increasing radiative recombination losses. It is further found that while passivation with a piperidinium salt slows halide segregation in perovskite films, the addition of a PTAA top-coating accelerates such effects, elucidating the specific nature of trap types that are able to drive the halide segregation process. This work highlights the importance of selective passivation techniques for achieving efficient and stable wide-bandgap perovskite photovoltaic devices.
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In Operando, Photovoltaic, and Microscopic Evaluation of Recombination Centers in Halide Perovskite-Based Solar Cells

ACS Applied Materials & Interfaces American Chemical Society (ACS) 14:30 (2022) 34171-34179

Authors:

Arava Zohar, Michael Kulbak, Silver H Turren-Cruz, Pabitra K Nayak, Adi Kama, Anders Hagfeldt, Henry J Snaith, Gary Hodes, David Cahen
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Rapid sequestration of perovskite solar cell-derived lead in soil

Journal of Hazardous Materials Elsevier 436 (2022) 128995

Authors:

Felix Schmidt, Luca Ledermann, Andreas Schäffer, Henry J Snaith, Markus Lenz
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Long-range charge carrier mobility in metal halide perovskite thin-films and single crystals via transient photo-conductivity

Nature Communications Springer Nature 13:1 (2022) 4201

Authors:

Jongchul Lim, Manuel Kober-Czerny, Yen-Hung Lin, James M Ball, Nobuya Sakai, Elisabeth A Duijnstee, Min Ji Hong, John G Labram, Bernard Wenger, Henry J Snaith

Abstract:

Charge carrier mobility is a fundamental property of semiconductor materials that governs many electronic device characteristics. For metal halide perovskites, a wide range of charge carrier mobilities have been reported using different techniques. Mobilities are often estimated via transient methods assuming an initial charge carrier population after pulsed photoexcitation and measurement of photoconductivity via non-contact or contact techniques. For nanosecond to millisecond transient methods, early-time recombination and exciton-to-free-carrier ratio hinder accurate determination of free-carrier population after photoexcitation. By considering both effects, we estimate long-range charge carrier mobilities over a wide range of photoexcitation densities via transient photoconductivity measurements. We determine long-range mobilities for FA0.83Cs0.17Pb(I0.9Br0.1)3, (FA0.83MA0.17)0.95Cs0.05Pb(I0.9Br0.1)3 and CH3NH3PbI3-xClx polycrystalline films in the range of 0.3 to 6.7 cm2 V−1 s−1. We demonstrate how our data-processing technique can also reveal more precise mobility estimates from non-contact time-resolved microwave conductivity measurements. Importantly, our results indicate that the processing of polycrystalline films significantly affects their long-range mobility.
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