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CMP
Credit: Jack Hobhouse

Prof Henry Snaith FRS

Professor of Physics

Sub department

  • Condensed Matter Physics

Research groups

  • Photovoltaic & Optoelectronic Device Group
Henry.Snaith@physics.ox.ac.uk
Clarendon Laboratory, room 045,045,044,071.6,071.5,071.4,071.3,G21 (office)
  • About
  • Publications

Perovskite-perovskite tandem photovoltaics with optimized band gaps.

Science 354:6314 (2016) 861-865

Authors:

GE Eperon, T Leijtens, KA Bush, R Prasanna, T Green, JT Wang, DP McMeekin, G Volonakis, RL Milot, R May, A Palmstrom, DJ Slotcavage, RA Belisle, JB Patel, ES Parrott, RJ Sutton, W Ma, F Moghadam, B Conings, A Babayigit, HG Boyen, S Bent, F Giustino, LM Herz, MB Johnston, MD McGehee, HJ Snaith

Abstract:

We demonstrate four- and two-terminal perovskite-perovskite tandem solar cells with ideally matched band gaps. We develop an infrared-absorbing 1.2-electron volt band-gap perovskite, FA0.75Cs0.25Sn0.5Pb0.5I3, that can deliver 14.8% efficiency. By combining this material with a wider-band gap FA0.83Cs0.17Pb(I0.5Br0.5)3 material, we achieve monolithic two-terminal tandem efficiencies of 17.0% with >1.65-volt open-circuit voltage. We also make mechanically stacked four-terminal tandem cells and obtain 20.3% efficiency. Notably, we find that our infrared-absorbing perovskite cells exhibit excellent thermal and atmospheric stability, not previously achieved for Sn-based perovskites. This device architecture and materials set will enable "all-perovskite" thin-film solar cells to reach the highest efficiencies in the long term at the lowest costs.
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Cs$_2$InAgCl$_6$: A new lead-free halide double perovskite with direct band gap

(2016)

Authors:

George Volonakis, Amir A Haghighirad, Rebecca L Milot, Weng H Sio, Marina R Filip, Bernard Wenger, Michael B Johnston, Laura M Herz, Henry J Snaith, Feliciano Giustino
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Towards Lead-free Perovskite Solar Cells

ACS Energy Letters American Chemical Society (2016)

Authors:

Feliciano Giustino, Henry J Snaith

Abstract:

Since the first reports of solar cells with power conversion efficiencies around 10% in 2012, the science and technology of perovskite photovoltaics has been progressing at an unprecedented rate. The current certified record efficiency of 22.1% makes perovskites the first solutionprocessable technology to outperform multicrystalline and thin-film silicon. For this technology to be deployed on a large scale, the two main challenges that need to be addressed are the material stability and the toxicity of lead. In particular, while lead is allowed in photovoltaic modules, it would be desirable to find alternatives which retained the unique optoelectronic properties of lead halide perovskites. Here we offer our perspective on the most exciting developments in the materials science of new halide perovskites, with an emphasis on alternatives to lead. After surveying recent developments of new perovskites and perovskite-related materials, we highlight the potential of halide double perovskites. This new family of compounds constitutes uncharted territory, and may offer a broad materials library for solar energy applications.
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Mechanism for rapid growth of organic-inorganic halide perovskite crystals.

Nat Commun 7 (2016) 13303-13303

Authors:

PK Nayak, DT Moore, B Wenger, S Nayak, AA Haghighirad, A Fineberg, NK Noel, OG Reid, G Rumbles, P Kukura, KA Vincent, HJ Snaith

Abstract:

Optoelectronic devices based on hybrid halide perovskites have shown remarkable progress to high performance. However, despite their apparent success, there remain many open questions about their intrinsic properties. Single crystals are often seen as the ideal platform for understanding the limits of crystalline materials, and recent reports of rapid, high-temperature crystallization of single crystals should enable a variety of studies. Here we explore the mechanism of this crystallization and find that it is due to reversible changes in the solution where breaking up of colloids, and a change in the solvent strength, leads to supersaturation and subsequent crystallization. We use this knowledge to demonstrate a broader range of processing parameters and show that these can lead to improved crystal quality. Our findings are therefore of central importance to enable the continued advancement of perovskite optoelectronics and to the improved reproducibility through a better understanding of factors influencing and controlling crystallization.
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Charge-Carrier Dynamics in 2D Hybrid Metal-Halide Perovskites.

Nano letters 16:11 (2016) 7001-7007

Authors:

RL Milot, RJ Sutton, GE Eperon, AA Haghighirad, J Martinez Hardigree, L Miranda, HJ Snaith, MB Johnston, LM Herz

Abstract:

Hybrid metal-halide perovskites are promising new materials for use in solar cells; however, their chemical stability in the presence of moisture remains a significant drawback. Quasi two-dimensional (2D) perovskites that incorporate hydrophobic organic interlayers offer improved resistance to degradation by moisture, currently still at the cost of overall cell efficiency. To elucidate the factors affecting the optoelectronic properties of these materials, we have investigated the charge transport properties and crystallographic orientation of mixed methylammonium (MA)-phenylethylammonium (PEA) lead iodide thin films as a function of the MA-to-PEA ratio and, thus, the thickness of the "encapsulated" MA lead-halide layers. We find that monomolecular charge-carrier recombination rates first decrease with increasing PEA fraction, most likely as a result of trap passivation, but then increase significantly as excitonic effects begin to dominate for thin confined layers. Bimolecular and Auger recombination rate constants are found to be sensitive to changes in electronic confinement, which alters the density of states for electronic transitions. We demonstrate that effective charge-carrier mobilities remain remarkably high (near 10 cm(2)V(-1)s(-1)) for intermediate PEA content and are enhanced for preferential orientation of the conducting lead iodide layers along the probing electric field. The trade-off between trap reduction, electronic confinement, and layer orientation leads to calculated charge-carrier diffusion lengths reaching a maximum of 2.5 μm for intermediate PEA content (50%).
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