Data sets for "3D-cross Nanowire Networks Recover Full Terahertz State"

University of Oxford (2020)

Abstract:

Comma separated variable data for each figure in the manuscript

Elucidating the Role of a Tetrafluoroborate‐Based Ionic Liquid at the n‐Type Oxide/Perovskite Interface

Advanced Energy Materials Wiley 10:4 (2020)

Authors:

Nakita K Noel, Severin N Habisreutinger, Bernard Wenger, Yen‐Hung Lin, Fengyu Zhang, Jay B Patel, Antoine Kahn, Michael B Johnston, Henry J Snaith

Revealing the origin of voltage loss in mixed-halide perovskite solar cells

Energy and Environmental Science Royal Society of Chemistry 13 (2019) 258-267

Authors:

Suhas Mahesh, JM Ball, RDJ Oliver, DP McMeekin, P Nayak, MB Johnston, H Snaith

Abstract:

The tunable bandgap of metal-halide perovskites has opened up the possibility of tandem solar cells with over 30% efficiency. Iodide-Bromide (I-Br) mixed-halide perovskites are crucial to achieve the optimum bandgap for such tandems. However, when the Br content is increased to widen the bandgap, cells fail to deliver the expected increase in open-circuit voltage (VOC). This loss in VOC has been attributed to photo-induced halide segregation. Here, we combine Fourier Transform Photocurrent Spectroscopy (FTPS) with detailed balance calculations to quantify the voltage loss expected from the halide segregation, providing a means to quantify the VOC losses arising from the formation of low bandgap iodide-rich phases during halide segregation. Our results indicate that, contrary to popular belief, halide segregation is not the dominant VOC loss mechanism in Br-rich wide bandgap cells. Rather, the loss is dominated by the relatively low initial radiative efficiency of the cells, which arises from both imperfections within the absorber layer, and at the perovskite/charge extraction layer heterojunctions. We thus identify that focussing on maximising the initial radiative efficiency of the mixed-halide films and devices is more important than attempting to suppress halide segeregation. Our results suggest that a VOC of up to 1.33 V is within reach for a 1.77 eV bandgap perovskite, even if halide segregation cannot be supressed

Dual-source co-evaporation of low-bandgap FA1-xCsxSn1-yPbyI3 perovskites for photovoltaics

ACS Energy Letters American Chemical Society 4 (2019) 2748-2756

Authors:

JM Ball, L Buizza, HC Sansom, Farrar, MT Klug, J Borchert, J Patel, LM Herz, Michael Johnston, Henry Snaith

A Highly Emissive Surface Layer in Mixed-Halide Multication Perovskites.

Advanced materials (Deerfield Beach, Fla.) 31:42 (2019) e1902374

Authors:

Zahra Andaji-Garmaroudi, Mojtaba Abdi-Jalebi, Dengyang Guo, Stuart Macpherson, Aditya Sadhanala, Elizabeth M Tennyson, Edoardo Ruggeri, Miguel Anaya, Krzysztof Galkowski, Ravichandran Shivanna, Kilian Lohmann, Kyle Frohna, Sebastian Mackowski, Tom J Savenije, Richard H Friend, Samuel D Stranks

Abstract:

Mixed-halide lead perovskites have attracted significant attention in the field of photovoltaics and other optoelectronic applications due to their promising bandgap tunability and device performance. Here, the changes in photoluminescence and photoconductance of solution-processed triple-cation mixed-halide (Cs0.06 MA0.15 FA0.79 )Pb(Br0.4 I0.6 )3 perovskite films (MA: methylammonium, FA: formamidinium) are studied under solar-equivalent illumination. It is found that the illumination leads to localized surface sites of iodide-rich perovskite intermixed with passivating PbI2 material. Time- and spectrally resolved photoluminescence measurements reveal that photoexcited charges efficiently transfer to the passivated iodide-rich perovskite surface layer, leading to high local carrier densities on these sites. The carriers on this surface layer therefore recombine with a high radiative efficiency, with the photoluminescence quantum efficiency of the film under solar excitation densities increasing from 3% to over 45%. At higher excitation densities, nonradiative Auger recombination starts to dominate due to the extremely high concentration of charges on the surface layer. This work reveals new insight into phase segregation of mixed-halide mixed-cation perovskites, as well as routes to highly luminescent films by controlling charge density and transfer in novel device structures.