Aron Walsh’s research while affiliated with Imperial College London and other places

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Publications (75)


Lasing performance of (PEA)2MAn‐1SnnI3n+1 (n = 1–3) flakes and the control of cavities via nanofabrication. a) Lasing spectra of (PEA)2SnI4 at 2.88 µJ cm⁻², (PEA)2MASn2I7 at 1.54 µJ cm⁻² and (PEA)2MA2Sn3I10 at 2.19 µJ cm⁻². b) 2D mapping of (PEA)2MA2Sn3I10 PL spectra associated with the excitation pump fluence. c) The FWHM as a function of the pump fluence of (PEA)2MAn‐1SnnI3n+1 (n = 1–3) nanolasers. d) Polarization‐resolved spectra of both the lasing (red) and PL (blue) of (PEA)2MA2Sn3I10 nanolasers. e) Lasing thresholds of nanolasers based on 2D tin halide perovskite synthesized in air, N2, and with biuret. f) The lasing image of an exfoliated (PEA)2SnI4 flake with a well‐defined nanowire morphology. The inset is the corresponding optical image. g) The lasing image of a circular (PEA)2SnI4 nanosheet fabricated via FIB etching. The inset is the corresponding SEM image. The SEM (h) and lasing (i) images of a highly periodic (PEA)2SnI4 array fabricated by FIB etching.
Optimized single crystal quality and dual oxidation suppression of Sn²⁺ via the biuret‐assisted two‐step growth strategy in an oxygen‐free atmosphere. a) Photographs of (PEA)2MA2Sn3I10 single crystals obtained via one‐step and modified two‐step synthesis methods. The length of the red square is 1 mm. PXRD profiles (b) and PL spectra (c) of (PEA)2MAn‐1SnnI3n+1 (n = 1–3) synthesized in air, N2, and with biuret. d) XPS core level spectra of Sn 3d for (PEA)2SnI4 in N2 and with biuret. e) Proportion of Sn⁴⁺ measured from the surface of (PEA)2MAn‐1SnnI3n+1 (n = 1‐3) crystals synthesized in air, N2 and with biuret. f) Proportion of Sn⁴⁺ on the surface and the inner area of (PEA)2MA2Sn3I10 synthesized in air, N2, and with biuret. g) Lifetime (τ2) of (PEA)2MA2Sn3I10 synthesized in air, N2 and with biuret.
Stabilization mechanism of biuret molecules. a) ESP map of biuret molecule and its potential interaction with [SnI6]⁴⁻ octahedra. b) Bader volume of (PEA)2MA2Sn3I10 with and without the biuret. Electron localization function images of (PEA)2MA2Sn3I10 (c) without biuret and (d) with the biuret. e) XRD profiles of the (PEA)2MA2Sn3I10 products under N2 without biuret (black), with biuret (blue), and with biuret & an additional 10% SnI2 (red). f) ¹³C NMR spectra of biuret, biuret + PEAI, biuret + MAI and biuret + SnI2 in DMSO‐d6 solution.
Photostability and lasing stability of 2D tin halide perovskites. a) PL retention of (PEA)2MA2Pb3I10, and (PEA)2MA2Sn3I10 at a pump fluence of 0.17 µJ cm⁻², both of which used 560 nm fs laser as the excitation light. b) Time‐resolved PL spectra of (PEA)2MA2Sn3I10 at the pristine state and after laser illumination. c) Time‐resolved PL spectra of (PEA)2MA2Pb3I10 in the pristine state and after laser illumination. d) Lasing stability of (PEA)2MA2Pb3I10 and (PEA)2MA2Sn3I10 at a pump fluence of 1.1 Pth, both of which use a 620 nm fs‐laser as excitation light. e) Evolution of the light emission of a (PEA)2MA2Sn3I10 flake from spontaneous PL to lasing under constant optical pumping. f) Extracted PL and lasing spectra from (e) at different periods.
Dual Oxidation Suppression in Lead‐Free Perovskites for Low‐Threshold and Long‐Lifespan Lasing
  • Article
  • Publisher preview available

March 2025

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3 Reads

Yahui Li

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Zhenzhu Li

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Yanxin Han

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[...]

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Enzheng Shi

Low lasing threshold and long‐term operational stability are essential in advancing cost‐effective, efficient lead‐free (tin) halide perovskite lasers. However, the rapid crystallization of tin perovskites and oxidation of Sn²⁺ lead to substantial amounts of lattice defects, detrimental to laser performance enhancement. Herein, a dual oxidation suppression strategy is developed to suppress the oxidation of Sn²⁺ 2D tin halide perovskites, i.e., adopting an oxygen‐free two‐step growth to enhance the crystal quality and incorporating electron‐donating biuret molecules to coordinate with Sn²⁺ during the crystal growth, which led to the substantial reduction of lasing threshold to <1 µJ cm⁻² in (PEA)2MASn2I7. This represents the lowest value in lead‐free perovskite nanolasers and approximately one order of magnitude lower than those previously reported for tin‐based nanolasers. Investigations into the spontaneous photoluminescence (PL) and stimulated lasing emission revealed that 2D tin perovskites exhibited superior photostability and lasing stability compared to their lead counterparts. Specifically, the lasing intensity of (PEA)2MA2Sn3I10 constantly increased by >300% under optical pumping and the lasing threshold decreased by ≈17%, which is not observed in their lead counterparts. The findings highlight the prospect of 2D tin halide perovskites as lead‐free gain materials and cavities for solution‐processed nanolasers with low lasing thresholds and exceptional stability.

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Electrostatic Control of Electronic Structure in Modular Inorganic Crystals

December 2024

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5 Reads

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1 Citation

Journal of the American Chemical Society

The rules that govern structure and bonding, established for elemental solids and simple compounds, are challenging to apply to more complex crystals formed of polyatomic building blocks, such as layered or framework materials. Whether these modular building blocks are electrically neutral or charged influences the physical properties of the resulting crystal. Despite the prevalence of alternating charged units, their effects on the electronic structure remain unclear. We demonstrate how the distribution of charged building blocks, driven by differences in the electrostatic potential, governs the electronic band energies formed in layered crystals. This coarse-grained model predicts the spatially separated valence and conduction band edges observed in the metal-oxyhalide Ba2Bi3Nb2O11Cl and explains observed property trends in the Sillén–Aurivillius crystal system. Moreover, the general nature of the model allows for extension to other modular structure types, illustrated for Sillén and Ruddlesden–Popper layered compounds, and can support the rational design of electronic properties in diverse materials.


Accelerating CO₂ Direct Air Capture Screening for Metal-Organic Frameworks with a Transferable Machine Learning Force Field

December 2024

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4 Reads

Direct air capture (DAC) of CO₂ is necessary for climate change mitigation, but it faces challenges from low atmospheric CO₂ concentrations and competition from water vapor. Metal-organic frameworks (MOFs) are attractive candidates for DAC owing to their exceptionally high surface area, tunable porosity, and potential for adsorption-based capture processes with relatively low regeneration cost. Identifying optimal MOFs is hindered by their structural complexity, the vastness of their chemical space, and the expense of accurate simulations. Here, we present a machine learning force field (MACE-DAC) tailored for CO2 and H2O interactions in MOFs by finetuning the foundation model MACE-MP-0. To address smoothing issues and catastrophic forgetting, we curated the diverse GoldDAC dataset and introduced a continual learning loss function. To efficiently sample gas configurations, we developed the DAC-SIM package that uses MLFFs to achieve ab initio quality thermodynamics based on Widom insertion at computational speeds comparable to classical force fields. High-throughput screening on more than 8,000 synthesized MOF structures was performed to identify optimal MOFs and extract important chemical features. This approach overcomes prior limitations in describing CO2/MOF and H₂O/MOF interactions, providing a scalable and accurate framework for accelerating DAC research for porous materials.


Picosecond Lifetimes of Hydrogen Bonds in the Halide Perovskite CH 3 NH 3 PbBr 3

November 2024

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9 Reads

The Journal of Physical Chemistry C

The structures and properties of organic–inorganic perovskites are influenced by the hydrogen bonding between the organic cations and the inorganic octahedral networks. This study explores the dynamics of hydrogen bonds in CH3NH3PbBr3 across a temperature range from 70 to 350 K, using molecular dynamics simulations with machine-learning force fields. The results indicate that the lifetime of hydrogen bonds decreases with increasing temperature from 7.6 ps (70 K) to 0.16 ps (350 K), exhibiting Arrhenius-type behavior. The geometric conditions for hydrogen bonding, which include bond lengths and angles, maintain consistency across the full temperature range. The relevance of hydrogen bonds for the vibrational states of the material is also evidenced through a detailed analysis of the vibrational power spectra, demonstrating their significant effect on the physical properties for this class of perovskites.


Exploration of crystal chemical space using text-guided generative artificial intelligence

November 2024

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22 Reads

The vastness of chemical space presents a long-standing challenge for the exploration of new compounds with pre-determined properties. In materials science, crystal structure prediction has become a mature tool for mapping from composition to structure based on global optimisation techniques. Generative artificial intelligence (AI) now offers the means to efficiently navigate larger regions of crystal chemical space informed by structure-property datasets of materials. We introduce a model, named Chemeleon, designed to generate chemical compositions and crystal structures by learning from both textual descriptions and three-dimensional structural data. The model employs denoising diffusion techniques for compound generation using textual inputs aligned with structural data via cross-modal contrastive learning. The potential of this approach is demonstrated for multi-component compound generation, including the prediction of stable phases in the Li-P-S-Cl quaternary space of relevance to solid-state batteries. Our work highlights the potential of bridging geometric and linguistic data to unlock approaches to materials design.


Roadmap on established and emerging photovoltaics for sustainable energy conversion

October 2024

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432 Reads

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11 Citations

Photovoltaics (PVs) are a critical technology for curbing growing levels of anthropogenic greenhouse gas emissions, and meeting increases in future demand for low-carbon electricity. In order to fulfill ambitions for net-zero carbon dioxide equivalent (CO2eq) emissions worldwide, the global cumulative capacity of solar PVs must increase by an order of magnitude from 0.9 TWp in 2021 to 8.5 TWp by 2050 according to the International Renewable Energy Agency, which is considered to be a highly conservative estimate. In 2020, the Henry Royce Institute brought together the UK PV community to discuss the critical technological and infrastructure challenges that need to be overcome to address the vast challenges in accelerating PV deployment. Herein, we examine the key developments in the global community, especially the progress made in the field since this earlier roadmap, bringing together experts primarily from the UK across the breadth of the PVs community. The focus is both on the challenges in improving the efficiency, stability and levelized cost of electricity of current technologies for utility-scale PVs, as well as the fundamental questions in novel technologies that can have a significant impact on emerging markets, such as indoor PVs, space PVs, and agrivoltaics. We discuss challenges in advanced metrology and computational tools, as well as the growing synergies between PVs and solar fuels, and offer a perspective on the environmental sustainability of the PV industry. Through this roadmap, we emphasize promising pathways forward in both the short- and long-term, and for communities working on technologies across a range of maturity levels to learn from each other.


Design and evidence of a ferroelectric 2D/3D/2D perovskite heterostructure
a Time of flight secondary ion mass spectrometry (ToF-SIMS) depth element profile and (b) photoluminescence (PL) spectrum of photo-ferroelectric perovskite thin film deposited on ITO. c Graphical representation of the 2D/3D/2D perovskite heterostructure. d Cross-sectional low mag transmission electron microscopy (TEM) image of device configuration with thick (~ 60 nm) discontinuous horizontal 2D at bottom (Zoom-in HAADF-STEM (inset)), and thinner (~30 nm) more discrete at top. e HRTEM of 2D-Bottom is n = 2 confirm by FFT (inset). f Similarly 2D-Top is n = 1 on top of 3D-pvk confirm by FFT (inset). g Topography, (h) amplitude, (i, j) phase and (k) corresponding profiles of a selected region of photo-ferroelectric perovskite thin film obtained from piezoresponce force microscopy (PFM) measurements. The phase signal is recorded with both a voltage bias of +3 V and −3 V to highlight that a switch in the orientation of the polar domains of the material is induced by changing the sign of the voltage bias applied to the tip.
Real space model of the 2D/3D interface
a Calculated charge density difference (CDD) and local potential difference (LPD) across the entire superlattice of the (4,4-DFPD)2PbI4/FAPbI3 interface, assuming an antiferroelectric configuration of 4,4-DFPD molecular cations. b Atomic geometry and schematic diagram illustrating the 2D/3D interface with an antiferroelectric molecular configuration, where the black arrows indicate the electric dipole directions of 4,4-DFPD and E→zferr\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\vec{E}}_{z}^{{ferr}}$$\end{document} represents the resulting electric field along the z direction. Atomic geometry and schematic diagrams for the 2D/3D interface in a ferroelectric configuration, with the net dipole along the z-direction towards the (c) 3D perovskite and (d) the 2D perovskite. The resultant potential difference between the 2D and 3D perovskites is depicted by the orange curves.
Photovoltaic performances of the photoferroelectric 2D/3D/2D perovskite based solar cells
Power conversion efficiency (PCE) (a), open circuit voltage (VOC) (b), short circuit current density (JSC) (c) and fill factor (FF) (d) for both control and photo-ferroelectric devices with and without an applied voltage bias to highlight the effect of domains reorientation on the photovoltaic parameters. Graphical representation of the effect of polarization bias on the photo-ferroelectric device, where E→ferr\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\vec{E}}_{{ferr}}$$\end{document} represents the additional electric field provided by the ferroelectric perovskite interfaces (e). Effect of voltage bias on the current-voltage (JV) curve (f) and detailed VOC losses analysis for the control and photo-ferroelectric devices. g PCE (h) and Voc (i) literature values for PSCs between 1.47 eV and 1.65 eV, with PCE > 22% and VOC > 1.16 V.
Steady-state and transient electro-optical analysis
Terahertz (THz), transient absorption (TA) and time resolved photoluminescence (TRPL) spectroscopy measurements (fitting traces in dashed lines) performed on different stacks configurations and with an initial charge carrier density of 1017 cm⁻³ for control (a–c) and photo-ferroelectric samples (d–f), respectively. Quasi-fermi level splitting (QFLS) maps extrapolated from PLQY images of neat perovskite layer (g, k), perovskite layer deposited upon MeO-2Pacz (h, l) and the full stack comprising MeO-2Pacz-perovskite-PCBM (i, m) for control and photo-ferroelectric samples, respectively. The maps represent the QFLS distribution on the surface of the layer in a range from 1.16 eV to 1.26 eV. QFLS histograms (j, n) extrapolated from the QFLS maps of the same device stacks reported in (g–i) and (k–m), respectively.
Photo-ferroelectric perovskite interfaces for boosting VOC in efficient perovskite solar cells

October 2024

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121 Reads

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3 Citations

Interface engineering is the core of device optimization, and this is particularly true for perovskite photovoltaics (PVs). The steady improvement in their performance has been largely driven by careful manipulation of interface chemistry to reduce unwanted recombination. Despite that, PVs devices still suffer from unavoidable open circuit voltage (VOC) losses. Here, we propose a different approach by creating a photo-ferroelectric perovskite interface. By engineering an ultrathin ferroelectric two-dimensional perovskite (2D) which sandwiches a perovskite bulk, we exploit the electric field generated by external polarization in the 2D layer to enhance charge separation and minimize interfacial recombination. As a result, we observe a net gain in the device VOC reaching 1.21 V, the highest value reported to date for highly efficient perovskite PVs, leading to a champion efficiency of 24%. Modeling depicts a coherent matching of the crystal and electronic structure at the interface, robust to defect states and molecular reorientation. The interface physics is finely tuned by the photoferroelectric field, representing a new tool for advanced perovskite device design.


Electrochemical Nitrogen Reduction: The Energetic Distance to Lithium

September 2024

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34 Reads

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5 Citations

ACS Energy Letters

Energy-efficient electrochemical reduction of nitrogen to ammonia could help in mitigating climate change. Today, only Li- and recently Ca-mediated systems can perform the reaction. These materials have a large intrinsic energy loss due to the need to electroplate the metal. In this work, we present a series of calculated energetics, formation energies, and binding energies as fundamental features to calculate the energetic distance between Li and Ca and potential new electrochemical nitrogen reduction systems. The featured energetic distance increases with the standard potential. However, dimensionality reduction using principal component analysis provides an encouraging picture; Li and Ca are not exceptional in this feature space, and other materials should be able to carry out the reaction. However, it becomes more challenging the more positive the plating potential is.



Ionic species representations for materials informatics

September 2024

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25 Reads

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2 Citations

High-dimensional representations of the elements have become common within the field of materials informatics to build useful, structure-agnostic models for the chemistry of materials. However, the characteristics of elements change when they adopt a given oxidation state, with distinct structural preferences and physical properties. We explore several methods for developing embedding vectors of elements decorated with oxidation states. Graphs generated from 110 160 crystals are used to train representations of 84 elements that form 336 species. Clustering these learned representations of ionic species in low-dimensional space reproduces expected chemical heuristics, particularly the separation of cations from anions. We show that these representations have enhanced expressive power for property prediction tasks involving inorganic compounds. We expect that ionic representations, necessary for the description of mixed valence and complex magnetic systems, will support more powerful machine learning models for materials.


Citations (40)


... By fully understanding the optimal SEI properties in a high performing, lithium-based electrolyte, we can look towards the targeted optimisation of other chemistries, such as those based on calcium 7 or, ideally, other less energy intensive options 20,58 , as well as even an artificial SEI. While lithium is certainly capable of activating nitrogen, it also has an advantage over other chemistries in its ability to make a suitable SEI for nitrogen reduction 20,58 . Therefore, while this work provides further evidence that ethanol does not act simply as a proton donor, we can also see that lithium does not act only as a catalyst. ...

Reference:

The Role of Ethanol in Lithium-Mediated Nitrogen Reduction
Electrochemical Nitrogen Reduction: The Energetic Distance to Lithium
  • Citing Article
  • September 2024

ACS Energy Letters

... 3 The accompanying code is now part of the Hugging Face PEFT library, demonstrating its practical impact. Other recent publications highlight a high-throughput, data-driven framework for discovering novel quantum materials, 4 advances in materials informatics for property prediction, 5 and a tutorial on Bayesian approaches to inverse problems. 6 On the AP for ML side, we have featured a comprehensive perspective on novel computing approaches, such as in-memory computing with emerging memory devices, 7 along with a tutorial on a publicly accessible tool-an analog in-memory hardware acceleration kit for neural network training and inference, 8 and research related to the development of physical learning machines. ...

Ionic species representations for materials informatics

... In the present study, the band gap of CdSeTe thin film is increased above that of CdTe. The incorporation of Se has further been suggested to play an additional role in passivating defects within the material [37]. The film grown at 0.150 mM has an energy band gap that is good for the material to be used as an absorber layer alternative to CdTe in solar cell fabrication. ...

Roadmap on established and emerging photovoltaics for sustainable energy conversion

... These tools allow chemical configurations and physical properties to be explored efficiently, overcoming the limitations of traditional trial-anderror methods. The advantages of artificial intelligence in green material design include its ability to significantly reduce time and costs by automating processes and exploring broad design spaces, achieving remarkable efficiency [126]. The main disadvantages of artificial intelligence in green material design include the reliance on large and well-structured data sets, which can limit the applicability of the models; the high computational complexity that demands significant resources for their implementation; and the difficulties in predicting complex interactions in multi-component systems, such as in cosmetic formulations or water treatment materials [89,124,126]. ...

Has generative artificial intelligence solved inverse materials design?
  • Citing Article
  • July 2024

Matter

... BO relies on two core components for decision-making: a predictive surrogate model that estimates the objective function with uncertainty quantication, and an acquisition function that guides the selection of the next material to sample. 27 The acquisition function balances exploitation (choosing materials for which the model predicts optimal values) with exploration (sampling areas of high uncertainty to gather new information). 28,29 In this study, we employ a Gaussian Process Regressor (GPR) as the surrogate model due to its strong uncertainty quantication capabilities, and two acquisition functions, namely the Expected Improvement (EI) and Upper Condence Bound (UCB), which are popular choices in BO. 30 The input to the surrogate model is a numerical representation of the materials. ...

Race to the bottom: Bayesian optimisation for chemical problems

... In this manner, collections of molecules or materials are conceptualized as lands of opportunities to be explored by informed searches, rather than as haystacks in which to blindly search for needles. Such informed searches can greatly improve the efficiency of new discoveries in various chemistry fields such as drug discovery [27][28][29], chemical synthesis [30,31], asymmetric catalysis [32,33], materials [34][35][36][37][38][39], quantum property predictions [40], or toxicology [41]. ...

Mapping inorganic crystal chemical space

Faraday Discussions

... Similar orbital hybridization between nsnp and O 2p states was reported for other stereochemically active lone pairs cations, such as Bi 3+ and Sb 3+ . 50,51 The presence of occupied Pb 6s−O 2p antibonding states and Pb 6p−O 2p bonding states are the chemical bonding origin of the second-order Jahn−Teller distortion and thus presents the so-called stereochemically active lone pair effect. 52 By projecting the valence electronic density map onto the (010) plane of BaPbGa 4 O 8 (see Figure 10c), the localized stereochemically active Pb 2+ lone pairs protruding outward to the vacant side can be intuitively envisioned. ...

Band Gap Narrowing by Suppressed Lone-Pair Activity of Bi3
  • Citing Article
  • February 2024

Journal of the American Chemical Society

... [24,34] Phenothiazine (PTZ) is a well-known, electron-rich heterocyclic compound containing nitrogen and sulfur heteroatoms, characterized by high chemical stability and significant hole mobility. [20,35,36] So far, the predominant linking group in PTZ-based SAMs (PTZ-SAMs) remains alkyl chains, which are insulating and prone to UV-induced radical damage. In our previous work, we demonstrated that fully aromatic SAMs, emphasizing aromatic linkers (Ar-SAMs), significantly improve hole extraction/transport efficiency. ...

A Hole-Selective Self-Assembled Monolayer for Both Efficient Perovskite and Organic Solar Cells
  • Citing Article
  • February 2024

Langmuir

... 29 The rough HTLs will lead to poor ohmic contact between the electrodes and the active layers, resulting in a large number of traps in the interfaces. 30,31 Therefore, it is crucially important to design new HTL materials that can form compact and uniform SAM HTL on the ITO substrates to reduce contact defects with active layers that suppress the nonradiative recombination. In addition, the WF of HTLs can also be tuned by the SAM molecular modification. ...

Molecularly Engineered Self-Assembled Monolayers as Effective Hole-Selective Layers for Organic Solar Cells
  • Citing Article
  • January 2024

ACS Applied Energy Materials

... What are the implications of FAIR principles in ensuring easy and equitable access to codes and data? Any cyberinfrastructure for community use must adhere to FAIR (Findable, Accessible, Interoperable, and Reusable) principles [105][106][107] to ensure easy and equitable access to code and data. For the purposes of h-MESO we distinguish three components: data (mostly of experimental origin), codes (data reduction, analysis, modeling and simulation, visualization), and workflow manager infrastructure. ...

Open computational materials science
  • Citing Article
  • January 2024

Nature Materials