DESIGN AND CHARACTERIZATION OF CU2O PHOTOCATHODES FOR PHOTOELECTROCHEMICAL WATER SPLITTING.

The exploitation of renewable energy sources is one of the most addressed aspects for the sustainable development of human activities. Molecular hydrogen can be considered one of the most interesting energy vectors to fulfill humankind\u2019s needs. In this context, photoelectrochemical water splitting (PEC-WS) using solar energy to produce H2 at semiconducting materials is considered one of the most interesting technologies. In the present study, Cu2O was selected as cathode material for its correct band position for hydrogen evolution, together with non\u2013toxic and low-cost starting material. The research activity was devoted to the development of photocathodes for the PEC-WS and their characterization under working conditions with different techniques. The work was divided in: I) The role of the underlayer in Cu2O photocathodes for PEC-WS; II) Characterization of copper oxide based materials under PEC-WS by X-Ray Absorption Spectroscopy (XAS) III) Characterization of Photoactive Semiconductor Materials by Cavity Micro-Electrodes (C_ME) & Scanning ElectroChemical Microscopy (SECM) IV) Development of new protective layers for the PEC_WS systems: FeOOH and CuO/Cu2O core-shell systems V) Application of the Density Function Theory (DFT) to study doping materials and vacancy formation in Cu2O 1) The complete electrode scheme is constituted by (i) a transparent conductive support (usually FTO), (ii) a conductive underlayer of electrodeposited Cu, that is assumed to enhance the electron-hole separation (iii) the semiconductor, (iv) a thin transparent protective overlayer of about 80 nanometers. In the present study, the underlayer of Cu replaces the expensive and toxic Cr/Au underlayer. Therefore, a specific protocol for the preparation of the Cu2O photoconverter was developed and validated, obtaining good results in terms of generated photocurrent (Figure 1). Appropriate modifications of underlayer deposition conditions also lead to large increase in the Cu2O photocurrents, thus denoting that the underlayer has a marked influence on the system performances. In the final deposition protocol, several parameters were defined and controlled: deposition potential and the relevant current intensity; temperature, pH and stirring conditions; loading (C/cm2) of Cu(0) underlayer and Cu2O active layer. In particular, the thickness of the Cu underlayer was controlled in order to obtain a transparent layer while maintaining high electric conductivity. Transparency of the entire support is an important feature, allowing the use of the electrode in both front and back illumination configurations. Moreover, a complete study of the copper lactate bath was performed with electrochemical methods and X-ray Absorption Spectroscopy (XAS). The experiments show that the best fit is obtained by a model where four lactate ions act as monodentate ligands, 1:4 (Cu:L), in a distorted tetrahedral geometry. Notwithstanding the good results in photocurrent, the actual Cu2O photoconverter is able to work at the highest potential only for a few minutes and for this reason the development of a protective overlayer was mandatory as explained later. 2) The short life of Cu2O photoconverter is due to photodegradation. In order to investigate this phenomenon, XAS measurements at Cu-K edge were performed to define photodegradation products, individuate stability potential window and elucidate the possible combined effects of light and potential. In-situ and operando techniques like X-Ray Absorption Near Edge Structure (XANES), Extended X-Ray Absorption Fine Structure (EXAFS) and Fixed Energy X-Ray Absorption Voltammetry (FEXRAV) allow us to better understand material behavior. Changes in copper oxidation states upon light and/or applied potential were observed and with XANES was possible to evaluate the amount of photo-generated Cu(0) responsible of the loss of activity (Figure 2A). FEXRAV measurements allow following the material (photo)degradation and defining the stability windows (Figure 2B). With difference light and dark XANES spectra the local changes in electronic structure upon spectro-electrochemical conditions were also investigated. 3) The photodegradation reaction showed by Cu2O, is common to many other materials for HER and OER (Oxygen Evolution Reaction,). This instability occurs when the redox potential of the material lies between valence band and conduction band. This implies that the photocurrents recorded in normal pulsed experiments are composed by the sum of water splitting and photodegradation. The novel method here presented allows the evaluation of the intensity of the photo-degradation processes, giving at the same time a rapid screening tool for differently prepared materials. Moreover, this method allows to evaluate the activity of a semiconductor without any influence of the supporting material. In addition, low experimental times and low amount of photo-produced material are required if compared to actual methods (GC and volume displacement). Scanning ElectroChemical Microcopy (SECM), here used in Tip Generation/ Substrate Collection mode (TG/SC), allows to discriminate between water splitting and photo-degradation. The system is so composed: \u2022 Tip (working electrode 1) is a micro cavity electrode filled with the semiconducting powder. The electrode potential is varied in the potential window of interest under light steps. \u2022 Substrate is a Pt foil (working electrode 2) with potential fixed at the H2 (or O2) oxidation (reduction) value, working as a \u201cprobe\u201d for the species of interest. Several materials were studied with good results: CuXO, CuI, NiO and TiO2. Influence of cavity depth and light intensity were tested too. From data analysis we can demonstrate different photocurrent efficiencies for the studied materials. Obviously TiO2 is near to 100% (Figure 3B) as expected from its very high stability while other materials, as CuI, in spite the high photocurrents, shows very low amount of photogenerated H2. 4) Previously, we have seen how Cu2O photodegradation is due to the combination of light and potential. The phenomenon occurs because the photogenerated electrons have enough energy to reduce water but also to reduce the material itself. For this reason, the development of a protective layer that can avoid the photodegradation is of paramount importance. Different materials were considered, and the final choice falls on the two phases of iron oxyhydroxide, \u3b1-FeOOH and \u3b3-FeOOH, non-toxic and low-cost materials, deeply studied because they are corrosion products of chlorate process cathodes. These materials were here studied by electrochemical and XAS techniques to gain information about their oxidation state during HER and its reversibility. Then the final interaction of FeOOH and Cu2O was studied to explore the possibility of protecting the Cu(I) oxide by 80 nm of a transparent FeOOH layer. A different approach was then adopted with the preparation of a CuO/Cu2O core-shell material (denoted as CuXO). CuXO is composed by a CuO core and an external shell of Cu2O with the proportion determined via FEXRAV. Cu2O is grown on CuO by cycling the potential as in Figure 4, and eventually a stable and active material for HER is obtained. We were also able to assess that CuO is not an active species for HER, but also that the electrochemically generated Cu2O (the true active material for HER) is protected from photo-degradation by the CuO core. Our explanation for this protective action lies in the relative band position of CuO and Cu2O. CuO has a smaller band gap (1.5eV) that lies inside the larger band gap of Cu2O. FEXRAV (Figure 4B) supports this explanation, since the signal becomes constant in time, to indicate that the material transformation is stopped and that the only reaction occurring at the electrode is hydrogen evolution. These results are in agreement with the high photoefficiency of the CuXO powder determined with SECM. 5) According to literature the p-type character of Cu2O is strictly related to the formation of copper vacancies in its lattice. Doping can enhance the formation of vacancies, improving the number of majority carriers (holes) and their mobility, and modifying the band gap by shifting the Cu2O states or by introducing an intermediate band within the band gap (Figure 5B). On the basis of the electrochemical results obtained with different underlayers, this work firstly aims to study a large array of potentially effective metal underlayers. The role of Density Functional Theory (DFT) is here to rank the underlayers\u2019 aptitude in modifying the properties of Cu2O, and, in particular, the formation of copper or oxygen vacancies in the semiconductor. Then, the doping of the material is studied for a selected number of transition metals. For each material, the valence and conduction band positions were computed as well as the number of vacancies and their formation energies. Eventually the influence of lattice strain on material band gap and energy levels is studied both with expansion and reduction of the Cu2O lattice after the deposition onto different substrates. The use of the alkaline metals as well as atomic hydrogen as dopants allowed to evaluate the influence of the dopant size on the doped material

Determining the Efficiency of Photoelectrode Materials by Coupling Cavity‐Microelectrode Tips and Scanning Electrochemical Microscopy

Photoelectrochemical water splitting (PEC-WS) is a promising route to obtain hydrogen (and oxygen) from sunlight and water. However, too many semiconductors show poor stability, due to photodegradation phenomena in aqueous solutions, thus loosing efficiency under operative conditions. Aim of this paper is to introduce a simple and fast method for screening different semiconductor materials and identify their efficiency in H2 (or O2) production with respect to photocorrosion. This method could be used with any finely dispersed semiconductor (powder) for a fast, preliminary evaluation of the material's behaviour without interferences from the supporting material (i. e. FTO) or any binder. The method is based on the combination of scanning electrochemical microscopy (SECM) in the tip generation/substrate collection (TG/SC) mode and of cavity microelectrodes as SECM tips. Here, we show results obtained on three powder materials, namely core-shell CuI/CuO, CuI and TiO2

Influence of Strain on the Band Gap of Cu₂O

Cu\u2082O has been considered as a candidate material for transparent conducting oxides and photocatalytic water splitting. Both applications require suitably tuned band gaps. Here we explore the influence of compressive and tensile strain on the band gap by means of density functional theory (DFT) modeling. Our results indicate that the band gap decreases under tensile strain while it increases to a maximum under moderate compressive strain and decreases again under extreme compressive strain. This peculiar behavior is rationalized through a detailed analysis of the electronic structure by means of density of states (DOS), density overlap region indicators (DORI), and crystal overlap Hamilton populations (COHP). Contrary to previous studies we do not find any indications that the band gap is determined by d10-d10 interactions. Instead, our analysis clearly shows that both the conduction and the valence band edges are determined by Cu-O antibonding states. The band gap decrease under extreme compressive strain is associated with the appearance of Cu 4sp states in the conduction band region

Electrodeposited cu thin layers as low cost and effective underlayers for Cu2O photocathodes in photoelectrochemical water electrolysis

Cu2O is one of the most studied semiconductors for photocathodes in photoelectrochemical water splitting (PEC-WS). Its low stability is counterbalanced by good activity, provided that a suitable underlayer/support is used. While Cu2O is mostly studied on Au underlayers, this paper proposes Cu(0) as a low-cost, easy to prepare and highly efficient alternative. Cu and Cu2O can be electrodeposited from the same bath, thus allowing in principle to tune the final material\u2019s physico-chemical properties with high precision with a scalable method. Electrodes and photoelectrodes are studied by means of electrochemical methods (cyclic voltammetry, Pb underpotential deposition) and by ex-situ X-ray absorption spectroscopy (XAS). While the potential applied for the deposition of Cu has no influence on the bulk structure and on the photocurrent displayed by the semiconductor, it plays a role on the dark currents, making this strategy promising for improving the material\u2019s stability. Au/Cu2O and Cu/Cu2O show similar performances, the latter having clear advantages in view of future use in practical applications. The influence of Cu underlayer thickness was also evaluated in terms of obtained photocurrent

3D-printed photo-spectroelectrochemical devices for in situ and in operando X-ray absorption spectroscopy investigation

Three-dimensional printed multi-purpose electrochemical devices for X-ray absorption spectroscopy are presented in this paper. The aim of this work is to show how three-dimensional printing can be a strategy for the creation of electrochemical cells for in situ and in operando experiments by means of synchrotron radiation. As a case study, the description of two cells which have been employed in experiments on photoanodes for photoelectrochemical water splitting are presented. The main advantages of these electrochemical devices are associated with their compactness and with the precision of the threedimensional printing systems which allows details to be obtained that would otherwise be difficult. Thanks to these systems it was possible to combine synchrotron-based methods with complementary techniques in order to study the mechanism of the photoelectrocatalytic process

Studies of new Higgs boson interactions through nonresonant HH production in the b¯bγγ fnal state in pp collisions at √s = 13 TeV with the ATLAS detector

A search for nonresonant Higgs boson pair production in the b ¯bγγ fnal state is performed using 140 fb−1 of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. This analysis supersedes and expands upon the previous nonresonant ATLAS results in this fnal state based on the same data sample. The analysis strategy is optimised to probe anomalous values not only of the Higgs (H) boson self-coupling modifer κλ but also of the quartic HHV V (V = W, Z) coupling modifer κ2V . No signifcant excess above the expected background from Standard Model processes is observed. An observed upper limit µHH < 4.0 is set at 95% confdence level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The 95% confdence intervals for the coupling modifers are −1.4 < κλ < 6.9 and −0.5 < κ2V < 2.7, assuming all other Higgs boson couplings except the one under study are fxed to the Standard Model predictions. The results are interpreted in the Standard Model efective feld theory and Higgs efective feld theory frameworks in terms of constraints on the couplings of anomalous Higgs boson (self-)interactions

Comparison of inclusive and photon-tagged jet suppression in 5.02 TeV Pb+Pb collisions with ATLAS

Parton energy loss in the quark–gluon plasma (QGP) is studied with a measurement of photon-tagged jet production in 1.7 nb−1 of Pb+Pb data and 260 pb−1 of pp data, both at sNN=5.02 TeV, with the ATLAS detector. The process pp →γ+jet+X and its analogue in Pb+Pb collisions is measured in events containing an isolated photon with transverse momentum (pT) above 50 GeV and reported as a function of jet pT. This selection results in a sample of jets with a steeply falling pT distribution that are mostly initiated by the showering of quarks. The pp and Pb+Pb measurements are used to report the nuclear modification factor, RAA, and the fractional energy loss, Sloss, for photon-tagged jets. In addition, the results are compared with the analogous ones for inclusive jets, which have a significantly smaller quark-initiated fraction. The RAA and Sloss values are found to be significantly different between those for photon-tagged jets and inclusive jets, demonstrating that energy loss in the QGP is sensitive to the colour-charge of the initiating parton. The results are also compared with a variety of theoretical models of colour-charge-dependent energy loss

Search for non-resonant Higgs boson pair production in the 2b+2l+ETmiss final state in pp collisions at s = 13 TeV with the ATLAS detector

A search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (bb ̄) and the other decays to WW*, ZZ*, or τ+τ−, with in each case a final state with l+l−+ neutrinos (l = e, μ). The analysis targets separately the gluon-gluon fusion and vector boson fusion production modes. Data recorded by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 140 fb−1, are used in this analysis. Events are selected to have exactly two b-tagged jets and two leptons with opposite electric charge and missing transverse momentum in the final state. These events are classified using multivariate analysis algorithms to separate the HH events from other Standard Model processes. No evidence of the signal is found. The observed (expected) upper limit on the cross-section for non-resonant Higgs boson pair production is determined to be 9.7 (16.2) times the Standard Model prediction at 95% confidence level. The Higgs boson self-interaction coupling parameter κλ and the quadrilinear coupling parameter κ2V are each separately constrained by this analysis to be within the ranges [−6.2, 13.3] and [−0.17, 2.4], respectively, at 95% confidence level, when all other parameters are fixed

Measurement of the H → γ γ and H → ZZ∗ → 4 cross-sections in pp collisions at √s = 13.6 TeV with the ATLAS detector

The inclusive Higgs boson production cross section is measured in the di-photon and the Z Z∗ → 4 decay channels using 31.4 and 29.0 fb−1 of pp collision data respectively, collected with the ATLAS detector at a centre of-mass energy of √s = 13.6 TeV. To reduce the model dependence, the measurement in each channel is restricted to a particle-level phase space that closely matches the chan nel’s detector-level kinematic selection, and it is corrected for detector effects. These measured fiducial cross-sections are σfid,γ γ = 76+14 −13 fb, and σfid,4 = 2.80 ± 0.74 fb, in agreement with the corresponding Standard Model predic tions of 67.6±3.7 fb and 3.67±0.19 fb. Assuming Standard Model acceptances and branching fractions for the two chan nels, the fiducial measurements are extrapolated to the full phase space yielding total cross-sections of σ (pp → H) = 67+12 −11 pb and 46±12 pb at 13.6 TeV from the di-photon and Z Z∗ → 4 measurements respectively. The two measure ments are combined into a total cross-section measurement of σ (pp → H) = 58.2±8.7 pb, to be compared with the Stan dard Model prediction of σ (pp → H)SM = 59.9 ± 2.6 p