FG Angewandte Physik und Halbleiterspektroskopie
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Cerium oxide-tin oxide (CeOx/SnOx) thin films with varying Sn content were deposited using RF magnetron sputtering and investigated for hydrogen sensing applications. Structural, compositional, and morphological properties were characterized using X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), atomic force microscopy (AFM), transmission electron microscopy (TEM), and energy-dispersive X-ray spectroscopy (EDX). Gas sensing measurements showed effective hydrogen detection at room temperature, with the sensitivity strongly influenced by Sn content and oxygen vacancy concentration. Higher Sn concentration enhanced the sensing response, which was correlated with microstructural features obtained from AFM and EDX, as well as with the presence of Ce3+ and Ce4+ oxidation states identified by XPS. This study highlights the potential of CeOx/SnOx thin films for possible back-end-of-line integration and provides proof-of-principle for room-temperature hydrogen sensing.
Here we report an investigation of ultrathin tin oxide films on Pt3Sn(111) using low-energy electron microscopy (LEEM), microspot low-energy electron diffraction (𝜇-LEED), scanning tunneling microscopy (STM), surface X-ray diffraction (SXRD), and high-resolution X-ray photoelectron spectroscopy (XPS). Oxidation at ∼390–410 ◦C produces triangular, two-dimensional oxide islands that nucleate rapidly and exhibit self-limited lateral growth, attributed to limited Sn diffusion from the subsurface of the crystal. 𝜇-LEED shows that the initially formed (4 × 4) Sn oxide is subsequently converted to a more oxygen-rich (2 × 2𝑛) ‘‘stripe’’ phase. At 630 ◦C, enhanced Sn mobility enables a closed (4 × 4) film. The (2 × 2𝑛) phase is shown to consist of a (2 × 2) Sn lattice modulated by 1D stripe defects with spacings of 𝑛 = 4–6 atomic rows; LEED and SXRD measurements show diffraction features corresponding to this striped superstructure. The two oxides can be distinguished in XPS by their O 1s lineshapes: the (4 × 4) phase shows a clear doublet attributable to distinct O species, whereas the (2 × 2𝑛) phase exhibits a broader envelope consistent with a distribution of O coordination environments. The Sn 3d5∕2 spectra are similar for both phases, reflecting closely related Sn bonding motifs. The spectra are consistent with those of previous near-ambient-pressure XPS measurements, suggesting that the surface oxides forming under CO oxidation conditions are similar to those studied here.
Development of detailed surface reaction mechanism for methanation process based on experiments
(2026)
The pressure to reduce greenhouse gas emissions is growing, which demands new and innovative technologies to produce mobile as well as stationary energy. The methanation offers a pathway to reduce greenhouse gas emissions by directly converting to . This also plays a crucial role in “power‐to‐gas” (P2G) technologies by providing an approach to store excess renewable energy in the form of methane in an existing natural gas infrastructure. However, methanation is a complex process due to its exothermic nature, interaction of the gas species with the catalyst, and possible catalyst degradation. Therefore, a deeper understanding is required for the methanation reaction, its different reaction pathways, and side reactions. In this work, we aim to understand the direct production of synthetic natural gas from and in a Sabatier process with the help of experiments over a Ni/ catalyst. A detailed surface reaction mechanism is developed to extend the study numerically by validating the simulation results with the experimental data. A one‐dimensional model, LOGEcat, based on a single‐channel catalyst model, is used for kinetic modeling. Experiments as well as simulations have been performed at various conditions, such as temperature variation and dilution to the inlet composition. We have successfully captured the experimental trends using the kinetic model developed for the conditions considered for the analysis.
The surface of β-Ga₂O₃ single crystals cleaved along their (100) plane is investigated using surface x-ray diffraction and atomic force microscopy. The results show the surface to consist of a single, so-called B-termination, which means that the crystal cleaves at planes formed by edge-sharing oxygen octahedra, thereby breaking the longest and weakest Ga–O bonds. Refinement of the atomic positions results in small displacements from the bulk structure, at most approximately 0.01 Å. Atomic force microscopy suggests that relatively large terraces form together with steps of half the a-axis length of approximately 0.6 nm, which means that terraces have the same atomic termination, related by the crystal symmetry. These results are important as a fundamental property of β-Ga₂O₃ when processed or used in various semiconductor applications.
Cerium oxide thin films were prepared by electron beam evaporation (EBE) under three deposition conditions: standard process, substrate heating at 200 °C, and ion beam assisted deposition (IBAD). The high optical transparency of the PVD-prepared coatings enables integration with transparent microelectronic devices, an aspect seldom explored in ceria-based gas sensors. Raman and optical analyses revealed various levels of oxygen vacancy-related defects in all films. Gas sensing measurements of the Pd/CeOx structures were correlated with their structural and electronic characteristics, including changes in Ce4+/Ce3+ ratios and band alignment during exposure to reducing gases, providing insight into the redox-driven sensing mechanism. All structures exhibit high ethanol sensitivity, while the highest response achieved for the films deposited with substrate heating and IBAD is consistent with their larger defect density and modified morphology. These findings demonstrate that tailoring EBE conditions provides an effective route to optimize CeOx thin films for improved gas sensing performance.
Nitrogen doping is a widely-used strategy for enhancing the electronic and electrocatalytic properties of graphene. On single-sheet graphene electrodes, substrate-induced charge density effects obscure their intrinsic behavior and limit the efficiency of surface-sensitive electron transfer. Here, we report a Janus bilayer electrode architecture that decouples a nitrogen-doped graphene top layer from the substrate via a pristine graphene bottom layer. This design allows the presentation of catalytically active nitrogen sites while simultaneously suppressing substrate effects, enabling a direct evaluation of the intrinsic effect of nitrogen-doping on the electron transfer (ET) properties of graphene. Using ferricyanide as a redox-probe, we show that the ET kinetics of pristine bilayer graphene are pH-dependent, while nitrogen-doped bilayer graphene displays stable, pH-independent redox behavior. As an application avenue of biological relevance, we demonstrate that nitrogen-doped bilayer graphene exhibits a reduced overpotential for NADH oxidation. These results demonstrate that the synergy between substrate decoupling and controlled nitrogen incorporation yields a robust electrode architecture with enhanced stability and improved electrocatalytic activity.
This study explores the role of atomic layer deposition (ALD) as an enabling technique for the defect engineering of catalytically active ultrathin deposits. In particular, we demonstrate the feasibility of tuning the O/Ce ratio in thermal ALD-based cerium oxide layers grown on silicon-based or alumina substrates by using the organometallic precursor tris(N, N’-diisopropyl-2-dimethylamido-guanidinato)cerium(III) ([Ce(dpdmg)3]) with H2O, O2, or O3 as coreactants. As revealed by in situ X-ray photoelectron spectroscopy (XPS), the Ce3+ concentration, i.e., the concentration of oxygen vacancies, depends strongly on three factors: the type of oxygen source, the chosen substrate, and the film thickness. The fixation of Ce3+ states during the early stages of growth is primarily determined by interface formation and the appearance of silicate and aluminate species, along with changes in morphology and surface-to-volume ratio. For thicker deposits (>5 nm), the intrinsic oxygen vacancies are coreactant-dependent. Furthermore, the chosen oxygen source also influences the morphology of ultrathin deposits, enabling potential surface functionalization with ceria nanoislands of varying composition and size. We point to a likely connection between this chemical and morphological tuning and changes in the ALD reaction pathway. The evolution of different nitrogen and carbon species depends on the oxygen source and the number of ALD cycles, indicating a shift in the ALD reaction mechanism from ligand exchange using H2O to ligand combustion for O3. The comprehensive investigation of these growth parameters is crucial for tailoring film properties via precise defect engineering.
Formation and role of the interface region in ultrathin metal oxide layers for resistive gas sensors
(2026)
In miniaturized gas resistive-sensor systems, understanding sensor performance and determining the optimal thickness of the active material requires an in-depth characterization of material deposition. In particular, the early stages of growth are mediated by interface formation and film/substrate interaction, which influence the mode of growth and the physicochemical properties of the active deposit, likely affecting the sensor response for ultrathin layers. We present the use of in-situ X-ray photoelectron spectroscopy and operando spectroscopic ellipsometry for characterizing thin (<20 nm) atomic layer-deposited layers for use in next-generation miniaturized sensor devices. By targeting cerium and tin oxide layers, we demonstrate how these techniques can provide insights into their material composition, thickness, and optical properties during interface formation and the transition to bulk-like properties.
Copper sulfide (CuS) is a multifunctional semiconductor with broad potential in catalysis, energy storage, and spintronics. In this work, Cr-doped CuS nanoparticles (Cu1-xCrxS, 0 ≤ x ≤ 0.4) were synthesized and investigated using scanning electron microscopy coupled with energy-dispersive X-ray spectroscopy (SEM/EDX), X-ray diffraction (XRD), electron paramagnetic resonance (EPR), and synchrotron-based X-ray absorption fine-structure spectroscopy (XAFS). SEM/EDX analyses reveal the nanostructured morphology of the samples and the homogeneous distribution of Cr within the Cu1-xCrxS matrix. XRD suggests the retention of the hexagonal covellite CuS phase across the entire doping series, while increasing Cr content, particularly beyond x ≈ 0.2, induces asymmetric peak broadening, selective intensity variations, and suppression of specific reflections, indicating increased lattice strain and solubility-limit-related structural perturbations. EPR reveals the presence of Cr3+ ions and magnetic defect states, accompanied by non-monotonic variations in linewidth and signal asymmetry at higher doping levels. XANES and EXAFS analyses support the substitution of Cu by Cr3+ within the covellite lattice, with the Cu–S first coordination shell remaining largely preserved, whereas higher-shell disorder progressively increases with Cr incorporation. Combined XRD, EPR, and XAFS results identify a composition range of x ≈ 0.05–0.1 associated with minimal structural perturbation, a transition regime at x = 0.1–0.2, and increasing local disorder at x ≥ 0.2. These findings correlate local Cr coordination with defect formation, lattice distortion, and local electronic-structure evolution. The results provide a spectroscopic and structural framework for understanding Cr-induced modifications in CuS-based materials.
This work presents the results of investigating the influence of experimental parameters on the growth and properties of pyrite thin films produced by sulfurating metallic Fe layers. We use in-situ monitoring of the Seebeck coefficient and electrical conductivity of the films to study the influence of three variables that directly control the partial pressure of molecular sulfur (S2) and, consequently, the growth of pyrite films. These variables are the sample temperature during their sulfuration (Ts), the final temperature of the basket holding the elemental sulfur (Tsb), and its heating ramp (TRsb). Compared with selected reference conditions in which the global sulfuration reaction is slowed down, our results show that higher Ts and S2 partial pressures increase the kinetics of the sulfuration process. This acceleration helps to put in evidence the two main stages of Fe sulfuration to pyrite: (i) first diffusion of Fe vacancies (Fe → Fe1-x S) and (ii) diffusion of interstitial sulfur (Fe1-xS → FeS2), with some overlapping between both steps. For Ts values below 540 K, the resulting sulfurated layers present traces of pyrrhotite. We also link differences in the stages of pyrite film growth to the formation of various types of defects, primarily iron and sulfur vacancies and interstitial sulfur atoms. These defects are correlated with the macroscopic transport properties of the films through a two-band conduction model. Our results highlight that precise control of specific experimental conditions enables tuning of the defects and the microstructure of the obtained pyrite films and, therefore, their macroscopic properties.