Amorphous titania
(am.-TiO2) has gained wide interest
in the field of photocatalysis, thanks to exceptional disorder-mediated
optical and electrical properties compared to crystalline TiO2. Here, we study the effects of intrinsic Ti3+ and
nitrogen defects in am.-TiO2 thin films via the atomic
layer deposition (ALD) chemistry of tetrakis(dimethylamido)titanium(IV)
(TDMAT) and H2O precursors at growth temperatures of 100–200
°C. X-ray photoelectron spectroscopy (XPS) and computational
analysis allow us to identify structural disorder-induced penta- and
heptacoordinated Ti4+ ions (Ti5/7c
4+), which are related to the formation of Ti3+ defects
in am.-TiO2. The Ti3+-rich ALD-grown am.-TiO2 has stoichiometric composition, which is explained by the
formation of interstitial peroxo species with oxygen vacancies. The
occupation of Ti3+ 3d in-gap states increases with the
ALD growth temperature, inducing both visible-light absorption and
electrical conductivity via the polaron hopping mechanism. At 200
°C, the in-gap states become fully occupied extending the lifetime
of photoexcited charge carriers from the picosecond to the nanosecond
time domain. Nitrogen traces from the TDMAT precursor had no effect
on optical properties and only little on charge transfer properties.
These results provide insights into the charge transfer properties
of ALD-grown am.-TiO2 that are essential to the performance
of protective photoelectrode coatings in photoelectrochemical solar
fuel reactors.
The increase in semiconductor conductivity that occurs when a hard indenter is pressed into its surface has been recognized for years, and nanoindentation experiments have provided numerous insights into the mechanical properties of materials. In particular, such experiments have revealed so called pop-in events, where the indenter suddenly enters deeper into the material without any additional force being applied; these mark the onset of the elastic-plastic transition. Here, we report the observation of a current spike--a sharp increase in electrical current followed by immediate decay to zero at the end of the elastic deformation--during the nanoscale deformation of gallium arsenide. Such a spike has not been seen in previous nanoindentation experiments on semiconductors, and our results, supported by ab initio calculations, suggest a common origin for the electrical and mechanical responses of nanodeformed gallium arsenide. This leads us to the conclusion that a phase transition is the fundamental cause of nanoscale plasticity in gallium arsenide, and the discovery calls for a revision of the current dislocation-based understanding of nanoscale plasticity.
Titanium dioxide (TiO2) thin films are widely employed for photocatalytic and photovoltaic applications where the long lifetime of charge carriers is a paramount requirement for the device efficiency. To ensure the long lifetime, a high temperature treatment is used which restricts the applicability of TiO2 in devices incorporating organic or polymer components. In this study, we exploited low temperature (100–150 °C) atomic layer deposition (ALD) of 30 nm TiO2 thin films from tetrakis(dimethylamido)titanium. The deposition was followed by a heat treatment in air to find the minimum temperature requirements for the film fabrication without compromising the carrier lifetime. Femto-to nanosecond transient absorption spectroscopy was used to determine the lifetimes, and grazing incidence X-ray diffraction was employed for structural analysis. The optimal result was obtained for the TiO2 thin films grown at 150 °C and heat-treated at as low as 300 °C. The deposited thin films were amorphous and crystallized into anatase phase upon heat treatment at 300–500 °C. The average carrier lifetime for amorphous TiO2 is few picoseconds but increases to >400 ps upon crystallization at 500 °C. The samples deposited at 100 °C were also crystallized as anatase but the carrier lifetime was <100 ps.
Valagiannopoulos, C.A.; Tukiainen, A.; Aho, T.; Niemi, T.; Guina, M.; Tretyakov, Sergei; Simovski, Konstantin Perfect magnetic mirror and simple perfect absorber in the visible spectrum Known experimental artificial magnetic conductors for terahertz and optical frequencies are formed by arrays of nanoparticles of various shapes. In this paper, we show that artificial magnetic conductors for the visible spectrum can be realized as simple, effectively quasistatic resonating structures, where the effective inductance is due to the magnetic flux inside a uniform metal substrate, and the effective capacitance is due to electric polarization of a thin uniform dielectric cover. To illustrate the main potential application of artificial magnetic conductors, we concentrate on the perfect-absorption regime, achieved by adjusting the loss factor of the artificial magnetic conductor to match its real input impedance to free space. We provide approximate analytical design formulas and introduce a simple equivalent circuit to explain the physical mechanism of emulation of magnetic response and perfect absorption of light. A prototype of a nearly perfect absorber for optical (from green to ultraviolet) frequencies is designed and experimentally tested. The results confirm the theoretical predictions and show polarization insensitivity and angular independence of response in a wide range of incidence angles.
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