Abstract:Titanium-based materials have been considered promising materials for many years. The structures and properties of the TixOy and TiC at nanoscale is important to study the formation mechanism of their...
“…Instead of octahedral metal centers, the Ti atoms in subnanometer titanium oxide clusters are typically tetracoordinated, and the O atoms serve as either terminal or bridging atoms. The minimum energy Ti n O 2 n structures are in agreement with previously reported structures using numerous computational methods. ,,,,− Each Ti n O 2 n cluster contains two dangling O atoms. They are closed shell species, where all of the Ti-d electrons are transferred to the O atoms and therefore serve as models for the electronic structure of defect-free bulk titania.…”
Section: Resultssupporting
confidence: 88%
“…Far less work has been performed on the suboxide clusters, with only a few calculations previously reported. , The initial choices for the atomic coordinates for the geometrical optimization of the suboxide clusters were considered and obtained from previously published studies but optimized using the functional and basis set described in the Methods section. For instances where multiple cluster geometries were examined, we report the lowest energy geometry.…”
TD-DFT calculations were performed on neutral TinO2n, TinO2n-1, and TinO2n-2 clusters, where n ≤ 7. Our calculations show that the TinO2n clusters are closed shell systems containing empty d orbitals and that the partially filled d orbitals of the suboxide clusters have a profound effect on their structural, electronic, and topological properties. The low energy photoexcitations of TinO2n clusters are all O-2p to Ti-3d transitions, while the open-shell suboxide clusters are all characterized by d-d transitions that occur at a much smaller optical gap. Upon photoabsorption, the localization of the hole is accompanied by a local bond elongation, i.e., polaron formation, whereas d-electrons are generally delocalized among the cluster. Several of the compact of the TinO2n-2 structures contain higher symmetry which is reflected in their relative stability in the experimental cluster distribution. In particular, the tetrahedral symmetry of the optimized ground state structure for Ti4O6 inhibits charge carrier localization and therefore contains higher stability.
“…Instead of octahedral metal centers, the Ti atoms in subnanometer titanium oxide clusters are typically tetracoordinated, and the O atoms serve as either terminal or bridging atoms. The minimum energy Ti n O 2 n structures are in agreement with previously reported structures using numerous computational methods. ,,,,− Each Ti n O 2 n cluster contains two dangling O atoms. They are closed shell species, where all of the Ti-d electrons are transferred to the O atoms and therefore serve as models for the electronic structure of defect-free bulk titania.…”
Section: Resultssupporting
confidence: 88%
“…Far less work has been performed on the suboxide clusters, with only a few calculations previously reported. , The initial choices for the atomic coordinates for the geometrical optimization of the suboxide clusters were considered and obtained from previously published studies but optimized using the functional and basis set described in the Methods section. For instances where multiple cluster geometries were examined, we report the lowest energy geometry.…”
TD-DFT calculations were performed on neutral TinO2n, TinO2n-1, and TinO2n-2 clusters, where n ≤ 7. Our calculations show that the TinO2n clusters are closed shell systems containing empty d orbitals and that the partially filled d orbitals of the suboxide clusters have a profound effect on their structural, electronic, and topological properties. The low energy photoexcitations of TinO2n clusters are all O-2p to Ti-3d transitions, while the open-shell suboxide clusters are all characterized by d-d transitions that occur at a much smaller optical gap. Upon photoabsorption, the localization of the hole is accompanied by a local bond elongation, i.e., polaron formation, whereas d-electrons are generally delocalized among the cluster. Several of the compact of the TinO2n-2 structures contain higher symmetry which is reflected in their relative stability in the experimental cluster distribution. In particular, the tetrahedral symmetry of the optimized ground state structure for Ti4O6 inhibits charge carrier localization and therefore contains higher stability.
“…Here, each O atom changes the oxidation state of the Ti atoms linearly, from a formal oxidation state of +3 (Ti2O3) and +2 (Ti2O2) which decreases the lifetime by 15% and 26% from the stoichiometric cluster, respectively. Geometries of Ti2O4-x (x < 4) clusters are well established 31,45 (Fig. 4).…”
Section: Oxidation Effect On Suboxide Cluster Lifetimementioning
confidence: 82%
“…Here, each O atom changes the oxidation state of the Ti atoms linearly, from a formal oxidation state of +3 (Ti2O3) and +2 (Ti2O2) which decreases the lifetime by 15% and 26% from the stoichiometric cluster, respectively. Geometries of Ti2O4-x (x < 4) clusters are well established31,45 (Fig.4). Ti2O4 is the least rigid cluster (containing two terminal O) and therefore should be the easiest to traverse a conical intersection since internal…”
Excited state lifetimes of neutral titanium oxide clusters (TinO2n-x, n < 10, x < 4) were measured using a sequence of 400 nm pump and 800 nm probe femtosecond laser pulses. Despite large differences in electronic properties between the closed shell stoichiometric TinO2n clusters and the suboxide TinO2n-x (x = 1-3) clusters, the transient responses for all clusters contain a fast response of 35 fs followed by a sub-picosecond excited state lifetime. In this non-scalable size regime, subtle changes in the sub-ps lifetimes are attributed to variations in the coordination of Ti atoms and localization of charge carriers following UV photoexcitation. In general, clusters exhibit longer lifetimes with increased size and also with addition of O atoms. This suggests that removal of O atoms develops stronger Ti-Ti interactions as the system transitions from a semiconducting character into a fast metallic electronic relaxation mechanism.
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