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Absorption (logic)

About: Absorption (logic) is a research topic. Over the lifetime, 5733 publications have been published within this topic receiving 236302 citations.


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TL;DR: In this paper, the authors measured the complex elastic compliance of the complex O deficiency and showed that the two main relaxation peaks in the absorption are identified with hopping of isolated O vacancies over a barrier of $0.60\phantom{\rule{0.3em}{0ex}}
Abstract: The complex elastic compliance ${s}_{11}(\ensuremath{\omega},T)$ of $\mathrm{Sr}\mathrm{Ti}{\mathrm{O}}_{3\ensuremath{-}\ensuremath{\delta}}$ has been measured as a function of the O deficiency $\ensuremath{\delta}l0.01$. The two main relaxation peaks in the absorption are identified with hopping of isolated O vacancies over a barrier of $0.60\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$ and reorientation of pairs of vacancies involving a barrier of $1\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$. The pair binding energy is $\ensuremath{\simeq}0.2\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$, and indications for additional clustering, possibly into chains, is found already at $\ensuremath{\delta}\ensuremath{\sim}0.004$. The anisotropic component of the elastic dipole of an O vacancy is $\ensuremath{\Delta}\ensuremath{\lambda}=0.026$. The possible role of electrostatic repulsion between vacancies in slowing the kinetics for their aggregation is discussed.

74 citations

Journal ArticleDOI
TL;DR: In this paper, ground-state and time-resolved excited-state spectra and fluorescence and phosphorescence spectra of three Thsup IV sandwich complexes, namely, Th{sup IV(TPP) and Th{Sup IV(OEP) are reported (OEP = 2,3,7,8,12,13,17,18,18-octaethyl porphyrinate, TPP = 5,10,15,20-tetraphenylporphyrin), in which the nitrogen planes of the two porphyrin
Abstract: Ground-state and time-resolved excited-state absorption spectra and fluorescence and phosphorescence spectra of three Th{sup IV} sandwich complexes, Th{sup IV}(TPP){sub 2}, Th{sup IV}(OEP){sub 2}, and Th{sup IV}(OEP)(TPP), are reported (OEP = 2,3,7,8,12,13,17,18-octaethylporphyrinate, TPP = 5,10,15,20-tetraphenylporphyrinate). These complexes, in which the nitrogen planes of the two porphyrin macrocycles are {approximately}2.9 {Angstrom} apart, exhibit a number of prominent optical characteristics: (1) monoporphyrin-like Q and B absorption bands, (2) a new absorption between the Q and B bands, (3) a weak, low-energy absorption that is substantially red-shifted relative to the Q bands of analogous monoporphyrin complexes, (4) fluorescence and phosphorescence emission bands that are even further red-shifted relative to typical emission bands from porphyrin monomers, and (5) a moderately intense near-infrared {sup 3}({pi},{pi}*) excited-state absorption not observed in monomeric porphyrins. These characteristic optical properties of the sandwich complexes are all accounted for by a relatively simple molecular orbital configuration-interaction model. Additionally, the spectral data and molecular orbital model identify the energies of charge-transfer configurations and delineate their contribution to the electronic states of these strongly-coupled {pi} systems. These results provide insights into the interactions that can take place between other pairs of chromophores brought within van der Waals contact, such as the bacteriochlorophyll dimermore » of the photosynthetic reaction center. 49 refs., 9 figs., 1 tab.« less

74 citations

Journal ArticleDOI
TL;DR: In this article, the unitarized model and the absorption model were evaluated for the charge transfer process with an atomic base $S$ matrix formulation represented by time-dependent bases which denote moving atomic orbitals.
Abstract: The charge-transfer process ${\mathrm{O}}^{8+}+\mathrm{H}(1s)\ensuremath{\rightarrow}{\mathrm{O}}^{7+}+{\mathrm{H}}^{+}$ is considered for ${\mathrm{O}}^{8+}$ impact energies from 0.025 to 200 keV/amu, using the atomic base $S$ matrix formulation represented by time-dependent bases which denote moving atomic orbitals. In the evaluation of the $S$ matrix, models of two extreme types, the unitarized model and the absorption model, are introduced. The numerical results show that there is only a small difference between the cross sections obtained using the respective models for impact energies above 0.5 keV/amu, while the cross section due to the unitarized model becomes smaller than one-half of that obtained with the absorption model at an impact energy of 0.05 keV/amu. The data are also compared with other calculations of the same process. For the investigation of the validity of our formula, the unitarized formula is also applied to the processes ${\mathrm{H}}^{+}+\mathrm{H}(1s)\ensuremath{\rightarrow}\mathrm{H}+{\mathrm{H}}^{+}$ and ${\mathrm{He}}^{2+}+\mathrm{H}(1s)\ensuremath{\rightarrow}{\mathrm{He}}^{+}+{\mathrm{H}}^{+}$. The results are in good agreement with the experimental data.

73 citations

Journal ArticleDOI
TL;DR: In this paper, a monoenergetic ion beam from an electrostatic accelerator strikes a thick target of the absorber, and the penetration depth is determined by a momentum analysis of mono-energetic protons elastically scattered from the target and the embedded atoms.
Abstract: The ranges of N, Ne, Ar, Kr, and Xe ions in Be, B, C, and Al have been measured to \ifmmode\pm\else\textpm\fi{}10% for incident ion energy 50-500 kev. A monoenergetic ion beam from an electrostatic accelerator strikes a thick target of the absorber, and the penetration depth is determined by a momentum analysis of monoenergetic protons elastically scattered from the target and the embedded atoms. An expression relating the penetration depth to the actual path length is derived. A linear range-energy behavior is found for Ar, Kr, and Xe ions; for N and Ne ions $\frac{\mathrm{dE}}{\mathrm{dX}}$ increases with ion energy. The experimental ranges are 20% shorter than theoretical values based on energy loss by elastic nuclear collisions. By including electronic contributions to the stopping process, good agreement with experiment is achieved.

73 citations

Journal ArticleDOI
TL;DR: The derived Pt geometric subprofile shows two discrete "outer-sphere" adsorbed layers, and the interface-specific x-ray absorption edge profile exhibits a significant white-line enhancement compared to the bulk-solution species.
Abstract: Resonant anomalous x-ray reflectivity near the Pt ${L}_{\mathrm{I}\mathrm{I}\mathrm{I}}$ edge simultaneously revealed the geometric and spectroscopic structures of $\mathrm{P}\mathrm{t}({\mathrm{N}\mathrm{H}}_{3})_{4}{}^{2+}$ ions adsorbed at the quartz(100)-water interface. The derived Pt geometric subprofile shows two discrete ``outer-sphere'' adsorbed layers, and the interface-specific x-ray absorption edge profile exhibits a significant white-line enhancement compared to the bulk-solution species.

73 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
2021290
2020249
2019220
2018230
2017162
2016163