967 resultados para Three body charge transfer reaction
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The effects of gamma irradiation on as-grown 5 at% Yb:YAlO3 (YAP) and air annealing on gamma-irradiated 5 at% Yb: YAP have been studied by the difference in the absorption spectra before and after treatment. The gamma irradiation and air annealing led to opposite changes of the absorption properties of the Yb: YAP crystal. After air annealing, the gamma-irradiation effects were totally removed over the wavelength range 390-800 nm and the concentrations of Fe3+ and Yb3+ were slightly increased. For the first time, the gamma-irradiation-induced valence changes between Yb3+ and Yb2+ ions in Yb: YAP crystals have been observed. (c) 2005 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
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Transparent polycrystalline MgO and TiO2 codoped Al2O3 ceramics were fabricated by conventional solid-state pressureless processing. The absorption, emission and excitation spectra of ( Mg, Ti : Al2O3 ceramics were measured. Owing to charge compensation of Mg2+, only UV absorption around 250nm was observed due to O2- -> Ti4+ charge transfer transitions (CT) when Ti content was low. As a result, the emission peaks of isolated Ti4+ ion located at 280-290nm and 410-420nm were observed. Besides absorption peak of V, ion, the characteristic absorption peak of V, ion centered at 490nm was observed in Mg, Ti) : Al2O3 ceramics when Ti content was high. The emission spectra of Ti3+, ion in polycrystalline Al2O3 ceramics coincide with that of Ti: Al2O3 single crystal.
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Hybrid quantum mechanics/molecular mechanics (QM/MM) simulations provide a powerful tool for studying chemical reactions, especially in complex biochemical systems. In most works to date, the quantum region is kept fixed throughout the simulation and is defined in an ad hoc way based on chemical intuition and available computational resources. The simulation errors associated with a given choice of the quantum region are, however, rarely assessed in a systematic manner. Here we study the dependence of two relevant quantities on the QM region size: the force error at the center of the QM region and the free energy of a proton transfer reaction. Taking lysozyme as our model system, we find that in an apolar region the average force error rapidly decreases with increasing QM region size. In contrast, the average force error at the polar active site is considerably higher, exhibits large oscillations and decreases more slowly, and may not fall below acceptable limits even for a quantum region radius of 9.0 A. Although computation of free energies could only be afforded until 6.0 A, results were found to change considerably within these limits. These errors demonstrate that the results of QM/MM calculations are heavily affected by the definition of the QM region (not only its size), and a convergence test is proposed to be a part of setting up QM/MM simulations.
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In this paper, some results on visible luminescence performed on Yb3+-doped gadolinium gallium garnets under 165 and 940 nm excitation were presented. The upconversion luminescence was ascribed to Yb3+ cooperative luminescence and the presence of rare earth impurity ions. The gain cross-sections of Yb:GGG crystal as a function of excited-state population fraction P were studied. Emission spectra under 165 nm at 20 K showed there was no charge transfer luminescence in Yb:GGG. (c) 2006 Elsevier B.V. All rights reserved.
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The TiOx thin films were prepared by electron beam evaporation using TiO as the starting material. The effect of the annealing temperature on the optical and electrical properties was investigated. The spectra of X-ray photoelectron spectroscopy reveal that Ti in the films mainly exist in the forms of Ti2+ and Ti3+ below 400 degrees C 24h annealing. The charge transfer between different titanium ion contribute greatly to the color, absorption, and electrical resistance of the films. (c) 2006 Elsevier Ltd. All rights reserved.
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Comunicación a congreso (póster): 11th European Biological Inorganic Chemistry Conference EUROBIC 11. 12-16 September, 2012 - Granada (Spain)
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A developmental series of larval and pelagic juvenile pygmy rockfish (Sebastes wilsoni) from central California is illustrated and described. Sebastes wilsoni is a non- commercially, but ecologically, important rockfish, and the ability to differentiate its young stages will aid researchers in population abundance studies. Pigment patterns, meristic characters, morphometric measurements, and head spination were recorded from specimens that ranged from 8.1 to 34.4 mm in standard length. Larvae were identified initially by meristic characters and the absence of ventral and lateral midline pigment. Pelagic juveniles developed a prominent pigment pattern of three body bars that did not extend to the ventral surface. Species identification was confirmed subsequently by using mitochondrial sequence data of four representative specimens of various sizes. As determined from the examination of otoliths, the growth rate of larval and pelagic juvenile pygmy rockfish was 0.28 mm/day, which is relatively slow in comparison to the growth rate of other species of Sebastes. These data will aid researchers in determining species abundance.
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Recently, experimental evidence was presented which suggests that as the stoichiometric composition CuTe, NiTe, Tl//2Te and MnTe are approached from pure Te in the liquid state, substantial charge transfer takes place and Te exists in the form Te**y**31 ions with y close to 2. The system studied (Te-Tl) is one in which charge transfer localizes electrons on the tellurium and leads to semiconducting behavior at the stoichiometric composition Tl//2Te.
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光系统II(PSII)是存在于类囊体膜中的多亚基色素蛋白复合物,是吸收光能、催化光诱导水裂解释放氧气、质子和电子的重要机构。它在体内的基本单位是由外周天线蛋白(LHCII)与PSII核心复合物结合形成的PSII-LHCII超分子复合物,这一结构保证了LHCII吸收的能量能够快速有效的传递到PSII反应中心(RC),进行原初光化学反应。 本论文分为两部分:1、利用捕光色素蛋白复合物(LHCII)与PSII核心复合物在以DGDG、PG、SQDG三种类囊体膜脂形成的脂质体中重组的方法,研究了LHCII与PSII在脂膜上结构与功能的相互作用;2、通过研究光破坏和色素置换对PSII RC的影响,探讨了RC中不同色素的功能。主要结果如下: 1、LHCII与PSII核心复合物的蛋白脂质体研究: 将OECC(粗提核心复合物)、pdOE(纯化核心复合物)、LHCII(大量天线)制剂分别与脂质体重组并研究了其光谱性质。LHCII在与脂质体重组前表现出典型的聚集态光谱特征,重组后吸收和荧光发射峰发生明显蓝移;LHCII、OECC和pdOE三种蛋白脂质体与重组前的样品相比荧光发射强度增加;表明脂环境影响了色素蛋白复合物的聚集状态以及色素和蛋白之间的相互作用。 OECC和pdOE分别与LHCII在脂质体中重组,得到两种重组蛋白(LHCII-OECC和LHCII-pdOE)脂质体,用冰冻蚀刻电镜技术和低温荧光光谱的方法研究其结构和功能特征。LHCII和核心复合物(OECC或pdOE)结合形成PSII-LHCII重组颗粒,并在脂质体中均匀排布,阻止了LHCII晶格状结构的形成。重组蛋白脂质体的吸收光谱既有LHCII的吸收特征,又有核心复合物的特征吸收峰,但低温荧光光谱的主要发射峰是核心复合物的特征峰(684 nm-685 nm),而不是LHCII的特征峰(680 nm);而且激发不同色素得到的荧光发射光谱基本一致,这些结果证明LHCII吸收的能量传递到了核心复合物中,在重组蛋白脂质体中不同色素蛋白复合物在结构和功能上都实现了相互偶联。 通过对OECC或pdOE与LHCII重组形成的蛋白脂质体放氧或DCPIP光还原活性的检测研究了PSII光化学活性特征。LHCII和核心复合物(OECC或pdOE)的重组蛋白脂质体与单独核心脂质体相比,在强光和弱光下光化学活性都明显提高。这从另一个角度证明了核心复合物与LHCII的功能偶联,LHCII的结合使捕光截面积增大,从而使PSII光化学活性增加。 用77K飞秒时间分辨荧光光谱分析了几种蛋白脂质体的能量传递和捕获情况。LHCII、OECC和pdOE三种蛋白脂质体的主要荧光衰减组分分别是670 ps(发射峰在680 nm)、650 ps(发射峰在690 nm)和570 ps(发射峰在685 nm)。LHCII-OECC和LHCII-pdOE脂质体的主要衰减组分分别是940 ps(发射峰在690 nm)和840 ps(发射峰在685 nm),并且出现了一个在核心复合物脂质体和LHCII脂质体中没有的40 ps组分,可以推测,这是LHCII和核心复合物之间达到平衡的时间组分,比激发态衰减的平均寿命要快得多,因此支持了PSII的trap-limited激发能衰减动力学模型。此外,可以看到天线的增大使Chl a荧光衰减的寿命延长,这一特性可能与PSII的光保护机制有关。 LHCII和OECC、LHCII和pdOE在脂质体中都成功的实现了重组,而且在结构和功能上没有明显差异;表明小天线以及23 kDa、17 kDa蛋白可能不是LHCII和核心复合物结合及能量传递所必需的。 2、受体侧光破坏和色素置换对PSII RC的影响: 在800 μmol.m-2 .s-1光照和无外加电子受体、供体的情况下,研究了PSII RC色素的受体侧光破坏情况。Chl a、Pheo和β-Car的光漂白几乎同时发生,其中在680 nm吸收的色素破坏最为显著,670 nm吸收的外周Chl比其他色素更加稳定。荧光发射强度呈先升高后降低的趋势,最大发射峰位逐渐蓝移,表明色素之间的能量传递受到破坏。用β-Car的主要吸收波长488 nm和514.5 nm激发得到两组谱带峰位和强度不同的拉曼光谱,表明在PSII RC中存在两个光谱性质不同的β-Car。光破坏过程中两组谱带的位置和带宽都没有明显变化,表明β-Car的光保护机制不涉及自身构象的变化。 将PSII RC与Cu-Chl a进行色素置换,得到了与Cu-Chl重组的RC(Cu-Chl-RC),含有0.5 Cu-Chl/2Pheo。与对照RC(按同样方式与Chl a置换的RC)和天然RC相比,Cu-Chl含量增加而Chl含量减少,660 nm的吸收增加而670 nm吸收降低,因此推测是外周Chl被替换。色素置换过程对RC的多肽组分及大部分的P680活性没有影响,CD光谱的变化也很小,表明产生CD信号的色素和蛋白环境也没有受到明显影响。但是Cu-Chl-RC的荧光发射强度明显降低,最大发射峰蓝移且峰形发生变化,Cu-Chl可能在重组RC中作为激发态的淬灭剂,阻碍了色素之间的能量传递。
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A fully integrated 0.18 μm DC-DC buck converter using a low-swing "stacked driver" configuration is reported in this paper. A high switching frequency of 660 MHz reduces filter components to fit on chip, but this suffers from high switching losses. These losses are reduced using: 1) low-swing drivers; 2) supply stacking; and 3) introducing a charge transfer path to deliver excess charge from the positive metal-oxide semiconductor drive chain to the load, thereby recycling the charge. The working prototype circuit converts 2.2 to 0.75-1.0 V at 40-55 mA. Design and simulation of an improved circuit is also included that further improves the efficiency by enhancing the charge recycling path, providing automated zero voltage switching (ZVS) operation, and synchronizing the half-swing gating signals. © 2009 IEEE.
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The effect of KI encapsulation in narrow (HiPCO) single-walled carbon nanotubes is studied via Raman spectroscopy and optical absorption. The analysis of the data explores the interplay between strain and structural modifications, bond-length changes, charge transfer, and electronic density of states. KI encapsulation appears to be consistent with both charge transfer and strain that shrink both the C-C bonds and the overall nanotube along the axial direction. The charge transfer in larger semiconducting nanotubes is low and comparable with some cases of electrochemical doping, while optical transitions between pairs of singularities of the density of states are quenched for narrow metallic nanotubes. Stronger changes in the density of states occur in some energy ranges and are attributed to polarization van der Waals interactions caused by the ionic encapsulate. Unlike doping with other species, such as atoms and small molecules, encapsulation of inorganic compounds via the molten-phase route provides stable effects due to maximal occupation of the nanotube inner space.
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The electronic and magnetic properties of the transition metal sesqui-oxides Cr(2)O(3), Ti(2)O(3), and Fe(2)O(3) have been calculated using the screened exchange (sX) hybrid density functional. This functional is found to give a band structure, bandgap, and magnetic moment in better agreement with experiment than the local density approximation (LDA) or the LDA+U methods. Ti(2)O(3) is found to be a spin-paired insulator with a bandgap of 0.22 eV in the Ti d orbitals. Cr(2)O(3) in its anti-ferromagnetic phase is an intermediate charge transfer Mott-Hubbard insulator with an indirect bandgap of 3.31 eV. Fe(2)O(3), with anti-ferromagnetic order, is found to be a wide bandgap charge transfer semiconductor with a 2.41 eV gap. Interestingly sX outperforms the HSE functional for the bandgaps of these oxides.
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In this letter we report a facile one-pot synthesis of intercalated ZnO particles for inexpensive, low-temperature solution processed dye-sensitised solar cells. High interconnectivity facilitates enhanced charge transfer between the ZnO nanoparticles and a consequent enhancement in cell efficiency. ZnO thin films were formed from a wide range of nanoparticle diameters which simultaneously increased optical scattering whilst enhancing dye loading. A possible growth mechanism was proposed for the synthesis of ZnO nanoparticles. The intercalated ZnO nanoparticle thin films were integrated into the photoanodes of dye-sensitised solar cells which showed an increase in performance of 37% compared to structurally equivalent cells employing ZnO nanowires. © 2012 Elsevier B.V.
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Graphene is used as the thinnest possible spacer between gold nanoparticles and a gold substrate. This creates a robust, repeatable, and stable sub-nanometre gap for massive plasmonic field enhancements. White light spectroscopy of single 80 nm gold nanoparticles reveals plasmonic coupling between the particle and its image within the gold substrate. While for a single graphene layer, spectral doublets from coupled dimer modes are observed shifted into the near infra-red, these disappear for increasing numbers of layers. These doublets arise from plasmonic charge transfer, allowing the direct optical measurement of out-of-plane conductivity in such layered systems. Gating the graphene can thus directly produce plasmon tuning.
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We describe studies of new nanostructured materials consisting of carbon nanotubes wrapped in sequential coatings of two different semiconducting polymers, namely, poly(3-hexylthiophene) (P3HT) and poly(9,9'-dioctylfluorene-co-benzothiadiazole) (F8BT). Using absorption spectroscopy and steady-state and ultrafast photoluminescence measurements, we demonstrate the role of the different layer structures in controlling energy levels and charge transfer in both solution and film samples. By varying the simple solution processing steps, we can control the ordering and proportions of the wrapping polymers in the solid state. The resulting novel coaxial structures open up a variety of new applications for nanotube blends and are particularly promising for implementation into organic photovoltaic devices. The carbon nanotube template can also be used to optimize both the electronic properties and morphology of polymer composites in a much more controlled fashion than achieved previously, offering a route to producing a new generation of polymer nanostructures.