1,345 research outputs found

    Growth of sulphuric acid nanoparticles under wet and dry conditions

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    New particle formation, which greatly influences the number concentrations and size distributions of an atmospheric aerosol, is often followed by a rapid growth of freshly formed particles. The initial growth of newly formed aerosol is the crucial process determining the fraction of nucleated particles growing to cloud condensation nuclei sizes, which have a significant influence on climate. In this study, we report the laboratory observations of the growth of nanoparticles produced by nucleation of H<sub>2</sub>SO<sub>4</sub> and water in a laminar flow tube at temperatures of 283, 293 and 303 K, under dry (a relative humidity of 1%) and wet conditions (relative humidity of 30%) and residence times of 30, 45, 60 and 90 s. The initial H<sub>2</sub>SO<sub>4</sub> concentration spans the range from 2 × 10<sup>8</sup> to 1.4 × 10<sup>10</sup> molecule cm<sup>−3</sup> and the calculated wall losses of H<sub>2</sub>SO<sub>4</sub> were assumed to be diffusion limited. The detected particle number concentrations, measured by the Ultrafine Condensation Particle Counter (UCPC) and Differential Mobility Particle Sizer (DMPS), were found to depend strongly on the residence time. Hygroscopic particle growth, presented by growth factors, was found to be in good agreement with the previously reported studies. The experimental growth rates ranged from 20 nm h<sup>−1</sup> to 890 nm h<sup>−1</sup> at relative humidity (RH) 1% and from 7 nm h<sup>−1</sup> to 980 nm h<sup>−1</sup> at RH 30% and were found to increase significantly with the increasing concentration of H<sub>2</sub>SO<sub>4</sub>. Increases in the nucleation temperature had a slight enhancing effect on the growth rates under dry conditions. The influence of relative humidity on growth was not consistent – at lower H<sub>2</sub>SO<sub>4</sub> concentrations, the growth rates were higher under dry conditions while at H<sub>2</sub>SO<sub>4</sub> concentrations greater than 1 × 10<sup>10</sup> molecule cm<sup>−3</sup>, the growth rates were higher under wet conditions. The growth rates show only a weak dependence on the residence time. The experimental observations were compared with predictions made using a numerical model, which investigates the growth of particles with three different extents of neutralization by ammonia, NH<sub>3</sub>: (1) pure H<sub>2</sub>SO<sub>4</sub> – H<sub>2</sub>O particles; (2) particles formed by ammonium bisulphate, (NH<sub>4</sub>)HSO<sub>4</sub>; (3) particles formed by ammonium sulphate, (NH<sub>4</sub>)<sub>2</sub>SO<sub>4</sub>. The highest growth rates were found for ammonium sulphate particles. Since the model accounting for the initial H<sub>2</sub>SO<sub>4</sub> concentration predicted the experimental growth rates correctly, our results suggest that the commonly presumed diffusional wall losses of H<sub>2</sub>SO<sub>4</sub> in case of long-lasting experiments are not so significant. We therefore assume that there are not only losses of H<sub>2</sub>SO<sub>4</sub> on the wall, but also a flux of H<sub>2</sub>SO<sub>4</sub> molecules from the wall into the flow tube, the effect being more profound under dry conditions and at higher temperatures of the tube wall. Based on a comparison with the atmospheric observations, our results indicate that sulphuric acid alone cannot explain the growth rates of particles formed in the atmosphere

    Risico's van bodemverontreiniging in het landelijk gebied; bodemkwaliteitskaarten, risico's voor de voedselveiligheid, actief bodembeheer en beslissingsondersteunende systemen

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    Dit rapport bevat achtergrondinformatie over de aanpak en resultaten van onderzoek naar bodemkwaliteitskaarten met daarop de gehalten en de risico's van zware metalen; de risico's van bodemverontreiniging voor gewaskwaliteit en diergezondheid; de effecten van veranderend landgebruik op bodemkwaliteit, bodemleven en hogere flora en fauna; de mogelijkheden van fytoremediëring voor het beheersen en terugdringen van risico's van bodemverontreiniging; verificatieonderzoek in verband met de toepassing van actief bodembeheer in de Krimpenerwaard; en ontwikkeling en toepassing van een beslissingondersteunend systeem voor inrichting en beheer van gronden voor natuurontwikkeling. De informatie in dit rapport is gebaseerd op artikelen die reeds toegestuurd zijn dan wel spoedig toegestuurd worden naar populair-wetenschappelijke tijdschriften

    An accurate description of quantum size effects in InP nanocrystallites over a wide range of sizes

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    We obtain an effective parametrization of the bulk electronic structure of InP within the Tight Binding scheme. Using these parameters, we calculate the electronic structure of InP clusters with the size ranging upto 7.5 nm. The calculated variations in the electronic structure as a function of the cluster size is found to be in excellent agreement with experimental results over the entire range of sizes, establishing the effectiveness and transferability of the obtained parameter strengths.Comment: 9 pages, 3 figures, pdf file available at http://sscu.iisc.ernet.in/~sampan/publications.htm

    Increased susceptibility to proactive interference in adults with dyslexia?

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    Recent findings show that people with dyslexia have an impairment in serial-order memory. Based on these findings, the present study aimed to test the hypothesis that people with dyslexia have difficulties dealing with proactive interference (PI) in recognition memory. A group of 25 adults with dyslexia and a group of matched controls were subjected to a 2-back recognition task, which required participants to indicate whether an item (mis)matched the item that had been presented 2 trials before. PI was elicited using lure trials in which the item matched the item in the 3-back position instead of the targeted 2-back position. Our results demonstrate that the introduction of lure trials affected 2-back recognition performance more severely in the dyslexic group than in the control group, suggesting greater difficulty in resisting PI in dyslexia.Peer reviewedFinal Accepted Versio

    Evolution of the electronic structure with size in II-VI semiconductor nanocrystals

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    In order to provide a quantitatively accurate description of the band gap variation with sizes in various II-VI semiconductor nanocrystals, we make use of the recently reported tight-binding parametrization of the corresponding bulk systems. Using the same tight-binding scheme and parameters, we calculate the electronic structure of II-VI nanocrystals in real space with sizes ranging between 5 and 80 {\AA} in diameter. A comparison with available experimental results from the literature shows an excellent agreement over the entire range of sizes.Comment: 17 pages, 4 figures, accepted in Phys. Rev.

    Multiband theory of quantum-dot quantum wells: Dark excitons, bright excitons, and charge separation in heteronanostructures

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    Electron, hole, and exciton states of multishell CdS/HgS/CdS quantum-dot quantum well nanocrystals are determined by use of a multiband theory that includes valence-band mixing, modeled with a 6-band Luttinger-Kohn Hamiltonian, and nonparabolicity of the conduction band. The multiband theory correctly describes the recently observed dark-exciton ground state and the lowest, optically active, bright-exciton states. Charge separation in pair states is identified. Previous single-band theories could not describe these states or account for charge separation.Comment: 10 pages of ReVTex, 6 ps figures, submitted to Phys. Rev.

    Theory of Luminescent Emission in Nanocrystal ZnS:Mn with an Extra Electron

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    We consider the effect of an extra electron injected into a doped quantum dot ZnS:Mn2+ZnS:Mn^{2+}. The Coulomb interaction and the exchange interaction between the extra electron and the states of the Mn ion will mix the wavefunctions, split the impurity energy levels, break the previous selection rules and change the transition probabilities. Using this model of an extra electron in the doped quantum dot, we calculated the energy and the wavefunctions, the luminescence probability and the transition lifetime and compare with the experiments. Our calculation shows that two orders of magnitudes of lifetime shortening can occur in the transition 4T1−6A1^4T_1-^6A_1 when an extra electron is present.Comment: 15 pages, 2 Figs No change in Fig
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