9,359 research outputs found

    A robotic platform for high-throughput electrochemical analysis of chalcopyrite leaching

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    A novel robotic platform for combinatorial screening of ionic liquid-based Cu extraction from chalcopyrite with real-time, in situ monitoring of dissolved copper.</p

    Home care: a review of effectiveness and outcomes

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    Comment on the Nature of the Ds1(2710)D_{s1}^*(2710) and DsJ(2860)D_{sJ}^*(2860) Mesons

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    Two charm-strange mesons, the Ds1(2710)D_{s1}^*(2710) and the DsJ(2860)D_{sJ}^*(2860), have recently been observed by several experiments. There has been speculation in the literature that the Ds1(2710)D_{s1}^*(2710) is the 23S1(csˉ)2^3S_1(c\bar{s}) state and the DsJ(2860)D_{sJ}^*(2860) is the 13D1(csˉ)1^3D_1(c\bar{s}) state. In this paper we explore this and other explanations in the context of the relativized quark model and the pseudoscalar emission decay model. We conclude that the Ds1(2710)D_{s1}^*(2710) is most likely the 13D1(csˉ)1^3D_1 (c\bar{s}) state and the DsJ(2860)D_{sJ}^*(2860) is most likely the 13D3(csˉ)1^3D_3 (c\bar{s}) state with the 1D21D_2 resonances also contributing to the observed signals and explaining the observed ratios of branching ratios to DKD^*K and DKDK final states. We point out that measuring the DsJ(2860)D_{sJ}^*(2860) spin can support or eliminate this explanation and that there are six excited DsD_s states in this mass region; the 23S12^3S_1, 21S02^1S_0, 13D11^3D_1, 13D31^3D_3 and two 1D21D_2 states. Observing some of the missing states would help confirm the nature of the Ds1(2710)D_{s1}^*(2710) and the DsJ(2860)D_{sJ}^*(2860) states.Comment: 8 pages, 2 figure

    Emotional and psychosomatic disorders in general practice

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    The knowledge of the genesis of emotional and psychosomatic illnesses is of paramount importance in medicine. This paper is an attempt to obtain a perspective of the problem as it presents itself to the general practitioner. It consists of (a), a study of the incidence of emotional and psychosomatic illnesses in general practice, and (b) of a study of the causes of such illnesses. 950 cases were studied consecutively in the month of November, 1969 as they attended the office. A case would be classified as psychosomatic on 3 conditions: (1) The condition must belong to one of those listed as possibly psychosomatic. (2) The patient must admit to an emotional disturbance. (3) The emotional disturbance must precede the somatic condition. In this study an attempt was made to trace the relationship between life events and emotional illness. According to this study the catastrophic events are: ill-health in a household member, bereavement, son or daughter leaving home, demotion or loss of a job, menopause, alcoholic spouse, and separation from parents or next of kin.peer-reviewe

    Influence of reheating on the trispectrum and its scale dependence

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    We study the evolution of the non-linear curvature perturbation during perturbative reheating, and hence how observables evolve to their final values which we may compare against observations. Our study includes the evolution of the two trispectrum parameters, \gnl and \taunl, as well as the scale dependence of both \fnl and \taunl. In general the evolution is significant and must be taken into account, which means that models of multifield inflation cannot be compared to observations without specifying how the subsequent reheating takes place. If the trispectrum is large at the end of inflation, it normally remains large at the end of reheating. In the classes of models we study, it is very hard to generate \taunl\gg\fnl^2, regardless of the decay rates of the fields. Similarly, for the classes of models in which \gnl\simeq\taunl during slow--roll inflation, we find the relation typically remains valid during reheating. Therefore it is possible to observationally test such classes of models without specifying the parameters of reheating, even though the individual observables are sensitive to the details of reheating. It is hard to generate an observably large \gnl however. The runnings, \nfnl and \ntaunl, tend to satisfy a consistency relation \ntaunl=(3/2)\nfnl, but are in general too small to be observed for the class of models considered regardless of reheating timescale

    Comment on ZZ''s and the H1 and ZEUS High Q2Q^2 Anomalies

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    We investigate the effects of extra neutral gauge bosons on the high Q2Q^2 region of the e+pe+Xe^+p \to e^+ X cross section at s=300\sqrt{s}=300 GeV. We found that the only models with electroweak strength coupling, typical of extended gauge theories, that give a better fit to the H1 and ZEUS high Q2Q^2 data than the standard model, are ruled out by existing data from the Tevatron. From general scaling arguments, using the allowed contact interactions, the only allowed models with ZZ''s would be those with strong couplings although even in this case the statistical evidence is not compelling.Comment: Latex file uses revtex version 3, epsfig, 1 postscript figure is attache

    Very high energy gamma rays from the Crab Nebula

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    Observations of the Crab pulsar using the atmospheric Cerenkov technique were conducted for 22 hours. The light curve obtained shows a single peak at approximately the position of the expected main peak with a significance level of 3.2 sigma. The pulsed flux above 200 GeV is 2.5 + or - 0.8 x 10 to the 11th power cm(-2)s(-1)
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