4,046 research outputs found

    Overview of Charm Physics at RHIC

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    Heavy-quark production provides a sensitive probe of the gluon structure of nucleons and its modication in nuclei. It is also a key probe of the hot-dense matter created in heavy-ion collisions. We will discuss the physics issues involved, as seen in quarkonia and open heavy-quark production, starting with those observed in proton-proton collisions. Then cold nuclear matter effects on heavy-quark production including shadowing, gluon saturation, energy loss and absorption will be reviewed in the context of recent proton-nucleus and deuteron-nucleus measurements. Next we survey the most recent measurements of open-charm and J/Psi's in heavy-ion collisions at RHIC and their interpretation. We discuss the high-pT suppression and flow of open charm in terms of energy loss and thermalization and, for J/Psi, contrast explanations in terms of screening in a deconfined medium vs. recombination models.Comment: 6 pages, 12 figures, proceedings for Quark Confinement and Hadron Spectrum VI

    Intravenous conscious sedation in patients under 16 years of age. Fact or fiction?

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    Recently published guidelines on the use of conscious sedation in dentistry have published varying recommendations on the lower age limit for the use of intravenous conscious sedation. There are a large number of dentists currently providing dental treatment for paediatric patients under intravenous conscious sedation. The 18 cases reported here (age range 11-15 years), were successfully managed with intravenous conscious sedation. The experience in this paper is not sufficient evidence to recommend the wholesale use of intravenous conscious sedation in patients who are under 16 years. The fact that a range of operators can use these techniques on paediatric patients would suggest that further study should be carried out in this population. The guidance should be modified to say there is insufficient evidence to support the use of intravenous conscious sedation in children, rather than arbitrarily selecting a cut off point at age 16 years

    How Does ATP Regulate Erythrocyte Glucose Transport?: a Dissertation

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    Human erythrocyte glucose sugar transport displays a complexity that is not explained by available models. Sugar transport was examined in resealed red cell ghosts under equilibrium exchange conditions (intracellular [sugar] = extracellular [sugar]). Exchange 3-O-methylglucose (3MG) import and export are monophasic in the absence of cytoplasmic ATP but are biphasic when ATP is present. Biphasic exchange is observed as the rapid filling of a large compartment (66% cell volume) followed by the slow filling of the remaining cytoplasmic space. Two models for biphasic sugar transport are presented in which 3MG must overcome a sugar-specific, physical (diffusional) or chemical (anomerization) barrier to equilibrate with cell water. The anomerization model was rejected through several lines of direct experimental investigation. 1) The sizes of the fast and slow phases of sugar transport do not correlate with the equilibrium anomer distributions of all GLUT1 sugar substrates. 2) Increasing the rate of anomerization by addition of exogenous intracellular mutarotase has no effect on biphasic transport kinetics. 3) Direct measurement of initial rates of sugar uptake or exchange demonstrates that GLUT1 shows no anomer preference. The physical barrier model was further refined by the use of the counterflow condition (intracellular [sugar] \u3e\u3e extracellular [sugar]). The presence of a physical barrier alone was unable to explain the complex counterflow time courses observed. As a result, the model was modified to include the action of a specific sugar export that is compartmentalized from rapidly equilibrating, GLUT1-mediated uptake and exit

    A child learns to speak: A guide for parents to normal speech and language development

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    Optical Observations of the Binary Millisecond Pulsars J2145-0750 and J0034-0534

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    We report on optical observations of the low-mass binary millisecond pulsar systems J0034-0534 and J2145-0750. A faint (I=23.5) object was found to be coincident with the timing position of PSR J2145-0750. While a galaxy or distant main-sequence star cannot be ruled out, its magnitude is consistent with an ancient white dwarf, as expected from evolutionary models. For PSR J0034-0534 no objects were detected to a limiting magnitude of R=25.0, suggesting that the white dwarf in this system is cold. Using white dwarf cooling models, the limit on the magnitude of the PSR J0034-0534 companion suggests that at birth the pulsar in this system may have rotated with a period as short as 0.6 ms. These observations provide further evidence that the magnetic fields of millisecond pulsars do not decay on time scales shorter than 1 Gyr.Comment: 6 pages, uuencoded, gz -9 compressed postscript, accepted by ApJ

    Heavy Quarkonia Production in p+p Collisions from the PHENIX Experiment

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    Quarkonia provide a sensitive probe of the properties of the hot dense medium created in high energy heavy ion collisions. Hard scattering processes result in the production of heavy quark pairs that interact with the collision medium during hadronization. These in-medium interactions convey information about the fundamental properties of the medium itself and can be used to examine the modification of the QCD confining potential in the collision environment. Baseline measurements from p+p and d+Au collision systems are used to distinguish cold nuclear matter effects while measurements from heavy ion collision systems are used to quantify in-medium effects. The PHENIX experiment has the capability of detecting heavy quarkonia at 1.2<∣η∣<2.21.2<|\eta|<2.2 via the μ+μ−\mu^+\mu^- decay channel and at ∣η∣<0.35|\eta|<0.35 via the e+e−e^+e^- decay channel. Recent runs have resulted in the collection of high statistics p+p data sets that provide an essential baseline reference for heavy ion measurements and allow for further critical evaluation of heavy quarkonia production mechanisms. The latest PHENIX results for the production of the J/ψJ/\psi in p+p collisions are presented and future prospects for ψ′\psi', χc\chi_{c} and Υ\Upsilon measurements are discussed.Comment: 4 pages, 2 figures, Proceedings for Quark Matter 200
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