440,952 research outputs found

    Methods of Assessment and Clinical Relevance of QT Dynamics

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    The dependence on heart rate of the QT interval has been investigated for many years and several mathematical formulae have been proposed to describe the QT interval/heart rate (or QT interval/RR interval) relationship. While the most popular is Bazett’s formula, it overcorrects the QT interval at high heart rates and under-corrects it at slow heart rates. This formulae and many others similar ones, do not accurately describe the natural behaviour of the QT interval. The QT interval/RR interval relationship is generally described as QT dynamics. In recent years, several methods of its assessment have been proposed, the most popular of which is linear regression. An increased steepness of the linear QT/RR slope correlates with the risk of arrhythmic death following myocardial infarction. It has also been demonstrated that the QT interval adapts to heart rate changes with a delay (QT hysteresis) and that QT dynamics parameters vary over time. New methods of QT dynamics assessment that take into account these phenomena have been proposed. Using these methods, changes in QT dynamics have been observed in patients with advanced heart failure, and during morning hours in patients with ischemic heart disease and history of cardiac arrest. The assessment of QT dynamics is a new and promising tool for identifying patients at increased risk of arrhythmic events and for studying the effect of drugs on ventricular repolarisation

    Optimisation of variables for studying dilepton transverse momentum distributions at hadron colliders

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    In future measurements of the dilepton (Z/γZ/\gamma^*) transverse momentum, \Qt, at both the Tevatron and LHC, the achievable bin widths and the ultimate precision of the measurements will be limited by experimental resolution rather than by the available event statistics. In a recent paper the variable \at, which corresponds to the component of \Qt\ that is transverse to the dilepton thrust axis, has been studied in this regard. In the region, \Qt\ << 30 GeV, \at\ has been shown to be less susceptible to experimental resolution and efficiency effects than the \Qt. Extending over all \Qt, we now demonstrate that dividing \at\ (or \Qt) by the measured dilepton invariant mass further improves the resolution. In addition, we propose a new variable, \phistarEta, that is determined exclusively from the measured lepton directions; this is even more precisely determined experimentally than the above variables and is similarly sensitive to the \Qt. The greater precision achievable using such variables will enable more stringent tests of QCD and tighter constraints on Monte Carlo event generator tunes.Comment: 8 pages, 5 figures, 2 table

    Quiet Time for Mechanically Ventilated Patients in The Medical Intensive Care Unit

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    Objective: Sleep disruption occurs frequently in critically ill patients. The primary aim of this study was to examine the effect of quiet time (QT) on patient sedation frequency, sedation and delirium scores; and to determine if consecutive QTs influenced physiologic measures (heart rate, mean arterial blood pressure and respiratory rate). Method: A prospective study of a quiet time protocol was conducted with 72 adult patients on mechanical ventilation. Setting: A Medical Intensive Care Unit (MICU) in the Midwest region of the United States. Results: Sedation was given less frequently after QT (p = 0.045). Those who were agitated prior to QT were more likely to be at goal sedation after QT (p \u3c 0.001). Although not statistically significant, the majority of patients who were negative on the Confusion Assessment Method (CAM-ICU) prior to QT remained delirium free after QT. Repeated measures analysis of variance (ANOVA) for three consecutive QTs showed a significant difference for respiratory rate (p = 0.035). Conclusion: QT may influence sedation administration and promote patient rest. Future studies are required to further understand the influence of QT on mechanically ventilated patients in the intensive care unit

    Quantum Drinfeld Modules II: Quantum Exponential and Ray Class Fields

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    This is the second in a series of two papers presenting a solution to Manin's Real Multiplication program \cite{Man} in positive characteristic. If KK is a quadratic and real extension of Fq(T)\mathbb{F}_{q}(T) and OK\mathcal{O}_{K} is the integral closure of Fq[T]\mathbb{F}_{q}[T] in KK, we associate to each modulus MOK\mathfrak{M}\subset \mathcal{O}_{K} the {\it unit narrow ray class field} KMK^{\mathfrak{M}}: a class field containing the narrow ray class field, whose class group contains an additional contribution coming from OK×\mathcal{O}^{\times}_{K}. For fKf\in K a fundamental unit, we introduce the associated {\it quantum Drinfeld module} ρfqt\rho^{\rm qt}_{f} of ff: a generalization of Drinfeld module whose elements are multi-points. The main theorem of the paper is that KM=HOK(Tr(ρfqt[M]),Tr(ρf1qt[M])) K^{\mathfrak{M}}=H_{\mathcal{O}_{K}} ( {\sf Tr}(\rho^{\rm qt}_{f}[\mathfrak{M}]), {\sf Tr}(\rho^{\rm qt}_{f^{-1}}[\mathfrak{M}])) where HOKH_{\mathcal{O}_{K}} is the Hilbert class field of OK\mathcal{O}_{K} and Tr(ρfqt[M]){\sf Tr}(\rho^{\rm qt}_{f}[\mathfrak{M}]), Tr(ρf1qt[M]){\sf Tr}(\rho^{\rm qt}_{f^{-1}}[\mathfrak{M}]) are the groups of traces of M\mathfrak{M} torsion points of ρfqt\rho^{\rm qt}_{f}, ρf1qt\rho^{\rm qt}_{f^{-1}}.Comment: 41 page

    Vector boson production at hadron colliders: transverse-momentum resummation and leptonic decay

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    We consider the transverse-momentum (qT ) distribution of Drell-Yan lepton pairs produced, via W and Z/γ∗ decay, in hadronic collisions. At small values of qT , we resum the logarithmically-enhanced perturbative QCD contributions up to next-to-next- to-leading logarithmic accuracy. Resummed results are consistently combined with the known O(αS2 ) fixed-order results at intermediate and large values of qT . Our calculation includes the leptonic decay of the vector boson with the corresponding spin correlations, the finite-width effects and the full dependence on the final-state lepton(s) kinematics. The computation is encoded in the numerical program DYRes, which allows the user to apply arbitrary kinematical cuts on the final-state leptons and to compute the corresponding distributions in the form of bin histograms. We present a comparison of our results with some of the available LHC data. The inclusion of the leptonic decay in the resummed cal- culation requires a theoretical discussion on the qT recoil due to the transverse momentum of the produced vector boson. We present a qT recoil procedure that is directly applica- ble to qT resummed calculations for generic production processes of high-mass systems in hadron collisions.Fil: Catani, Estefano. Universita Degli Studi Di Firenze; ItaliaFil: de Florian, Daniel Enrique. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Departamento de Física; Argentina. Universidad Nacional de San Martín. Escuela de Ciencia y Tecnología. Centro Internacional de Estudios Avanzados; ArgentinaFil: Ferrera, Giancarlo. Università degli Studi di Milano; ItaliaFil: Grazzini, Massimiliano. Universitat Zurich; Suiz
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