288 research outputs found

    The measurement of the anomalous magnetic moment of the muon at fermilab

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    The anomalous magnetic moment of the muon is one of the most precisely measured quantities in experimental particle physics. Its latest measurement at Brookhaven National Laboratory deviates from the Standard Model expectation by approximately 3.5 standard deviations. The goal of the new experiment, E989, now under construction at Fermilab, is a fourfold improvement in precision. Here, we discuss the details of the future measurement and its current status

    Verallgemeinerte filternde IBLU-Zerlegungen der Ordnung l

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    Die vorliegende Arbeit befasst sich mit der Konstruktion und Analyse einer neuen Klasse frequenzfilternder IBLU-Zerlegungen für schwachbesetzte lineare Gleichungssysteme, die bei Diskretisierungen elliptischer partieller Differentialgleichungen entstehen. Die wichtigste Eigenschaft dieser Zerlegungen ist ihre Anwendbarkeit auf nicht-triviale Gebietsgeometrien. Des Weiteren werden Folgen der eingeführten Zerlegungen als frequenzfilternder Vorkonditionierer des Gradientenverfahrens für Eigenwertprobleme für elliptische Differentialoperatoren zur Beschleunigung des Lösungsprozesses verwendet

    Uncertainty quantification in coastal aquifers using the multilevel Monte Carlo method

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    We consider a class of density-driven flow problems. We are particularly interested in the problem of the salinization of coastal aquifers. We consider the Henry saltwater intrusion problem with uncertain porosity, permeability, and recharge parameters as a test case. The reason for the presence of uncertainties is the lack of knowledge, inaccurate measurements, and inability to measure parameters at each spatial or time location. This problem is nonlinear and time-dependent. The solution is the salt mass fraction, which is uncertain and changes in time. Uncertainties in porosity, permeability, recharge, and mass fraction are modeled using random fields. This work investigates the applicability of the well-known multilevel Monte Carlo (MLMC) method for such problems. The MLMC method can reduce the total computational and storage costs. Moreover, the MLMC method runs multiple scenarios on different spatial and time meshes and then estimates the mean value of the mass fraction. The parallelization is performed in both the physical space and stochastic space. To solve every deterministic scenario, we run the parallel multigrid solver ug4 in a black-box fashion. We use the solution obtained from the quasi-Monte Carlo method as a reference solution.Comment: 24 pages, 3 tables, 11 figure

    Data acquisition system for the MuLan muon lifetime experiment

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    We describe the data acquisition system for the MuLan muon lifetime experiment at Paul Scherrer Institute. The system was designed to record muon decays at rates up to 1 MHz and acquire data at rates up to 60 MB/sec. The system employed a parallel network of dual-processor machines and repeating acquisition cycles of deadtime-free time segments in order to reach the design goals. The system incorporated a versatile scheme for control and diagnostics and a custom web interface for monitoring experimental conditions.Comment: 19 pages, 8 figures, submitted to Nuclear Instruments and Methods

    Cross section of the processes e++ee++e(γ)e^++e^-\to e^++e^-(\gamma), π++π(γ)\to \pi^++\pi^-(\gamma), μ++μ(γ) \mu^++\mu^-(\gamma), γ+γ(γ) \gamma+\gamma(\gamma) in the energy region 200 MeV 2E\le 2E\le 3 GeV

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    The cross section for different processes induced by e+ee^+e^- annihilation, in the kinematical limit βμβπ=(1mπ2/ϵ2)1/21\beta_{\mu}\approx\beta_{\pi}=(1-m_{\pi}^2/\epsilon^2)^{1/2}\sim 1, is calculated taking into account first order corrections to the amplitudes and the corrections due to soft emitted photons, with energy ωΔEϵ\omega\le\Delta E\le \epsilon in the center of mass of the e+ee^+e^- colliding beams. The results are given separately for charge--odd and charge--even terms in the final channels π+π(γ)\pi^+\pi^-(\gamma) and μ+μ(γ)\mu^+\mu^-(\gamma). In case of pions, form factors are taken into account. The differential cross sections for the processes: e++ee++e(+γ)e^++e^-\to e^++e^-(+\gamma), π++π(γ)\to \pi^++\pi^-(\gamma), μ++μ(γ),γγ(γ)\to \mu^++\mu^-(\gamma),\to \gamma\gamma(\gamma) have been calculated and the corresponding formula are given in the ultrarelativistic limit s/2=ϵmμmπ\sqrt{s}/2= \epsilon \gg m_{\mu}\sim m_{\pi} . For a quantitative evaluation of the contribution of higher order of the perturbation theory, the production of π+π\pi^+\pi^-, including radiative corrections, is calculated in the approach of the lepton structure functions. This allows to estimate the precision of the obtained results as better than 0.5% outside the energy region corresponding to narrow resonances. A method to integrate the cross section, avoiding the difficulties which arise from singularities is also described.Comment: 25 pages 3 firgur

    New results on the hadronic vacuum polarization to the muon g-2

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    Results on the lowest-order hadronic vacuum polarization contribution to the muon magnetic anomaly are presented. They are based on the latest published experimental data used as input to the dispersion integral. Thus recent results on tau to nutau pi pi0 decays from Belle and on e+ e- annihilation to pi+ pi- from BABAR and KLOE are included. The new data, together with improved isospin-breaking corrections for tau decays, result into a much better consistency among the different results. A discrepancy between the Standard Model prediction and the direct g-2 measurement is found at the level of 3 sigma.Comment: proceedings of the PhiPsi09 conference, Oct. 13-16, 2009, Beijing, Chin

    Measurement of the Positive Muon Lifetime and Determination of the Fermi Constant to Part-per-Million Precision

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    We report a measurement of the positive muon lifetime to a precision of 1.0 parts per million (ppm); it is the most precise particle lifetime ever measured. The experiment used a time-structured, low-energy muon beam and a segmented plastic scintillator array to record more than 2 x 10^{12} decays. Two different stopping target configurations were employed in independent data-taking periods. The combined results give tau_{mu^+}(MuLan) = 2196980.3(2.2) ps, more than 15 times as precise as any previous experiment. The muon lifetime gives the most precise value for the Fermi constant: G_F(MuLan) = 1.1663788 (7) x 10^-5 GeV^-2 (0.6 ppm). It is also used to extract the mu^-p singlet capture rate, which determines the proton's weak induced pseudoscalar coupling g_P.Comment: Accepted for publication in Phys. Rev. Let
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