3,420 research outputs found

    Linkage and association analyses of microsatellites and single-nucleotide polymorphisms in nuclear families

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    Several simulation studies have suggested that a high-density single-nucleotide polymorphisms (SNPs) marker set may be as useful as a traditional microsatellites (MS) marker set in performing whole-genome linkage analysis. However, very few studies have directly tested the SNPs-based genome-wide scan. In the present study, we compared the linkage results from the SNPs-based scan with a map density of 3-cM spacing with those from the MS scan using a 10-cM marker set among 300 nuclear families each from the Aipotu (AI), Danacaa (DA), and Karangar (KA) populations from the simulated Genetic Analysis Workshop 14 Problem 2 data. We found that information contents obtained from the SNPs scan were somewhat lower than those from the MS scan. However, the linkage results obtained from the two scans showed a high degree of similarity. Both scans identified a similar number of chromosomal regions attaining nominal significance (p < 0.05). Specifically, both scans detected confirmed evidence for linkage (NPL β‰₯ 4.07, p = 2 Γ— 10(-5)) to chromosome 1 in the AI families, chromosomes 1 and 3 in the DA families, and chromosomes 3, 5, and 9 in the KA families. An additional confirmed linkage to chromosome 5 in the AI families was detected only by the MS scan. We also observed slightly wider 1-LOD intervals for more of the SNP peaks than for the MS peaks, which is likely due to lower information contents for the SNPs. Subsequent fine-mapping association analysis further identified 2 to 3 markers significantly associated with disease status in each population; B03T3056, B03T3058, and B05T4139 in the AI population, B03T3056 and B03T3058 in the KA population, and B03T3056, B03T3057, and B03T3058 in the DA population. Among the four markers, three were chosen based on results obtained from the two scans, but one was solely from the SNP scan. In summary, our finding suggests that the SNP-based genome scan has the potential to be as powerful as the traditional MS-based scan and offers good identification of peak location for further fine-mapped association analysis

    Anomalous gauge couplings of the Higgs boson at the CERN LHC: Semileptonic mode in WW scatterings

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    We make a full tree level study of the signatures of anomalous gauge couplings of the Higgs boson at the CERN LHC via the semileptonic decay mode in WW scatterings. Both signals and backgrounds are studied at the hadron level for the Higgs mass in the range 115 GeV to 200 GeV. We carefully impose suitable kinematical cuts for suppressing the backgrounds. To the same sensitivity as in the pure leptonic mode, our result shows that the semileptonic mode can reduce the required integrated luminosity by a factor of 3. If the anomalous couplings in nature are actually larger than the sensitivity bounds shown in the text, the experiment can start the test for an integrated luminosity of 50 inverse fb.Comment: PACS numbers updated. Version published in Phys.Rev.D79,055010(2009

    Average AoI Minimization for Energy Harvesting Relay-aided Status Update Network Using Deep Reinforcement Learning

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    A dual-hop status update system aided by energy harvesting (EH) relays with finite data and energy buffers is studied in this work. To achieve timely status updates, the best relays should be selected to minimize the average age of information (AoI), which is a recently proposed metric to evaluate information freshness. The average AoI minimization can be formulated as a Markov decision process (MDP), but the state space for capturing channel and buffer evolution grows exponentially with the number of relays, leading to high solution complexity. We propose a relay selection (RS) scheme based on deep reinforcement learning (DRL) according to the instantaneous channel packet freshness and buffer information of each relay. Simulation results show a significant improvement of the proposed DRL-based RS scheme over state-of-art approaches.Comment: This article has been accepted for publication in IEEE Wireless Communications Letters. Citation information: DOI 10.1109/LWC.2023.327886

    Dynamic Magneto-Conductance Fluctuations and Oscillations in Mesoscopic Wires and Rings

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    Using a finite-frequency recursive Green's function technique, we calculate the dynamic magneto-conductance fluctuations and oscillations in disordered mesoscopic normal metal systems, incorporating inter-particle Coulomb interactions within a self-consistent potential method. In a disordered metal wire, we observe ergodic behavior in the dynamic conductance fluctuations. At low Ο‰\omega, the real part of the conductance fluctuations is essentially given by the dc universal conductance fluctuations while the imaginary part increases linearly from zero, but for Ο‰\omega greater than the Thouless energy and temperature, the fluctuations decrease as Ο‰βˆ’1/2\omega^{-1/2}. Similar frequency-dependent behavior is found for the Aharonov-Bohm oscillations in a metal ring. However, the Al'tshuler-Aronov-Spivak oscillations, which predominate at high temperatures or in rings with many channels, are strongly suppressed at high frequencies, leading to interesting crossover effects in the Ο‰\omega-dependence of the magneto-conductance oscillations.Comment: 4 pages, REVTeX 3.0, 5 figures(ps file available upon request), #phd0

    Understanding the e+eβˆ’β†’D(βˆ—)+D(βˆ—)βˆ’e^+e^-\to D^{(*)+}D^{(*)-} processes observed by Belle

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    We calculate the production cross sections for Dβˆ—+Dβˆ—βˆ’D^{*+}D^{*-}, D+Dβˆ—βˆ’D^+D^{*-} and D+Dβˆ’D^+D^- in e+eβˆ’e^+e^- annihilation through one virtual photon in the framework of perturbative QCD with constituent quarks. The calculated cross sections for Dβˆ—+Dβˆ—βˆ’D^{*+}D^{*-} and D+Dβˆ—βˆ’D^+D^{*-} production are roughly in agreement with the recent Belle data. The helicity decomposition for Dβˆ—D^{*} meson production is also calculated. The fraction of the DLβˆ—Β±DTβˆ—βˆ“D^{*\pm}_LD^{*\mp}_T final state in e+eβˆ’β†’Dβˆ—+Dβˆ—βˆ’e^+e^-\to D^{*+}D^{*-} process is found to be 65%. The fraction of DDTβˆ—DD^*_T production is 100% and DDLβˆ—DD^*_L is forbidden in e+eβˆ’e^+e^- annihilation through one virtual photon. We further consider e+eβˆ’e^+e^- annihilation through two virtual photons, and then find the fraction of DDTβˆ—DD^{*}_T in e+eβˆ’β†’DDβˆ—e^+e^-\to DD^{*} process to be about 91%.Comment: 8 pages, 2 figure
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