620 research outputs found

    The membrane protein MiRP3 regulates Kv4.2 channels in a KChIP‐dependent manner

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    MiRP3, the single-span membrane protein encoded by KCNE4, is localized by immunofluorescence microscopy to the transverse tubules of murine cardiac myocytes. MiRP3 is found to co-localize with Kv4.2 subunits that contribute to cardiac transient outward potassium currents (I(to)). Whole-cell, voltage-clamp recordings of human MiRP3 and Kv4.2 expressed in a clonal cell line (tsA201) reveal MiRP3 to modulate Kv4.2 current activation, inactivation and recovery from inactivation. MiRP3 shifts the half-maximal voltage for activation (V(1/2)) approximately 20 mV and slows time to peak approximately 100%. In addition, MiRP3 slows inactivation approximately 100%, speeds recovery from inactivation approximately 30%, and enhances restored currents so they 'overshoot' baseline levels. The cytoplasmic accessory subunit KChIP2 also assembles with Kv4.2 in tsA201 cells to increase peak current, shift V(1/2) approximately 5 mV, slow time to peak approximately 10%, slow inactivation approximately 100%, and speed recovery from inactivation approximately 250% without overshoot. Simultaneous expression of all three subunits yields a biophysical profile unlike either accessory subunit alone, abolishes MiRP3-induced overshoot, and allows biochemical isolation of the ternary complex. Thus, regional heterogeneity in cardiac expression of MiRP3, Kv4.2 and KChIP2 in health and disease may establish the local attributes and magnitude of cardiac I(to)

    Search for a new heavy scalar particle decaying into a Higgs boson and a new scalar singlet in final states with one or two light leptons and a pair of τ\tau-leptons with the ATLAS detector

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    A search for a new heavy scalar particle XX decaying into a Standard Model (SM) Higgs boson and a new singlet scalar particle SS is presented. The search uses a proton-proton (pppp) collision data sample with an integrated luminosity of 140 fb1^{-1} recorded at a centre-of-mass energy of s=13\sqrt{s} = 13 TeV with the ATLAS detector at the Large Hadron Collider. The most sensitive mass parameter space is explored in XX mass ranging from 500 to 1500 GeV, with the corresponding SS mass in the range 200-500 GeV. The search selects events with two hadronically decaying τ\tau-lepton candidates from Hτ+τH\to \tau^+\tau^- decays and one or two light leptons (=e,μ\ell=e,\,\mu) from SVVS\to VV (V=W,ZV = W,\,Z) decays while the remaining VV boson decays hadronically or to neutrinos. A multivariate discriminant based on event kinematics is used to separate the signal from the background. No excess is observed beyond the expected SM background and 95% confidence level upper limits between 72 fb and 542 fb are derived on the cross-section σ(ppXSH)\sigma(pp\to X\to SH) assuming the same SM-Higgs boson-like decay branching ratios for the SVVS\to VV decay. Upper limits on the visible cross-sections σ(ppXSHWWττ)\sigma(pp\to X\to SH \to WW\tau\tau) and σ(ppXSHZZττ)\sigma(pp\to X\to SH \to ZZ\tau\tau) are also set in the ranges 3-26 fb and 6-33 fb, respectively.Comment: 46 pages in total, author list starting page 28, 5 figures, 5 tables, published in JHEP. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HDBS-2022-4

    Probing Charm Quark Dynamics via Multiparticle Correlations in Pb-Pb Collisions at √sNN=5.02 TeV

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    Multiparticle azimuthal correlations of prompt D-0 mesons arc measured in Pb-Pb collisions at a nucleon-nucleon center-of-mass energy of root s(NN) = 5.02 TeV. For the first time, a four-particle cumulant method is used to extract the second Fourier coefficient of the azimuthal distribution (v(2)) of D-0 mesons as a function of event centrality and the D-0 transverse momentum. The ratios of the four-particle v(2) values to previously measured two-particle cumulant results provide direct experimental access to event-by-event fluctuations of charm quark azimuthal anisotropies. These ratios are also found to be comparable to those of inclusive charged particles in the event. However, hints of deviations are seen in the most central and peripheral collisions. To investigate the origin of flow fluctuations in the charm sector, these measurements are compared to a model implementing fluctuations of charm quark energy loss via collisional or radiative processes in the quark-gluon plasma. These models cannot quantitatively describe the data over the full transverse momentum and centrality ranges, although the calculations with collisional energy loss provide a better description of the data

    Search for Higgs Boson Pair Production in the Four b Quark Final State in Proton-Proton Collisions at √s=13 TeV

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    A search for pairs of Higgs bosons produced via gluon and vector boson fusion is presented, focusing on the four b quark final state. The data sample consists of proton-proton collisions at a center-of-mass energy of 13 TeV, collected with the CMS detector at the LHC, and corresponds to an integrated luminosity of 138 fb^{-1}. No deviation from the background-only hypothesis is observed. A 95% confidence level upper limit on the Higgs boson pair production cross section is observed at 3.9 times the standard model prediction for an expected value of 7.8. Constraints are also set on the modifiers of the Higgs field self-coupling, κ_{λ}, and of the coupling of two Higgs bosons to two vector bosons, κ_{2 V}. The observed (expected) allowed intervals at the 95% confidence level are -2.3<9.4 (-5.0<12.0) and -0.1<2.2 (-0.4<2.5). These are the most stringent observed constraints to date on the HH production cross section and on the κ_{2 V } coupling

    Sex differences in incidence, mortality, and survival in individuals with stroke in Scotland, 1986 to 2005

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    <p><b>Background and Purpose:</b> The aim of this study was to examine the effect of sex across different age groups and over time for stroke incidence, 30-day case-fatality, and mortality.</p> <p><b>Methods:</b> All first hospitalizations for stroke in Scotland (1986 to 2005) were identified using linked morbidity and mortality data. Age-specific rate ratios (RRs) for comparing women with men for both incidence and mortality were modeled with adjustment for study year and socioeconomic deprivation. Logistic regression was used to model 30-day case-fatality.</p> <p><b>Results:</b> Women had a lower incidence of first hospitalization than men and size of effect varied with age (55 to 64 years, RR=0.65, 95% CI 0.63 to 0.66; 85 years, RR=0.94, 95% CI 0.91 to 0.96). Women aged 55 to 84 years had lower mortality than men and again size of effect varied with age (65 to 74 years, RR=0.79, 95% CI 0.76 to 0.81); 75 to 84 years, RR=0.94, 95% CI 0.92 to 0.95). Conversely, women aged 85 years had 15% higher stroke mortality than men (RR=1.15, 95% CI 1.12 to 1.18). Adjusted risk of death within 30 days was significantly higher in women than men, and this difference increased over the 20-year period in all age groups (adjusted OR in 55 to 64 year olds 1.23, 95% CI 1.14 to 1.33 in 1986 and 1.51, 95% CI 1.39 to 1.63 in 2005).</p> <p><b>Conclusions:</b> We observed lower rates of incidence and mortality in younger women than men. However, higher numbers of older women in the population mean that the absolute burden of stroke is greater in women. Short-term case-fatality is greater in women of all ages and, worryingly, these differences have increased from 1986 to 2005.</p&gt

    Measurement of the Bs0μμB_s^0 \to \mu\mu Effective Lifetime with the ATLAS Detector

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    This paper reports the first ATLAS measurement of the Bs0μμB_s^0 \to \mu\mu effective lifetime. The measurement is based on the data collected in 2015-2016, amounting to 26.3 fb1^{-1} of 13 TeV LHC proton-proton collisions. The proper decay-time distribution of 58±1358\pm13 background-subtracted signal candidates is fit with simulated signal templates parameterised as a function of the Bs0B_s^0 effective lifetime, with statistical uncertainties extracted through a Neyman construction. The resulting effective measurement of the Bs0μμB_s^0 \to \mu\mu lifetime is 0.990.07+0.42(stat.)±0.17 (syst.)ps0.99^{+0.42}_{-0.07} \, (\text{stat.})\pm 0.17 \text{ (syst.)}\,\mathrm{ps} and it is found to be consistent with the Standard Model.Comment: 32 pages in total, author list starting page 14, 4 figures and 1 table. All figures/tables (including auxiliary ones), are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/BPHY-2020-07

    Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at s=13TeV\sqrt{s} = 13\,\text {Te}\text {V}

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    International audienceA combination of searches for top squark pair production using proton–proton collision data at a center-of-mass energy of 13TeV\,\text {Te}\text {V} at the CERN LHC, corresponding to an integrated luminosity of 137fb1\,\text {fb}^{-1} collected by the CMS experiment, is presented. Signatures with at least 2 jets and large missing transverse momentum are categorized into events with 0, 1, or 2 leptons. New results for regions of parameter space where the kinematical properties of top squark pair production and top quark pair production are very similar are presented. Depending on the model, the combined result excludes a top squark mass up to 1325GeV\,\text {Ge}\text {V} for a massless neutralino, and a neutralino mass up to 700GeV\,\text {Ge}\text {V} for a top squark mass of 1150GeV\,\text {Ge}\text {V}. Top squarks with masses from 145 to 295GeV\,\text {Ge}\text {V}, for neutralino masses from 0 to 100GeV\,\text {Ge}\text {V}, with a mass difference between the top squark and the neutralino in a window of 30GeV\,\text {Ge}\text {V} around the mass of the top quark, are excluded for the first time with CMS data. The results of theses searches are also interpreted in an alternative signal model of dark matter production via a spin-0 mediator in association with a top quark pair. Upper limits are set on the cross section for mediator particle masses of up to 420GeV\,\text {Ge}\text {V}

    Measurement of the cross-sections of the electroweak and total production of a ZγZ \gamma pair in association with two jets in pppp collisions at s\sqrt{s} = 13 TeV with the ATLAS detector

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    This Letter presents the measurement of the fiducial and differential cross-sections of the electroweak production of a ZγZ \gamma pair in association with two jets. The analysis uses 140 fb1^{-1} of LHC proton-proton collision data taken at s\sqrt{s}=13 TeV recorded by the ATLAS detector during the years 2015-2018. Events with a ZZ boson candidate decaying into either an e+ee^+e^- or μ+μ\mu^+ \mu^- pair, a photon and two jets are selected. The electroweak component is extracted by requiring a large dijet invariant mass and a large rapidity gap between the two jets and is measured with an observed and expected significance well above five standard deviations. The fiducial ppZγjjpp \rightarrow Z \gamma jj cross-section for the electroweak production is measured to be 3.6 ±\pm 0.5 fb. The total fiducial cross-section that also includes contributions where the jets arise from strong interactions is measured to be 16.81.8+2.016.8^{+2.0}_{-1.8} fb. The results are consistent with the Standard Model predictions. Differential cross-sections are also measured using the same events and are compared with parton-shower Monte Carlo simulations. Good agreement is observed between data and predictions.Comment: 44 pages in total, author list starting page 27, 6 figures, 3 tables, submitted to PLB. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/STDM-2018-36

    Search for flavor-changing neutral tqHtqH interactions with HγγH\rightarrow \gamma\gamma in pppp collisions at s\sqrt{s} = 13 TeV using the ATLAS detector

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    A search for flavour-changing neutral interactions involving the top quark, the Higgs boson and an up-type quark qq (q=c,uq = c, u) is presented. The proton-proton collision data set used, with an integrated luminosity of 139 fb1^{-1}, was collected at s=13\sqrt{s} = 13\~TeV by the ATLAS experiment at the Large Hadron Collider. Both the decay process tqHt \to qH and the production process pptHpp \to tH, with the Higgs boson decaying into two photons, are investigated. No significant excess is observed and upper limits are set on the tcHt\rightarrow cH and the tuHt\rightarrow uH branching ratios of 4.3×1044.3\times 10^{-4} and 3.8×1043.8\times 10^{-4}, respectively, at the 95% confidence level, while the expected limits in the absence of signal are 4.7×1044.7\times 10^{-4} and 3.9×1043.9\times 10^{-4}. Combining this search with ATLAS searches in the Hτ+τH \to \tau^+\tau^- and HbbˉH \to b\bar{b} final states yields observed (expected) upper limits on the tcHt\to cH branching ratio of 5.8×104 (3.0×104)5.8\times 10^{-4}\ (3.0\times 10^{-4}) at the 95% confidence level. The corresponding observed (expected) upper limit on the tuHt\rightarrow uH branching ratio is $4.0 \times 10^{-4}\ (2.4 \times 10^{-4})$Comment: 51 pages in total, author list starting page 34, 11 figures, 6 tables, published by JHEP. All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2019-0
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