1,693 research outputs found

    Reaching silicon-based NEMS performances with 3D printed nanomechanical resonators

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    The extreme miniaturization in NEMS resonators offers the possibility to reach an unprecedented resolution in high-performance mass sensing. These very low limits of detection are related to the combination of two factors: a small resonator mass and a high quality factor. The main drawback of NEMS is represented by the highly complex, multi-steps, and expensive fabrication processes. Several alternatives fabrication processes have been exploited, but they are still limited to MEMS range and very low-quality factor. Here we report the fabrication of rigid NEMS resonators with high-quality factors by a 3D printing approach. After a thermal step, we reach complex geometry printed devices composed of ceramic structures with high Young’s modulus and low damping showing performances in line with silicon-based NEMS resonators ones. We demonstrate the possibility of rapid fabrication of NEMS devices that present an effective alternative to semiconducting resonators as highly sensitive mass and force sensors

    Search for a Standard Model Higgs boson produced in association with a W or Z boson decaying to bottom quarks

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    A search for a Standard Model Higgs boson decaying to bbˉ\bar{\text{b}} produced in association with a W or Z boson is reported for the following channels W(eν\nu)H, W(μν\mu\nu)H, W(τν\tau\nu)H, Z(μμ)\mu\mu)H, Z(ee)H, and Z(νν\nu\nu)H. The search is performed on data samples corresponding to integrated luminosities of 5.1 fb1\text{fb}^{-1} at s=7\sqrt{s} = 7 TeV and 18.9 fb1\text{fb}^{-1} at s=8\sqrt{s} = 8 TeV, collected by the CMS experiement at the LHC. An excess of events is observed above the expected background with a local significance of 2.1 standard deviations for a Higgs boson with mass 125 GeV consistent with Standard Model expectations. The signal strength corresponding to this excess, relative to that of the Standard Model Higgs boson, was 0.89 ±\pm 0.43

    Symplectic subspaces of symplectic Grassmannians

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    AbstractLet V be a non-degenerate symplectic space of dimension 2n over the field F and for a natural number l<n denote by Cl(V) the incidence geometry whose points are the totally isotropic l-dimensional subspaces of V. Two points U,W of Cl(V) will be collinear when W⊂U⊥ and dim(U∩W)=l−1 and then the line on U and W will consist of all the l-dimensional subspaces of U+W which contain U∩W. The isomorphism type of this geometry is denoted by Cn,l(F). When char(F)≠2 we classify subspaces S of Cl(F) where S≅Cm,k(F)

    Observation of Higgs boson decay to bottom quarks

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    The observation of the Standard Model Higgs boson decay to a bottom quark-antiquark pair is presented. The primary contribution to this result is from processes in which the Higgs boson is produced in association with a W or Z boson. The latest measurement of these processes is described, using 41.3/fb of proton-proton collision data at center-of-mass energy √s = 13 TeV, collected by the CMS experiment in 2017. The significance of the observed excess in data over Standard Model backgrounds is 3.3 standard deviations. The result is combined with similar measurements performed by CMS on previous datasets, resulting in an observed significance of 5.6 standard deviations. The measured signal is well consistent with the Standard Model expectation for a Higgs boson with mass 125 GeV decaying to bottom quarks, with a precision of 20%

    Observation of Higgs boson decay to bottom quarks

    No full text
    The observation of the Standard Model Higgs boson decay to a bottom quark-antiquark pair is presented. The primary contribution to this result is from processes in which the Higgs boson is produced in association with a W or Z boson. The latest measurement of these processes is described, using 41.3/fb of proton-proton collision data at center-of-mass energy √s = 13 TeV, collected by the CMS experiment in 2017. The significance of the observed excess in data over Standard Model backgrounds is 3.3 standard deviations. The result is combined with similar measurements performed by CMS on previous datasets, resulting in an observed significance of 5.6 standard deviations. The measured signal is well consistent with the Standard Model expectation for a Higgs boson with mass 125 GeV decaying to bottom quarks, with a precision of 20%

    Observation of Higgs boson decay to bottom quarks

    No full text
    The observation of the Standard Model Higgs boson decay to a bottom quark-antiquark pair is presented. The primary contribution to this result is from processes in which the Higgs boson is produced in association with a W or Z boson. The latest measurement of these processes is described, using 41.3 fb1^{−1} of proton-proton collision data at center-of-mass energy s\sqrt{s}= 13 TeV, collected by the CMS experiment in 2017. The significance of the observed excess in data over Standard Model backgrounds is 3.3 standard deviations. The result is combined with similar measurements performed by CMS on previous datasets, resulting in an observed significance of 5.6 standard deviations. The measured signal is well consistent with the Standard Model expectation for a Higgs boson with mH_{H} = 125 GeV decaying to bottom quarks, with a precision of 20%

    Can Nuclear Power Be Part of the Solution?

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    The author discusses the importance of incorporating the full costs of operating a nuclear power plant in the U.S., such as climate impact, risk of accidents, and safe disposal of radioactive waste. He argues on the need for changes in the country\u27s evaluation of nuclear power which include the elimination of subsidies, and the requirement to buy full-coverage insurance for accidents. The author further highlights the cost of greenhouse gas emissions from nuclear power plants
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