10 research outputs found

    High-Performance NB-LDPC Decoder With Reduction of Message Exchange

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    © 2016 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future media, including reprinting/republishing this material for advertising or promotional purposes, creating new collective works, for resale or redistribution to servers or lists, or reuse of any copyrighted component of this work in other works.This paper presents a novel algorithm based on trellis min-max for decoding non-binary low-density parity-check (NB-LDPC) codes. This decoder reduces the number of messages exchanged between check node and variable node processors, which decreases the storage resources and the wiring congestion and, thus, increases the throughput of the decoder. Our frame error rate performance simulations show that the proposed algorithm has a negligible performance loss for high-rate codes with GF(16) and GF(32), and a performance loss smaller than 0.07 dB for high-rate codes over GF(64). In addition, a layered decoder architecture is presented and implemented on a 90-nm CMOS process for the following high-rate NB-LDPC codes: (2304, 2048) over GF(16), (837, 726) over GF(32), and (1536, 1344) over GF(64). In all cases, the achieved throughput is higher than 1 Gb/s.This work was supported in part by the Spanish Ministerio de Ciencia e Innovacion under Grant TEC2011-27916 and Grant TEC2012-38558-C02-02, and in part by Generalitat Valenciana under Grant GV/2014/011.Lacruz, JO.; García Herrero, FM.; Canet Subiela, MJ.; Valls Coquillat, J. (2016). High-Performance NB-LDPC Decoder With Reduction of Message Exchange. IEEE Transactions on Very Large Scale Integration (VLSI) Systems. 24(5):1950-1961. https://doi.org/10.1109/TVLSI.2015.2493041S1950196124

    Measurements of triple-differential cross sections for inclusive isolated-photon+jet events in pp\mathrm{p}\mathrm{p} collisions at s=8TeV\sqrt{s} = 8\,\text {TeV}

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    Positioning and Sensing for Vehicular Safety Applications in 5G and beyond

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    This article presents a shared vision among stakeholders across the value chain on the use of radio positioning and sensing for road safety in the 5G ecosystem. The key enabling technologies and architectural functionalities are explored, focusing on the extremely stringent localization and communication requirements. A case study for joint radar and communication using experimental data showcases the potential of the new enablers that are paving the way toward enhanced road safety in beyond 5G scenarios

    Measurements of triple-differential cross sections for inclusive isolated-photon+jet events in pp collisions at root s=8 TeV

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    Measurements are presented of the triple-differential cross section for inclusive isolated-photon+jet events in pp collisions at root s = 8 TeV as a function of photon transverse momentum (p(T)(gamma)), photon pseudorapidity (eta(gamma)), and jet pseudorapidity (eta(jet)). The data correspond to an integrated luminosity of 19.7 fb(-1) that probe a broad range of the available phase space, for vertical bar eta(gamma)vertical bar 25 GeV. The measurements are compared to next-to-leading order perturbative quantum chromodynamics calculations, which reproduce the data within uncertainties.Peer reviewe

    Opportunistic infections and AIDS malignancies early after initiating combination antiretroviral therapy in high-income countries

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    Background: There is little information on the incidence of AIDS-defining events which have been reported in the literature to be associated with immune reconstitution inflammatory syndrome (IRIS) after combined antiretroviral therapy (cART) initiation. These events include tuberculosis, mycobacterium avium complex (MAC), cytomegalovirus (CMV) retinitis, progressive multifocal leukoencephalopathy (PML), herpes simplex virus (HSV), Kaposi sarcoma, non-Hodgkin lymphoma (NHL), cryptococcosis and candidiasis. Methods: We identified individuals in the HIV-CAUSAL Collaboration, which includes data from six European countries and the US, who were HIV-positive between 1996 and 2013, antiretroviral therapy naive, aged at least 18 years, hadCD4+ cell count and HIV-RNA measurements and had been AIDS-free for at least 1 month between those measurements and the start of follow-up. For each AIDS-defining event, we estimated the hazard ratio for no cART versus less than 3 and at least 3 months since cART initiation, adjusting for time-varying CD4+ cell count and HIV-RNA via inverse probability weighting. Results: Out of 96 562 eligible individuals (78% men) with median (interquantile range) follow-up of 31 [13,65] months, 55 144 initiated cART. The number of cases varied between 898 for tuberculosis and 113 for PML. Compared with non-cART initiation, the hazard ratio (95% confidence intervals) up to 3 months after cART initiation were 1.21 (0.90-1.63) for tuberculosis, 2.61 (1.05-6.49) for MAC, 1.17 (0.34-4.08) for CMV retinitis, 1.18 (0.62-2.26) for PML, 1.21 (0.83-1.75) for HSV, 1.18 (0.87-1.58) for Kaposi sarcoma, 1.56 (0.82-2.95) for NHL, 1.11 (0.56-2.18) for cryptococcosis and 0.77 (0.40-1.49) for candidiasis. Conclusion: With the potential exception of mycobacterial infections, unmasking IRIS does not appear to be a common complication of cART initiation in high-income countries

    Measurements of triple-differential cross sections for inclusive isolated-photon + jet events in pp collisions at <tex>\sqrt{s}$</tex>=8 TeV

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    Measurements of triple-differential cross sections for inclusive isolated-photon+jet events in pp\mathrm{p}\mathrm{p} collisions at s=8TeV\sqrt{s} = 8\,\text {TeV}

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    Measurements are presented of the triple-differential cross section for inclusive isolated-photon+jet events in pp\mathrm{p}\mathrm{p} collisions at s=8\sqrt{s} = 8 TeV as a function of photon transverse momentum (p_{\mathrm {T}} ^{{\upgamma {}{}}}), photon pseudorapidity (\eta ^{{\upgamma {}{}}}), and jet pseudorapidity (ηjet\eta ^{\text {jet}}). The data correspond to an integrated luminosity of 19.7fb119.7{\,\text {fb}^{-1}} that probe a broad range of the available phase space, for |\eta ^{{\upgamma {}{}}} | 25\,\text {GeV}. The measurements are compared to next-to-leading order perturbative quantum chromodynamics calculations, which reproduce the data within uncertainties

    Measurements of triple-differential cross sections for inclusive isolated-photon+jet events in p p collisions at √s=8TeV

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    Measurements are presented of the triple-differential cross section for inclusive isolated-photon+jet events in p p collisions at s=8 TeV as a function of photon transverse momentum (pTγ), photon pseudorapidity (ηγ), and jet pseudorapidity (ηjet). The data correspond to an integrated luminosity of 19.7fb-1 that probe a broad range of the available phase space, for | ηγ| &amp;lt; 1.44 and 1.57 &amp;lt; | ηγ| &amp;lt; 2.50 , | ηjet| &amp;lt; 2.5 , 40&amp;lt;pTγ&amp;lt;1000GeV, and jet transverse momentum, pTjet, &amp;gt; 25GeV. The measurements are compared to next-to-leading order perturbative quantum chromodynamics calculations, which reproduce the data within uncertainties. © 2019, CERN for the benefit of the CMS collaboration

    Observation of a peaking structure in the J/psi phi mass spectrum from B-+/- -&gt; J/psi phi K-+/- decays

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    A peaking structure in the J/ψφ mass spectrum near threshold is observed in B ±→J/ψφK± decays, produced in pp collisions at √s=7 TeV collected with the CMS detector at the LHC. The data sample, selected on the basis of the dimuon decay mode of the J/ψ, corresponds to an integrated luminosity of 5.2 fb-1. Fitting the structure to an S-wave relativistic Breit-Wigner lineshape above a three-body phase-space nonresonant component gives a signal statistical significance exceeding five standard deviations. The fitted mass and width values are m = 4148.0 ± 2.4 (stat.) ± 6.3 (syst.)MeV and Γ=28-11 +15(stat.)±19(syst.)MeV, respectively. Evidence for an additional peaking structure at higher J/ψφ mass is also reported. © 2014 The Authors

    Measurements of the <tex>\Upsilon</tex>(1S),<tex>Υ</tex>(1S), <tex>\Upsilon</tex>(2S), and <tex>\Upsilon</tex>(3S)differentialcrosssectionsinppcollisionsat<tex>s</tex>(3S) differential cross sections in pp collisions at <tex>\sqrt{s}</tex>=7 TeV

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