164 research outputs found

    Diagnosis and rational treatment of painful diabetic peripheral neuropathy: an interdisciplinary expert consensus

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    Diabetic peripheral neuropathy is a common chronic complication of diabetes mellitus, significantly impairing well-being, quality of life and functioning of patients. The prevalence of diabetic peripheral neuropathy in the Russian Federation ranges from 0.1% to 67.2% in type 1 and from 0.1 to 42.4% in type 2 diabetes mellitus. However, based on the large-scale epidemiological studies, the true prevalence of diabetic peripheral neuropathy is much higher (50 to 70%), with its painful variant occurring in 16% to 30% of patients. Despite the fact that diabetic peripheral neuropathy remains the most common chronic complication of diabetes mellitus, its diagnosis and therapy leave much to be desired. To optimize diagnostic and treatment approaches to painful diabetic peripheral neuropathy, a group of experts representing the leading Russian professional medical associations has developed clinical guidelines for the diagnosis and rational therapy of patients with painful diabetic peripheral neuropathy. This document presents practical aspects of the clinical diagnosis of painful diabetic peripheral neuropathy and an algorithm for differential diagnosis of pain in the lower extremities in patients with diabetes mellitus. The use of symptomatic analgesics with central action, such as anticonvulsants, antidepressants and opioids, is based on the main aspects of neuropathic pain pathophysiology. The characteristics of each drug class are given, with consideration of evidence on their efficacy, tolerability, and the possibility of combination therapy. The data on the first, second, and third lines of agents is presented in accordance with several international clinical guidelines. The need for a tailored drug choice, taking into account the evidence-based data on their efficacy and safety, concomitant drug therapy, tolerability, cost and preferences of the patient, age of the patient and concomitant disorders, is emphasized

    LHCb upgrade software and computing : technical design report

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    This document reports the Research and Development activities that are carried out in the software and computing domains in view of the upgrade of the LHCb experiment. The implementation of a full software trigger implies major changes in the core software framework, in the event data model, and in the reconstruction algorithms. The increase of the data volumes for both real and simulated datasets requires a corresponding scaling of the distributed computing infrastructure. An implementation plan in both domains is presented, together with a risk assessment analysis

    Physics case for an LHCb Upgrade II - Opportunities in flavour physics, and beyond, in the HL-LHC era

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    The LHCb Upgrade II will fully exploit the flavour-physics opportunities of the HL-LHC, and study additional physics topics that take advantage of the forward acceptance of the LHCb spectrometer. The LHCb Upgrade I will begin operation in 2020. Consolidation will occur, and modest enhancements of the Upgrade I detector will be installed, in Long Shutdown 3 of the LHC (2025) and these are discussed here. The main Upgrade II detector will be installed in long shutdown 4 of the LHC (2030) and will build on the strengths of the current LHCb experiment and the Upgrade I. It will operate at a luminosity up to 2×1034 cm−2s−1, ten times that of the Upgrade I detector. New detector components will improve the intrinsic performance of the experiment in certain key areas. An Expression Of Interest proposing Upgrade II was submitted in February 2017. The physics case for the Upgrade II is presented here in more depth. CP-violating phases will be measured with precisions unattainable at any other envisaged facility. The experiment will probe b → sl+l−and b → dl+l− transitions in both muon and electron decays in modes not accessible at Upgrade I. Minimal flavour violation will be tested with a precision measurement of the ratio of B(B0 → ÎŒ+Ό−)/B(Bs → ÎŒ+Ό−). Probing charm CP violation at the 10−5 level may result in its long sought discovery. Major advances in hadron spectroscopy will be possible, which will be powerful probes of low energy QCD. Upgrade II potentially will have the highest sensitivity of all the LHC experiments on the Higgs to charm-quark couplings. Generically, the new physics mass scale probed, for fixed couplings, will almost double compared with the pre-HL-LHC era; this extended reach for flavour physics is similar to that which would be achieved by the HE-LHC proposal for the energy frontier

    Measurement of the branching fraction and CPCP asymmetry in B+→J/ψρ+B^{+}\rightarrow J/\psi \rho^{+} decays

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    International audienceThe branching fraction and direct C ⁣PC\!P asymmetry of the decay B+ ⁣→J/ψρ+{{{B} ^+}} \!\rightarrow {{J /\psi }} {{\rho } ^+} are measured using proton-proton collision data collected with the LHCb detector at centre-of-mass energies of 7 and 8 TeV, corresponding to a total integrated luminosity of 3   fb −1\,\text{ fb }^{-1} . The following results are obtained: B(B+ ⁣→J/ψρ+)=(3.81+0.25−0.24±0.35)×10−5,AC ⁣P(B+ ⁣→J/ψρ+)=−0.045+0.056−0.057±0.008,\begin{aligned} \mathcal {B}({{B} ^+} \!\rightarrow {{J /\psi }} {{\rho } ^+} )&= (3.81^{+0.25-0.24} \pm 0.35) \times 10^{-5},\\ \mathcal {A}^{{C\!P}} ({{B} ^+} \!\rightarrow {{J /\psi }} {{\rho } ^+} )&= -0.045^{+0.056-0.057} \pm 0.008, \end{aligned} where the first uncertainties are statistical and the second systematic. Both measurements are the most precise to date

    Amplitude analysis of the B(s)0→K∗0K‟∗0B^0_{(s)} \to K^{*0} \overline{K}^{*0} decays and measurement of the branching fraction of the B0→K∗0K‟∗0B^0 \to K^{*0} \overline{K}^{*0} decay

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    International audienceThe B0→K∗0K‟∗0 {B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} and Bs0→K∗0K‟∗0 {B}_s^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} decays are studied using proton-proton collision data corresponding to an integrated luminosity of 3 fb−1^{−1}. An untagged and timeintegrated amplitude analysis of B_{( s}_{)}^{0}  → (K+^{+}π−^{−})(K−^{−}π+^{+}) decays in two-body invariant mass regions of 150 MeV/c2^{2} around the K∗0^{∗0} mass is performed. A stronger longitudinal polarisation fraction in the B0→K∗0K‟∗0 {B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} decay, fL_{L} = 0.724 ± 0.051 (stat) ± 0.016 (syst), is observed as compared to fL_{L} = 0.240 ± 0.031 (stat) ± 0.025 (syst) in the Bs0→K∗0K‟∗0 {B}_s^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} decay. The ratio of branching fractions of the two decays is measured and used to determine B(B0→K∗0K‟∗0)=(8.0±0.9(stat)±0.4(syst))×10−7 \mathrm{\mathcal{B}}\left({B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0}\right)=\left(8.0\pm 0.9\left(\mathrm{stat}\right)\pm 0.4\left(\mathrm{syst}\right)\right)\times {10}^{-7}

    Measurement of CPCP-violating and mixing-induced observables in Bs0â†’Ï•ÎłB_s^0 \to \phi\gamma decays

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    International audienceA time-dependent analysis of the Bs0â†’Ï•Îł decay rate is performed to determine the CP -violating observables SÏ•Îł and CÏ•Îł and the mixing-induced observable AÏ•ÎłÎ”. The measurement is based on a sample of pp collision data recorded with the LHCb detector, corresponding to an integrated luminosity of 3  fb-1 at center-of-mass energies of 7 and 8 TeV. The measured values are SÏ•Îł=0.43±0.30±0.11, CÏ•Îł=0.11±0.29±0.11, and AÏ•ÎłÎ”=-0.67-0.41+0.37±0.17, where the first uncertainty is statistical and the second systematic. This is the first measurement of the observables S and C in radiative Bs0 decays. The results are consistent with the standard model predictions

    Measurement of the charm-mixing parameter yCP

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