Diagnóstico molecular de hipercolesterolemia familiar: uma ferramenta importante para a estratificação do risco cardiovascular

Familial hypercholesterolemia (FH) is associated with an increased risk of premature coronary heart disease. Molecular identification of these patients can reduce the burden of mortality from cardiovascular disorders simply by the correct identification of the disease early in life, followed by counseling and appropriate lifestyle modifications, and therapeutic measures when required. Recent studies show that, in Portugal, this disease is severely under-diagnosed. After more than 10 years of research through the Portuguese FH Study, it is now possible to translate the original research results into clinical application. AIMS: The main aims of the present work were to determine whether clinical characterization is sufficient to identify these individuals at high risk of developing CHD and to evaluate the clinical applicability of molecular diagnosis for FH. METHODS: All patients described in this study were recruited for the Portuguese FH Study. The diagnostic criteria used to select the index patients were adapted from the Simon Broome Heart Research Trust. To analyze the usefulness of the molecular diagnosis, graphs of total and LDL cholesterol values by age were constructed for 622 possible FH patients. The lipid profile of patients genetically identified as having FH, before and under medication, were analyzed to assess whether these patients were receiving appropriate treatment. The data are shown separately for children and adults and for female and male propositi (index cases and hypercholesterolemic relatives), both with and without a detectable mutation in the LDLR gene. RESULTS: The Portuguese FH Study has already genetically identified 404 individuals (171 index patients and 233 relatives) among more than one thousand individuals sent for study. A total of 78 different mutations in the LDLR gene were found in 171 index patients, 2 different mutations were found in the apoB gene of 4 patients and 2 patients had a unique PCSK9 mutation. Statistical analysis revealed that there are significant differences between total cholesterol (p < 0.001) and apoB (p = 0.026) values in the group of children (male and female) with and without a mutation in LDLR. For female children LDL values were also significantly different (p < 0.001) between subgroups but for male children this difference did not reach statistical significance. In adult women there is a statistically significant difference for total cholesterol (p = 0.049), LDL cholesterol (p = 0.031) and apoB (p = 0.003) values in the subgroups with and without a LDLR mutation. In adult males there is a statistical difference for total cholesterol (p = 0.002). LDL cholesterol (p = 0.003) and apoB (p = 0.0023) in subgroups with and without an LDLR mutation. Nevertheless there was considerable dispersion of values and individually it is not possible to distinguish between patients with and without a mutation in the LDLR gene, based only on lipid profile. CONCLUSIONS: By analysis of the clinical data of 696 possible FH patients, the present report shows evidence that clinical characterization is not sufficient to distinguish between patients with genetic or environmental dyslipidemia, and so molecular diagnosis is useful in clinical practice, allowing correct identification of FH patients and their relatives, and the early implementation of therapeutic measures to reduce the elevated cardiovascular risk of these patients. In general, molecular diagnosis of FH is feasible and could be obtained in 1-2 months if the technology is available. In Portugal the test will be offered to the population by our Institute at a cost of about 500 euros, like many other genetic tests or exams such as nuclear magnetic resonance

Caracterização bioquímica e molecular de doentes com diagnóstico clínico de Dislipidemia Familiar Combinada

A Dislipidemia Familiar Combinada (FCHL) é uma doença poligénica caracterizada por hiperlipidemia simples ou combinada, variabilidade intra-individual e intra-familiar do perfil lipídico, ApoB elevada (> 120 mg/dL) e risco elevado de doença cardiovascular (DCV). A sua causa é desconhecida mas alterações nos genes LPL, APOAIV, APOAV, APOCIII e USF1 parecem contribuir para o seu fenótipo. O objectivo deste estudo é caracterizar bioquímica e molecularmente doentes com diagnóstico clínico de FCHL. Todos os exões e promotor dos genes LPL, APOAIV, APOAV, APOCIII e regiões do gene USF1 (s1,s2) de 41 doentes foram amplificados por PCR e sequenciados. O colesterol total (CT), c-LDL, c-HDL, sdLDL, trigliceridos (TG), apoB e apoCIII foram determinados num aparelho automatizado. Em alguns doentes as sdLDL foram também analisadas por electroforese de lipoproteínas. A ApoAIV e ApoAV foram quantificadas por ELISA. Foram encontradas alterações genéticas em 37 doentes, 3 não descritas (APOAIV Q359_E362, APOAV D332fsX336 e APOCIII 3269C>A). O índex com a alteração Q359_E362del apresentou valores normais de apo AIV (15.5 mg/dL) e o índex com a alteração D332fsX336 apresentou valores baixos de apo AV (74.5 ng/mL). Os doentes estudados apresentam valores elevados de CT (285 ± 83 mg/dL), c-LDL (189 ± 85 mg/dL), TG (310 ± 253 mg/dL), e apo CIII (15 ± 4 mg/dL) e valores reduzidos de c-HDL (45 ± 11 mg/dL), sem medicação. Os valores de apoAIV (17,5 ± 10,4 mg/dL) e apoAV (150 ± 135 ng/mL) encontram-se, na maioria dos casos, no intervalo normal assim como os valores de sdLDL (35 ± 18 mg/dL), no entanto alguns casos apresentam valores acima do cut-off para DCV (35 mg/dL). A análise de sdLDL por electroforese foi realizada em 11 doentes, 9 dos quais apresentaram um perfil aterogénico. O valor médio de ApoB destes doentes era de 94 ± 43 mg/dL, mas aproximadamente 70% dos doentes estavam medicados com terapêutica hipolimiante (estatinas e/ou fibratos). Cerca de 30% dos doentes apresentavam DCV prematura. Os resultados obtidos parecem indicar que alterações nos genes estudados influenciam o fenótipo da FCHL. Os níveis séricos de apo CIII encontram-se alterados nesta dislipidemia. Doentes com FCHL, apesar de estarem medicados, apresentam valores elevados de sdLDL, evidenciando o seu elevado risco cardiovascular. A caracterização bioquímica complementa a identificação genética e permite uma melhor avaliação do risco cardiovascular do doente bem como a escolha de uma terapêutica adequada

The global burden of cancer attributable to risk factors, 2010–19: a systematic analysis for the Global Burden of Disease Study 2019

BACKGROUND: Understanding the magnitude of cancer burden attributable to potentially modifiable risk factors is crucial for development of effective prevention and mitigation strategies. We analysed results from the Global Burden of Diseases, Injuries, and Risk Factors Study (GBD) 2019 to inform cancer control planning efforts globally. METHODS: The GBD 2019 comparative risk assessment framework was used to estimate cancer burden attributable to behavioural, environmental and occupational, and metabolic risk factors. A total of 82 risk–outcome pairs were included on the basis of the World Cancer Research Fund criteria. Estimated cancer deaths and disability-adjusted life-years (DALYs) in 2019 and change in these measures between 2010 and 2019 are presented. FINDINGS: Globally, in 2019, the risk factors included in this analysis accounted for 4·45 million (95% uncertainty interval 4·01–4·94) deaths and 105 million (95·0–116) DALYs for both sexes combined, representing 44·4% (41·3–48·4) of all cancer deaths and 42·0% (39·1–45·6) of all DALYs. There were 2·88 million (2·60–3·18) risk-attributable cancer deaths in males (50·6% [47·8–54·1] of all male cancer deaths) and 1·58 million (1·36–1·84) risk-attributable cancer deaths in females (36·3% [32·5–41·3] of all female cancer deaths). The leading risk factors at the most detailed level globally for risk-attributable cancer deaths and DALYs in 2019 for both sexes combined were smoking, followed by alcohol use and high BMI. Risk-attributable cancer burden varied by world region and Socio-demographic Index (SDI), with smoking, unsafe sex, and alcohol use being the three leading risk factors for risk-attributable cancer DALYs in low SDI locations in 2019, whereas DALYs in high SDI locations mirrored the top three global risk factor rankings. From 2010 to 2019, global risk-attributable cancer deaths increased by 20·4% (12·6–28·4) and DALYs by 16·8% (8·8–25·0), with the greatest percentage increase in metabolic risks (34·7% [27·9–42·8] and 33·3% [25·8–42·0]). INTERPRETATION: The leading risk factors contributing to global cancer burden in 2019 were behavioural, whereas metabolic risk factors saw the largest increases between 2010 and 2019. Reducing exposure to these modifiable risk factors would decrease cancer mortality and DALY rates worldwide, and policies should be tailored appropriately to local cancer risk factor burden

Search for resonances decaying into photon pairs in 139 fb−1 of pp collisions at √s = 13 TeV with the ATLAS detector

Searches for new resonances in the diphoton final state, with spin 0 as predicted by theories with an extended Higgs sector and with spin 2 using a warped extra-dimension benchmark model, are presented using 139 fb−1 of √s = 13 TeV pp collision data collected by the ATLAS experiment at the LHC. No significant deviation from the Standard Model is observed and upper limits are placed on the production cross-section times branching ratio to two photons as a function of the resonance mass

Measurement of the top-quark mass using a leptonic invariant mass in pp collisions at s√ = 13 TeV with the ATLAS detector

A measurement of the top-quark mass (mt) in the tt¯ → lepton + jets channel is presented, with an experimental technique which exploits semileptonic decays of b-hadrons produced in the top-quark decay chain. The distribution of the invariant mass mℓμ of the lepton, ℓ (with ℓ = e, μ), from the W-boson decay and the muon, μ, originating from the b-hadron decay is reconstructed, and a binned-template profile likelihood fit is performed to extract mt. The measurement is based on data corresponding to an integrated luminosity of 36.1 fb−1 of s√ = 13 TeV pp collisions provided by the Large Hadron Collider and recorded by the ATLAS detector. The measured value of the top-quark mass is mt = 174.41 ± 0.39 (stat.) ± 0.66 (syst.) ± 0.25 (recoil) GeV, where the third uncertainty arises from changing the PYTHIA8 parton shower gluon-recoil scheme, used in top-quark decays, to a recently developed setup

Search for heavy resonances decaying into a Z or W boson and a Higgs boson in final states with leptons and b-jets in 139 fb−1 of pp collisions at s√ = 13 TeV with the ATLAS detector

This article presents a search for new resonances decaying into a Z or W boson and a 125 GeV Higgs boson h, and it targets the νν¯¯¯bb¯¯, ℓ+ℓ−bb¯¯, or ℓ±νbb¯¯ final states, where ℓ = e or μ, in proton-proton collisions at s√ = 13 TeV. The data used correspond to a total integrated luminosity of 139 fb−1 collected by the ATLAS detector during Run 2 of the LHC at CERN. The search is conducted by examining the reconstructed invariant or transverse mass distributions of Zh or Wh candidates for evidence of a localised excess in the mass range from 220 GeV to 5 TeV. No significant excess is observed and 95% confidence-level upper limits between 1.3 pb and 0.3 fb are placed on the production cross section times branching fraction of neutral and charged spin-1 resonances and CP-odd scalar bosons. These limits are converted into constraints on the parameter space of the Heavy Vector Triplet model and the two-Higgs-doublet model

The ATLAS trigger system for LHC Run 3 and trigger performance in 2022

The ATLAS trigger system is a crucial component of the ATLAS experiment at the LHC. It is responsible for selecting events in line with the ATLAS physics programme. This paper presents an overview of the changes to the trigger and data acquisition system during the second long shutdown of the LHC, and shows the performance of the trigger system and its components in the proton-proton collisions during the 2022 commissioning period as well as its expected performance in proton-proton and heavy-ion collisions for the remainder of the third LHC data-taking period (2022–2025)

Inclusive-photon production and its dependence on photon isolation in pp collisions at s√ = 13 TeV using 139 fb−1 of ATLAS data

Measurements of differential cross sections are presented for inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13 TeV provided by the LHC and using 139 fb−1 of data recorded by the ATLAS experiment. The cross sections are measured as functions of the photon transverse energy in different regions of photon pseudorapidity. The photons are required to be isolated by means of a fixed-cone method with two different cone radii. The dependence of the inclusive-photon production on the photon isolation is investigated by measuring the fiducial cross sections as functions of the isolation-cone radius and the ratios of the differential cross sections with different radii in different regions of photon pseudorapidity. The results presented in this paper constitute an improvement with respect to those published by ATLAS earlier: the measurements are provided for different isolation radii and with a more granular segmentation in photon pseudorapidity that can be exploited in improving the determination of the proton parton distribution functions. These improvements provide a more in-depth test of the theoretical predictions. Next-to-leading-order QCD predictions from JETPHOX and SHERPA and next-to-next-to-leading-order QCD predictions from NNLOJET are compared to the measurements, using several parameterisations of the proton parton distribution functions. The measured cross sections are well described by the fixed-order QCD predictions within the experimental and theoretical uncertainties in most of the investigated phase-space region

Measurements of Zγ+jets differential cross sections in pp collisions at s√ = 13 TeV with the ATLAS detector

Differential cross-section measurements of Zγ production in association with hadronic jets are presented, using the full 139 fb−1 dataset of s√ = 13 TeV proton–proton collisions collected by the ATLAS detector during Run 2 of the LHC. Distributions are measured using events in which the Z boson decays leptonically and the photon is usually radiated from an initial-state quark. Measurements are made in both one and two observables, including those sensitive to the hard scattering in the event and others which probe additional soft and collinear radiation. Different Standard Model predictions, from both parton-shower Monte Carlo simulation and fixed-order QCD calculations, are compared with the measurements. In general, good agreement is observed between data and predictions from MATRIX and MiNNLOPS, as well as next-to-leading-order predictions from MADGRAPH5_AMC@NLO and SHERPA

Search for light long-lived neutral particles that decay to collimated pairs of leptons or light hadrons in pp collisions at s√ = 13 TeV with the ATLAS detector

A search for light long-lived neutral particles with masses in the O(MeV–GeV) range is presented. The analysis targets the production of long-lived dark photons in the decay of a Higgs boson produced via gluon–gluon fusion or in association with a W boson. Events that contain displaced collimated Standard Model fermions reconstructed in the calorimeter or muon spectrometer are selected in 139 fb−1 of s√ = 13 TeV pp collision data collected by the ATLAS detector at the LHC. Background estimates for contributions from Standard Model processes and instrumental effects are extracted from data. The observed event yields are consistent with the expected background. Exclusion limits are reported on the production cross-section times branching fraction as a function of the mean proper decay length cτ of the dark photon, or as a function of the dark-photon mass and kinetic mixing parameter that quantifies the coupling between the Standard Model and potential hidden (dark) sectors. A Higgs boson branching fraction above 1% is excluded at 95% CL for a Higgs boson decaying into two dark photons for dark-photon mean proper decay lengths between 10 mm and 250 mm and dark photons with masses between 0.4 GeV and 2 GeV