La sécrétion de la protéine tau : mécanisme de propagation de la pathologie de tau dans la maladie d’Alzheimer

Dans la maladie d’Alzheimer, il existe deux marqueurs histopathologiques : les plaques amyloïdes composées de la protéine amyloïde-bêta et les enchevêtrements neurofibrillaires (NFTs) composés de la protéine tau agrégée. Dans le cerveau, la propagation de la pathologie de tau est observée le long des circuits neuronaux connectés synaptiquement, selon une séquence de stades, caractérisés par le Docteur Braak en 1991. Chez les patients, le degré de démence corrèle avec le nombre de NFTs. Ces derniers apparaissent dans des régions précises du cerveau et se propagent, de manière prédictible, le long des projections neuronales à des stades plus tardifs de la pathologie. Il reste à éclaircir la manière dont les NFTs se propagent dans les différentes régions du cerveau. Dans notre laboratoire, nous avons émis l’hypothèse que la propagation de tau pourrait se produire par un processus de transmission de cellule à cellule. Ainsi, la protéine tau serait tout d’abord sécrétée par un neurone, puis endocytée par un neurone adjacent. Nos travaux de recherche se sont concentrés sur la sécrétion de la protéine tau. Dans une première étape, nous avons démontré l’existence de la sécrétion active de tau dans l’espace extracellulaire, en utilisant des modèles in vitro de cellules non neuronales et neuronales. Par la suite, nous avons caractérisé les formes de protéines tau sécrétées. Enfin dans un dernier temps, nous avons exploré les voies de sécrétion de la protéine tau ainsi que les mécanismes régulant ce phénomène. Nous avons réussi à moduler la sécrétion de tau en reproduisant plusieurs insultes observées dans la maladie d’Alzheimer. Nos recherches nous ont permis d’identifier l’appareil de Golgi comme étant une organelle dont la fragmentation augmente la sécrétion de la protéine tau. A la lumière de cette découverte, nous avons été capable de moduler la sécrétion de tau en ciblant spécifiquement l’activité de cdk5 et l’expression de rab1A contrôlant la morphologie du Golgi. Ainsi, nous avons réussi à diminuer significativement la sécrétion de la protéine tau. Nos travaux de recherche proposent de nouvelles cibles thérapeutiques pour la maladie d’Alzheimer, visant à diminuer la propagation de la pathologie de tau par de nouveaux mécanismes cellulaires.In Alzheimer’s disease, the amyloid plaques and the neurofibrillary tangles composed of misfolded aggregated tau protein are the two hallmarks of the pathology. In the brain, the propagation of tau pathology was observed along the neuronal circuits. Described by Doctor Braak in 1991, the appearence of the neurofibrillary tangles was predictable in the brain and correlated with the degree of cognitive deficits. Its remains unclear how tau pathology spreads in the brain. In our laboratory, we made the hypothesis that the propagation could occur by cell-to-cell transmission. This implies that NFTs would propagate in the brain by the release of misfolded tau aggregates from an affected neuron followed by its uptake in neighboring neurons. My thesis focuses on the mechanism of tau secretion. Firstly, we demonstrated that tau was actively secreted in the extracellular space by non neuronal cells and primary neurons. Then, we characterized the tau secreted forms. Finally, we explored the secretory pathways and the mechanisms leading to tau secretion. We were able to modulate tau secretion by mimicking specific insults observed in Alzheimer disease. Our research led us to identify the Golgi apparatus as a major contributor to tau secretion. Concomitant with this, modulation of cdk5 pathway and rab1A expression, which are known to affect the Golgi morphology, altered significantly tau secretion. Our research provides new therapeutic strategies for Alzheimer’s disease, targeting tau secretion to reduce the propagation of tau pathology by new cellular mecanisms

G3BP1 promotes stress-induced RNA granule interactions to preserve polyadenylated mRNA

G3BP1, a target of TDP-43, is required for normal stress granule (SG) assembly, but the functional consequences of failed SG assembly remain unknown. Here, using both transformed cell lines and primary neurons, we investigated the functional impact of this disruption in SG dynamics. While stress-induced translational repression and recruitment of key SG proteins was undisturbed, depletion of G3BP1 or its upstream regulator TDP-43 disturbed normal interactions between SGs and processing bodies (PBs). This was concomitant with decreased SG size, reduced SG–PB docking, and impaired preservation of polyadenylated mRNA. Reintroduction of G3BP1 alone was sufficient to rescue all of these phenotypes, indicating that G3BP1 is essential for normal SG–PB interactions and SG function

Hyperphosphorylation and Cleavage at D421 Enhance Tau Secretion

It is well established that tau pathology propagates in a predictable manner in Alzheimer’s disease (AD). Moreover, tau accumulates in the cerebrospinal fluid (CSF) of AD’s patients. The mechanisms underlying the propagation of tau pathology and its accumulation in the CSF remain to be elucidated. Recent studies have reported that human tau was secreted by neurons and non-neuronal cells when it was overexpressed indicating that tau secretion could contribute to the spreading of tau pathology in the brain and could lead to its accumulation in the CSF. In the present study, we showed that the overexpression of human tau resulted in its secretion by Hela cells. The main form of tau secreted by these cells was cleaved at the C-terminal. Surprisingly, secreted tau was dephosphorylated at several sites in comparison to intracellular tau which presented a strong immunoreactivity to all phospho-dependent antibodies tested. Our data also revealed that phosphorylation and cleavage of tau favored its secretion by Hela cells. Indeed, the mimicking of phosphorylation at 12 sites known to be phosphorylated in AD enhanced tau secretion. A mutant form of tau truncated at D421, the preferential cleavage site of caspase-3, was also significantly more secreted than wild-type tau. Taken together, our results indicate that hyperphosphorylation and cleavage of tau by favoring its secretion could contribute to the propagation of tau pathology in the brain and its accumulation in the CSF

Design and baseline characteristics of the finerenone in reducing cardiovascular mortality and morbidity in diabetic kidney disease trial

Background: Among people with diabetes, those with kidney disease have exceptionally high rates of cardiovascular (CV) morbidity and mortality and progression of their underlying kidney disease. Finerenone is a novel, nonsteroidal, selective mineralocorticoid receptor antagonist that has shown to reduce albuminuria in type 2 diabetes (T2D) patients with chronic kidney disease (CKD) while revealing only a low risk of hyperkalemia. However, the effect of finerenone on CV and renal outcomes has not yet been investigated in long-term trials. Patients and Methods: The Finerenone in Reducing CV Mortality and Morbidity in Diabetic Kidney Disease (FIGARO-DKD) trial aims to assess the efficacy and safety of finerenone compared to placebo at reducing clinically important CV and renal outcomes in T2D patients with CKD. FIGARO-DKD is a randomized, double-blind, placebo-controlled, parallel-group, event-driven trial running in 47 countries with an expected duration of approximately 6 years. FIGARO-DKD randomized 7,437 patients with an estimated glomerular filtration rate >= 25 mL/min/1.73 m(2) and albuminuria (urinary albumin-to-creatinine ratio >= 30 to <= 5,000 mg/g). The study has at least 90% power to detect a 20% reduction in the risk of the primary outcome (overall two-sided significance level alpha = 0.05), the composite of time to first occurrence of CV death, nonfatal myocardial infarction, nonfatal stroke, or hospitalization for heart failure. Conclusions: FIGARO-DKD will determine whether an optimally treated cohort of T2D patients with CKD at high risk of CV and renal events will experience cardiorenal benefits with the addition of finerenone to their treatment regimen. Trial Registration: EudraCT number: 2015-000950-39; ClinicalTrials.gov identifier: NCT02545049

Operation and performance of the ATLAS Tile Calorimeter in Run 1

The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report

Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector

A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions

Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector

A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV

The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1

Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector

A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1  fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex