Retaliation against whistleblowers is a well-recognized problem, yet there is little explanation for why uninvolved peers choose to retaliate through ostracism. We conduct two experiments in which ...participants take the role of a peer third-party observer of theft and subsequent whistleblowing. We manipulate injunctive norms (whether company policy is ambiguous or unambiguous regarding the action) and descriptive norms (whether others behave similarly). Both experiments (1) support the core of our theoretical model, based on social intuitionist theory (Haidt in Psychol Rev 108:814–834, 2001), such that moral judgments of the acts of wrongdoing and whistleblowing influence the perceived likeability of each actor and ultimately influence intention to ostracize each actor and (2) indicate more willingness to ostracize the whistleblower than the wrongdoer. When we vary norms for the wrongdoing in Experiment 1, we find that descriptive and injunctive norms indirectly influence intentions to ostracize both the wrongdoer and whistleblower. These relationships are serially mediated by the observers’ moral judgments of the act (wrongdoing or whistleblowing) and likeability of the actor (wrongdoer or whistleblower). When we vary norms for whistleblowing in Experiment 2, the injunctive norm manipulation affected moral judgment of the action of whistleblowing, and we do not observe any other significant effects of the norm manipulations on moral judgments of the actions of wrongdoing or whistleblowing.
Introduction : La production endogène de glucose est une fonction restreinte à trois tissus : le foie, le rein et l’intestin qui, seuls, expriment la glucose-6-phosphatase (G6Pase). Les souris ...transgéniques invalidées pour la sous-unité catalytique de la G6Pase spécifiquement dans le foie (B6.g6pcex3del .SA+/CreERT2 ) sont capables de réguler leur glycémie même au cours du jeûne grâce à leurs productions intestinale et rénale de glucose. Nous avons voulu déterminer le rôle de l’intestin dans cette régulation. Matériels et Méthodes : Des souris B6.g6pcex3lox .SA+/CreERT2 (pour l’invalidation hépatique) et des souris B6.g6pcex3lox .Vill+/CreERT2 (pour l’invalidation intestinale) ont été croisées pour obtenir des souris doublement invalidées (DKO) par une stratégie Cre-Lox ciblée et inductible. La glycémie des souris a été étudiée au cours du jeûne. Les activités des enzymes de la néoglucogenèse ont été déterminées sur des homogénats tissulaires. Résultats : La glycémie des souris DKO est fortement diminuée (61 ± 2,3 mg/dL) à 6 h de jeûne, comme celle des souris invalidées dans le foie (L-g6pc-/-), en raison de l’absence de glycogénolyse hépatique. Au contraire, les souris témoins maintiennent leur glycémie (169 ± 3,9 mg/dL). Au cours du jeûne prolongé, la glycémie des souris DKO reste basse (environ 60 mg/dL) alors que celle des souris L-g6pc-/- augmente dès 16 h de jeûne, pour atteindre environ 100 mg/dL à 48 h de jeûne. A l’euthanasie des souris, les activités G6Pase et phosphoénol pyruvate carboxykinase cytosolique rénales des souris DKO étaient augmentées par rapport à celles des souris témoins et comparables à celles des souris L-g6pc-/-. Conclusion : En l’absence de production hépatique et intestinale de glucose, les reins sont capables d’assurer le maintien d’une glycémie minimale, compatible avec la survie au cours du jeûne. Nos résultats suggèrent aussi que la néoglucogenèse intestinale, lorsqu’elle s’ajoute à la néoglucogenèse rénale, permet le maintien d’une glycémie physiologique dans cette situation.
A high-granularity timing detector for the ATLAS phase-II upgrade Casado, M.P.; Adam Bourdarios, C.; Belfkir, M. ...
Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment,
2022, Letnik:
1032
Journal Article
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The large increase of pileup interactions is one of the main experimental challenges for the HL-LHC physics programme. A powerful new way to mitigate the effects of pileup is to use high-precision ...timing information to distinguish between collisions occurring close in space but well-separated in time. A High-Granularity Timing Detector, based on low gain avalanche detector technology, is therefore proposed for the ATLAS Phase-II upgrade. Covering the pseudorapidity region between 2.4 and 4.0, this device will improve the detector physics performance in the forward region. The typical number of hits per track in the detector was optimized so that the target average time resolution per track for a minimum-ionising particle is 30 ps at the start of lifetime, increasing to 50 ps at the end of HL-LHC operation. The high-precision timing information improves the pileup reduction to improve the forward object reconstruction, complementing the capabilities of the upgraded Inner Tracker (ITk) in the forward regions of ATLAS and leading to an improved performance for both jet and lepton reconstruction. These improvements in object reconstruction performance translate into sensitivity gains and enhance the reach of the ATLAS physics programme at the HL-LHC. In addition, the HGTD offers unique capabilities for the online and offline luminosity determination, an important requirement for precision physics measurements.
The top quark mass is measured in the $t\bar{t}\to$ dilepton channel (lepton $= e, \mu$) using ATLAS data recorded in the year 2012 at the LHC. The data were taken at a proton--proton centre-of-mass ...energy of $\sqrt{s}=$ 8 TeV and correspond to an integrated luminosity of about 20.2 fb$^{-1}$. Exploiting the template method, and using the distribution of invariant masses of lepton--b-jet pairs, the top quark mass is measured to be $m_{top} =$ 172.99 $\pm$ 0.41 (stat) $\pm$ 0.74 (syst) GeV, with a total uncertainty of 0.84 GeV. Finally, a combination with previous ATLAS $m_{top}$ measurements from $\sqrt{s}=$7 TeV data in the $t\bar{t}\to$ dilepton and $t\bar{t}\to$ lepton+jets channels results in $m_{top} =$ 172.84 $\pm$ 0.34 (stat) $\pm$ 0.61 (syst) GeV, with a total uncertainty of 0.70 GeV.
This paper describes a measurement of the inclusive top quark pair production cross-section ($\sigma_{t\bar{t}}$) with a data sample of 3.2 fb$^{-1}$ of proton--proton collisions at a centre-of-mass ...energy of $\sqrt{s}$=13 TeV, collected in 2015 by the ATLAS detector at the LHC. This measurement uses events with an opposite-charge electron--muon pair in the final state. Jets containing $b$-quarks are tagged using an algorithm based on track impact parameters and reconstructed secondary vertices. The numbers of events with exactly one and exactly two $b$-tagged jets are counted and used to determine simultaneously $\sigma_{t\bar{t}}$ and the efficiency to reconstruct and $b$-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section is measured to be: $\sigma_{t\bar{t}}$= 818 $\pm$ 8 (stat) $\pm$ 27 (syst) $\pm$ 19 (lumi) $\pm$ 12 (beam) pb, where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, the integrated luminosity and the LHC beam energy, giving a total relative uncertainty of 4.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. A fiducial measurement corresponding to the experimental acceptance of the leptons is also presented.
Differential cross sections for the production of at least four jets have been measured in proton--proton collisions at $\sqrt{s} = 8$ TeV at the Large Hadron Collider using the ATLAS detector. The ...dataset corresponds to an integrated luminosity of 20.3 $fb^{-1}$. The cross sections, corrected for detector effects, are compared to leading-order and next-to-leading-order calculations as a function of the jet momenta, invariant masses, minimum and maximum opening angles and other kinematic variables.
This paper reports inclusive and differential measurements of the $t\bar{t}$ charge asymmetry $A_{\textrm{C}}$ in 20.3 fb$^{-1}$ of $\sqrt{s} = 8$ TeV $pp$ collisions recorded by the ATLAS experiment ...at the Large Hadron Collider at CERN. Three differential measurements are performed as a function of the invariant mass, transverse momentum and longitudinal boost of the $t\bar{t}$ system. The $t\bar{t}$ pairs are selected in the single-lepton channels ($e$ or $\mu$) with at least four jets, and a likelihood fit is used to reconstruct the $t\bar{t}$ event kinematics. A Bayesian unfolding procedure is performed to infer the asymmetry at parton level from the observed data distribution. The inclusive $t\bar{t}$ charge asymmetry is measured to be $A_{\textrm{C}} = 0.009 \pm 0.005$ (stat.$+$syst.). The inclusive and differential measurements are compatible with the values predicted by the Standard Model.
A search is performed for an excited muon in the channel pp→μμ∗→μμ jet jet, assuming both the production and decay occur via a contact interaction. The analysis is based on 20.3 fb−1 of pp collision ...data at a centre-of-mass energy of s√ = 8 TeV taken with the ATLAS detector at the Large Hadron Collider. No evidence of excited muons is found, and limits are set at the 95% confidence level on the cross section times branching ratio as a function of the excited-muon mass mμ∗. For mμ∗ between 1.3 TeV and 3.0 TeV, the upper limit on σB(μ∗→μqq¯) is between 0.6 and 1 fb. Limits on σB are converted to lower bounds on the compositeness scale Λ. In the limiting case Λ=mμ∗, excited muons with a mass below 2.8 TeV are excluded. With the same model assumptions, these limits at larger μ∗ masses improve upon previous limits from searches based on the decay μ∗→μγ.
The inclusive jet cross-section is measured in proton-proton collisions at a centre-of-mass energy of 7 TeV using a data set corresponding to an integrated luminosity of 4.5 fb$^{-1}$ collected with ...the ATLAS detector at the Large Hadron Collider in 2011. Jets are identified using the anti-$k_t$ algorithm with radius parameter values of 0.4 and 0.6. The double-differential cross-sections are presented as a function of the jet transverse momentum and the jet rapidity, covering jet transverse momenta from 100 GeV to 2 TeV. Next-to-leading-order QCD calculations corrected for non-perturbative effects and electroweak effects, as well as Monte Carlo simulations with next-to-leading-order matrix elements interfaced to parton showering, are compared to the measured cross-sections. A quantitative comparison of the measured cross-sections to the QCD calculations using several sets of parton distribution functions is performed.
A search is presented for a narrow diboson resonances decaying to $WW$ or $WZ$ in the final state where one $W$ boson decays leptonically (to an electron or a muon plus a neutrino) and the other ...$W/Z$ boson decays hadronically. The analysis is performed using an integrated luminosity of 20.3 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the LHC. No evidence for resonant diboson production is observed, and resonance masses below 700 GeV and 1490 GeV are excluded at 95% confidence level for the spin-2 Randall-Sundrum bulk graviton $G^*$ with coupling constant of 1.0 and the extended gauge model $W'$ boson respectively.
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