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Harmonic decomposition of two particle angular correlations in Pb–Pb collisions at √sNN=2.76 TeV
(2012)
Angular correlations between unidentified charged trigger (t) and associated (a) particles are measured by the ALICE experiment in Pb–Pb collisions at √sNN=2.76 TeV for transverse momenta 0.25<pTt,a<15 GeV/c, where pTt>pTa. The shapes of the pair correlation distributions are studied in a variety of collision centrality classes between 0 and 50% of the total hadronic cross section for particles in the pseudorapidity interval |η|<1.0. Distributions in relative azimuth Δϕ≡ϕt−ϕa are analyzed for |Δη|≡|ηt−ηa|>0.8, and are referred to as “long-range correlations”. Fourier components VnΔ≡〈cos(nΔϕ)〉 are extracted from the long-range azimuthal correlation functions. If particle pairs are correlated to one another through their individual correlation to a common symmetry plane, then the pair anisotropy VnΔ(pTt,pTa) is fully described in terms of single-particle anisotropies vn(pT) as VnΔ(pTt,pTa)=vn(pTt)vn(pTa). This expectation is tested for 1⩽n⩽5 by applying a global fit of all VnΔ(pTt,pTa) to obtain the best values vn{GF}(pT). It is found that for 2⩽n⩽5, the fit agrees well with data up to pTa∼3–4 GeV/c, with a trend of increasing deviation as pTt and pTa are increased or as collisions become more peripheral. This suggests that no pair correlation harmonic can be described over the full 0.25<pT<15 GeV/c range using a single vn(pT) curve; such a description is however approximately possible for 2⩽n⩽5 when pTa<4 GeV/c. For the n=1 harmonic, however, a single v1(pT) curve is not obtained even within the reduced range pTa<4 GeV/c.
The study of the azimuthal anisotropy of inclusive muons produced in p–Pb collisions at √sNN=8.16 TeV, using the ALICE detector at the LHC is reported. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, v2, is performed as a function of transverse momentum pT in the 0–20% high-multiplicity interval at both forward (2.03<yCMS<3.53) and backward (−4.46<yCMS<−2.96) rapidities over a wide pT range, 0.5<pT<10 GeV/c, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at pT>2 GeV/c. The v2 coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward–central two-particle correlations. Both techniques give compatible results. A positive v2 is measured at both forward and backward rapidities with a significance larger than 4.7σ and 7.6σ, respectively, in the interval 2<pT<6 GeV/c. Comparisons with previous measurements in p–Pb collisions at √sNN=5.02 TeV, and with AMPT and CGC-based theoretical calculations are discussed. The findings impose new constraints on the theoretical interpretations of the origin of the collective behaviour in small collision systems.
Production of inclusive charmonia in pp collisions at center-of-mass energy of √s = 13 TeV and p–Pb collisions at center-of-mass energy per nucleon pair of √sNN = 8.16 TeV is studied as a function of charged-particle pseudorapidity density with ALICE. Ground and excited charmonium states (J/ψ, ψ(2S)) are measured from their dimuon decays in the interval of rapidity in the center-of-mass frame 2.5 < ycms < 4.0 for pp collisions, and 2.03 < ycms < 3.53 and −4.46 < ycms < −2.96 for p–Pb collisions. The charged-particle pseudorapidity density is measured around midrapidity (|η| < 1.0). In pp collisions, the measured charged-particle multiplicity extends to about six times the average value, while in p-Pb collisions at forward (backward) rapidity a multiplicity corresponding to about three (four) times the average is reached. The ψ(2S) yield increases with the charged-particle pseudorapidity density. The ratio of ψ(2S) over J/ψ yield does not show a significant multiplicity dependence in either colliding system, suggesting a similar behavior of J/ψ and ψ(2S) yields with respect to charged-particle pseudorapidity density. Results for the ψ(2S) yield and its ratio with respect to J/ψ agree with available model calculations.
In particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD). These partons subsequently emit further partons in a process that can be described as a parton shower which culminates in the formation of detectable hadrons. Studying the pattern of the parton shower is one of the key experimental tools for testing QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a heavy quark of mass mQ and energy E, within a cone of angular size mQ/E around the emitter. Previously, a direct observation of the dead-cone effect in QCD had not been possible, owing to the challenge of reconstructing the cascading quarks and gluons from the experimentally accessible hadrons. We report the direct observation of the QCD dead cone by using new iterative declustering techniques to reconstruct the parton shower of charm quarks. This result confirms a fundamental feature of QCD. Furthermore, the measurement of a dead-cone angle constitutes a direct experimental observation of the non-zero mass of the charm quark, which is a fundamental constant in the standard model of particle physics.
At particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD). The vacuum is not transparent to the partons and induces gluon radiation and quark pair production in a process that can be described as a parton shower. Studying the pattern of the parton shower is one of the key experimental tools in understanding the properties of QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a heavy quark of mass m and energy E, within a cone of angular size m/E around the emitter. A direct observation of the dead-cone effect in QCD has not been possible until now, due to the challenge of reconstructing the cascading quarks and gluons from the experimentally accessible bound hadronic states. We report the first direct observation of the QCD dead-cone by using new iterative declustering techniques to reconstruct the parton shower of charm quarks. This result confirms a fundamental feature of QCD, which is derived more generally from its origin as a gauge quantum field theory. Furthermore, the measurement of a dead-cone angle constitutes a direct experimental observation of the non-zero mass of the charm quark, which is a fundamental constant in the standard model of particle physics.
A measurement of the transverse momentum spectra of jets in Pb-Pb collisions at sNN−−−√=2.76 TeV is reported. Jets are reconstructed from charged particles using the anti-kT jet algorithm with jet resolution parameters R of 0.2 and 0.3 in pseudo-rapidity |η|<0.5. The transverse momentum pT of charged particles is measured down to 0.15 GeV/c which gives access to the low pT fragments of the jet. Jets found in heavy-ion collisions are corrected event-by-event for average background density and on an inclusive basis (via unfolding) for residual background fluctuations and detector effects. A strong suppression of jet production in central events with respect to peripheral events is observed. The suppression is found to be similar to the suppression of charged hadrons, which suggests that substantial energy is radiated at angles larger than the jet resolution parameter R=0.3 considered in the analysis. The fragmentation bias introduced by selecting jets with a high pT leading particle, which rejects jets with a soft fragmentation pattern, has a similar effect on the jet yield for central and peripheral events. The ratio of jet spectra with R=0.2 and R=0.3 is found to be similar in Pb-Pb and simulated PYTHIA pp events, indicating no strong broadening of the radial jet structure in the reconstructed jets with R<0.3.
Die zellfreie Proteinsynthese hat sich in den letzten Jahren zu einem potenten Werkzeug – auch in der Produktion von Membranproteinen – entwickelt. Da keine lebenden Zellen genutzt werden, kann der Prozess der präparativen Membranproteinproduktion vereinfacht und individuell optimiert werden. Im Gegensatz zu konventionellen zellbasierten Expressionssystemen gewährleistet die zellfreie Proteinsynthese die direkte Zugänglichkeit zum Reaktionsort und damit die Möglichkeit der unmittelbaren Kontrolle. Dies ermöglicht eine genaue Anpassung der Reaktionsbedingungen auf das Zielprotein. Die Verbesserung und Entwicklung neuer Modi der zellfreien Membranproteinsynthese war ein Teil der vorliegenden Arbeit. Setzt man dem Zellfrei-System von Außen keine hydrophobe Umgebung zu, so präzipitiert das neu-synthetisierte Membranprotein im Reaktionsmix (P-CF). Interessanter Weise unterscheiden sich diese Präzipitate von den aus der E.coli zellbasierten Proteinproduktion bekannten Einschlußkörperchen, da sie sich teilweise leicht in mildem Detergenz resolubilisieren lassen. Zudem konnte für verschiedene Transportproteine, die aus Präzpitat resolubilisiert und danach in Liposomen rekonstituiert wurden, spezifische Transportaktivität gezeigt werden (z.B. eukaryotische Ionentransporter, Multi-Drug Resistenzproteine von E.coli). Alternativ können die Membranproteine direkt, durch die Zugabe von Detergenzien in den Reaktionsmix, solubilisiert werden (D-CF). Um die einzelnen Expressionsmodi zu optimieren wurden 24 gebräuchliche Detergenzien auf ihre Eigenschaft hin gestestet, strukturell sehr unterschiedliche Membranproteine zu solubilisieren. Die Familie der langkettigen Polyoxyethylen-alkyl Ether hat sich dabei als sehr geeignet erwiesen um das prokaryotische α-helikale Multi-Drug Resistenzprotein EmrE, den bakteriellen vornehmlich aus ß-sheets bestehenden Transporter Tsx und den eukaryotischen G-Protein gekoppelten Vasopressin Rezeptor V2R direkt im D-CF Modus zu solubilisieren. Zudem konnte eine Abhängigkeit der spezifischen Aktivität von Tsx vom verwendeten Expressionsmodus bzw. des verwendeten Detergenz mit Hilfe der Black Lipid Membrane´ Methode gezeigt werden. Die Expression eines repäsentativen Teils von 134 Zielproteinen des inneren Membranproteoms von E.coli wurde in drei verschiedenen Zellfrei-Expressionsmodi getestet. Ein an jedes Zielprotein des Membranroteoms C-terminal fusioniertes GFP diente der Konzentrationsbestimmung im D-CF Expressionsmodus. Die Faltung von GFP ist in Anwesenheit von Detergenz signifikant reduziert. Zunächst wurden alle Zielproteine in einem batch´ System im D-CF Modus im Mikrotiterplatten Maßstab mit Hilfe eines Roboters hergestellt. Die Etablierung einer robotergestützten Plattform, welche das Pipettieren, Inkubieren und Detektieren kombiniert, diente als Grundlage für den Herstellungsprozess des Membranroteoms von E.coli in einem Medium-Durchsatz Verfahren in batch´ Konfiguration. In dieser ersten Stufe des Screens im D-CF Modus konnten 84 Zielproteine (63%) aufgrund der detektierten GFP-Fluoreszens in Mengen von 1 bis 60μg pro mL Reaktion als erfolgreich produziert identifiziert werden. Zudem wurde das Membranproteom in dem effektiveren continous exchange (CE) Verfahren im P-CF, wie auch im D-CF Modus wiederholt exprimiert. Im Vergleich zur batch´ Konfiguration konnten im CE D-CF Modus deutlich mehr Zielproteine (75%) als positiv identifiziert werden. 16 Zielproteine wurden dabei bereits in Expressionsmengen von mehr als 100μg solubilisierte Membranproteinfusion pro mL Reaktionsmix gewonnen. 99 Zielproteine (74%) konnten als positiv identifiziert werden, nachdem die unlösliche Fraktion der CE P-CF Reaktion elektrophoretisch getrennt und angefärbt wurde. Für 66 Kandidaten (49%) stellt das produzierte Protein nach Coomassie-Färbung eine dominante Bande, und damit (semi-)präparative Proteinmengen, dar. Der Erhalt von Detergenz-solubilisierten Membranproteinproben von hoher Qualität ist ein wichtiger Schritt zur Gewinnung struktureller sowie biochemischer Daten. Das E.coli α-helikale Multi- Drug Resistenz Protein SugE konnte im CE P-CF Verfahren in präparativen Mengen von mehr als 2mg Protein pro mL des Reaktionsansatzes gewonnen werden. Durchgeführte analytische Größenausschlusschromatographie zeigte, dass der Transporter unter optimierten Reaktionsbedingungen in einem homogenen, schlanken Peak eluiert. Mittels elektronenmikroskopischer Gefrierbruchanalysen konnte eine effiziente und homogene Rekonstitution von SugE in E.coli Liposomen gezeigt werden. Bindungsstudien unter der Verwendung fluoreszensbasierter Anisotropie-Messungen haben gezeigt dass Proflavin – im Gegenteil zu Ethidium – ein Substrat von SugE ist. YedZ ist ein 24kDa leucinreiches Membranprotein mit sechs putativen Transmembransegmenten und enthält zwei Kofaktoren, ein Häm b und ein Flavin-mononukleotid (FMN). Im P-CF Modus exprimiertes YedZ kann effizient in den Detergenzien LMPG, LPPG, SDS und DPC resolubilisiert werden. Analytische Größenausschlusschromatographie zeigte einen symmetrischen Elutionspeak der apo-Form. Mittels CD-Spektroskopie des gereinigten apo-YedZ in 0.02% DDM wurde ein α-helikaler Sekundärstrukturanteil von 55% ermittelt. Zur Gewinnung von holo-YedZ wurde anstatt Hämb das chemisch verwandte Hemin eingesetzt. Die aufgenommenen UV/Vis Spektren der zellfrei produzierten holo-YedZ Proteinprobe in ihrer oxydierten und reduzierten Form, zeigen zu einer in vivo exprimierten Vergleichsprobe identische Absorptionsmaxima. Für sechs G-Protein gekoppelten Rezeptoren konnte die zellfreie Expression in präparativen Mengen gezeigt werden. Das Steroid-Derivat Digitonin, sowie einzelne Mitglieder der Detergenzfamilie der langkettigen Polyoxyethylen-alkyl Ether, wurden als am geeignetsten für die lösliche Expression der GPCRs im CE D-CF Verfahren ermittelt. Löslich in Anwesenheit von Brij78 produzierter GPCR Proben, zeigten nach Negativfärbung in elektronenmikroskopischen Einzelpartikelanalysen eine homogene Probenpräparation und geben Hinweis auf eine strukturelle Dimerisierug der Rezeptoren. Detergenzsolubilisierte Rezeptoren konnten in Liposomen, basierend auf E.coli Lipid-Mischungen, rekonstituiert werden. Elektronen-mikroskopische Gefrierbruchanalysen zeigten eine homogene Rekonstitution, welche auf eine funktionelle Faltung der Rezeptoren schließen lässt.
Peri-implantitis: summary and consensus statements of group 3. The 6th EAO Consensus Conference 2021
(2021)
Objective: To evaluate the influence of implant and prosthetic components on peri-implant tissue health. A further aim was to evaluate peri-implant soft-tissue changes following surgical peri-implantitis treatment. Materials and methods: Group discussions based on two systematic reviews (SR) and one critical review (CR) addressed (i) the influence of implant material and surface characteristics on the incidence and progression of peri-implantitis, (ii) implant and restorative design elements and the associated risk for peri-implant diseases, and (iii) peri-implant soft-tissue level changes and patient-reported outcomes following peri-implantitis treatment. Consensus statements, clinical recommendations, and implications for future research were discussed within the group and approved during plenary sessions. Results: Data from preclinical in vivo studies demonstrated significantly greater radiographic bone loss and increased area of inflammatory infiltrate at modified compared to non-modified surface implants. Limited clinical data did not show differences between modified and non-modified implant surfaces in incidence or progression of peri-implantitis (SR). There is some evidence that restricted accessibility for oral hygiene and an emergence angle of >30 combined with a convex emergence profile of the abutment/prosthesis are associated with an increased risk for peri-implantitis (CR). Reconstructive therapy for peri-implantitis resulted in significantly less soft-tissue recession, when compared with access flap. Implantoplasty or the adjunctive use of a barrier membrane had no influence on the extent of peri-implant mucosal recession following peri-implantitis treatment (SR).
This report provides a brief review of the 20th annual meeting of the German Language Branch of the Society of Environmental Toxicology and Chemistry (SETAC GLB) held from September 7th to 10th 2015 at ETH (Swiss Technical University) in Zurich, Switzerland. The event was chaired by Inge Werner, Director of the Swiss Centre for Applied Ecotoxicology (Ecotox Centre) Eawag-EPFL, and organized by a team from Ecotox Centre, Eawag, Federal Office of the Environment, Federal Office of Agriculture, and Mesocosm GmbH (Germany). Over 200 delegates from academia, public agencies and private industry of Germany, Switzerland and Austria attended and discussed the current state of science and its application presented in 75 talks and 83 posters. In addition, three invited keynote speakers provided new insights into scientific knowledge ‘brokering’, and—as it was the International Year of Soil—the important role of healthy soil ecosystems. Awards were presented to young scientists for best oral and poster presentations, and for best 2014 master and doctoral theses. Program and abstracts of the meeting (mostly in German) are provided as Additional file 1.
How long does it take to emit an electron from an atom? This question has intrigued scientists for decades. As such emission times are in the attosecond regime, the advent of attosecond metrology using ultrashort and intense lasers has re-triggered strong interest on the topic from an experimental standpoint. Here, we present an approach to measure such emission delays, which does not require attosecond light pulses, and works without the presence of superimposed infrared laser fields. We instead extract the emission delay from the interference pattern generated as the emitted photoelectron is diffracted by the parent ion’s potential. Targeting core electrons in CO, we measured a 2d map of photoelectron emission delays in the molecular frame over a wide range of electron energies. The emission times depend drastically on the photoelectrons’ emission directions in the molecular frame and exhibit characteristic changes along the shape resonance of the molecule.
Men and women differ substantially regarding height, weight, and body fat. Interestingly, previous work detecting genetic effects for waist-to-hip ratio, to assess body fat distribution, has found that many of these showed sex-differences. However, systematic searches for sex-differences in genetic effects have not yet been conducted. Therefore, we undertook a genome-wide search for sexually dimorphic genetic effects for anthropometric traits including 133,723 individuals in a large meta-analysis and followed promising variants in further 137,052 individuals, including a total of 94 studies. We identified seven loci with significant sex-difference including four previously established (near GRB14/COBLL1, LYPLAL1/SLC30A10, VEGFA, ADAMTS9) and three novel anthropometric trait loci (near MAP3K1, HSD17B4, PPARG), all of which were significant in women, but not in men. Of interest is that sex-difference was only observed for waist phenotypes, but not for height or body-mass-index. We found no evidence for sex-differences with opposite effect direction for men and women. The PPARG locus is of specific interest due to its link to diabetes genetics and therapy. Our findings demonstrate the importance of investigating sex differences, which may lead to a better understanding of disease mechanisms with a potential relevance to treatment options.