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The first measurement of neutron emission in electromagnetic dissociation of 208Pb nuclei at the LHC is presented. The measurement is performed using the neutron Zero Degree Calorimeters of the ALICE experiment, which detect neutral particles close to beam rapidity. The measured cross sections of single and mutual electromagnetic dissociation of Pb nuclei at sNN−−−√ = 2.76 TeV with neutron emission are σsingle EMD=187.4±0.2 (stat.) +13.2−11.2 (syst.) b and σmutual EMD=5.7±0.1 (stat.) ±0.4 (syst.) b, respectively. The experimental results are compared to the predictions from a relativistic electromagnetic dissociation model.
Knowledge about the biogeographic affinities of the world’s tropical forests helps to better understand regional differences in forest structure, diversity, composition, and dynamics. Such understanding will enable anticipation of region-specific responses to global environmental change. Modern phylogenies, in combination with broad coverage of species inventory data, now allow for global biogeographic analyses that take species evolutionary distance into account. Here we present a classification of the world’s tropical forests based on their phylogenetic similarity. We identify five principal floristic regions and their floristic relationships: (i) Indo-Pacific, (ii) Subtropical, (iii) African, (iv) American, and (v) Dry forests. Our results do not support the traditional neo- versus paleotropical forest division but instead separate the combined American and African forests from their Indo-Pacific counterparts. We also find indications for the existence of a global dry forest region, with representatives in America, Africa, Madagascar, and India. Additionally, a northern-hemisphere Subtropical forest region was identified with representatives in Asia and America, providing support for a link between Asian and American northern-hemisphere forests.
Measurement of electrons from semileptonic heavy-flavor hadron decays in pp collisions at √s = 7 TeV
(2012)
The differential production cross section of electrons from semileptonic heavy-flavour hadron decays has been measured at mid-rapidity (|y|<0.5) in proton-proton collisions at s√=7 TeV with ALICE at the LHC. Electrons were measured in the transverse momentum range 0.5 <pT< 8 GeV/c. Predictions from a fixed order perturbative QCD calculation with next-to-leading-log resummation agree with the data within the theoretical and experimental uncertainties.
The production of K∗(892)0 and ϕ(1020) in pp collisions at s√=7 TeV was measured by the ALICE experiment at the LHC. The yields and the transverse momentum spectra d2N/dydpT at midrapidity |y|<0.5 in the range 0<pT<6 GeV/c for K∗(892)0 and 0.4<pT<6 GeV/c for ϕ(1020) are reported and compared to model predictions. Using the yield of pions, kaons, and Omega baryons measured previously by ALICE at s√=7 TeV, the ratios K∗/K−, ϕ/K∗, ϕ/K−, ϕ/π−, and (Ω + Ω¯¯¯¯)/ϕ are presented. The values of the K∗/K−, ϕ/K∗ and ϕ/K− ratios are similar to those found at lower centre-of-mass energies. In contrast, the ϕ/π− ratio, which has been observed to increase with energy, seems to saturate above 200 GeV. The (Ω + Ω¯¯¯¯)/ϕ ratio in the pT range 1-5 GeV/c is found to be in good agreement with the prediction of the HIJING/BB v2.0 model with a strong colour field.
We report the first measurement of the net-charge fluctuations in Pb-Pb collisions at sNN−−−√ = 2.76 TeV, measured with the ALICE detector at the CERN Large Hadron Collider. The dynamical fluctuations per unit entropy are observed to decrease when going from peripheral to central collisions. An additional reduction in the amount of fluctuations is seen in comparison to the results from lower energies. We examine the dependence of fluctuations on the pseudorapidity interval, which may account for the dilution of fluctuations during the evolution of the system. We find that the fluctuations at LHC are smaller compared to the measurements at the Relativistic heavy Ion Collider (RHIC), and as such, closer to what has been theoretically predicted for the formation of Quark-Gluon Plasma (QGP).
Measurements of charge-dependent azimuthal correlations with the ALICE detector at the LHC are reported for Pb-Pb collisions at √𝑠𝑁𝑁=2.76 TeV. Two- and three-particle charge-dependent azimuthal correlations in the pseudorapidity range |𝜂|<0.8 are presented as a function of the collision centrality, particle separation in pseudorapidity, and transverse momentum. A clear signal compatible with a charge-dependent separation relative to the reaction plane is observed, which shows little or no collision energy dependence when compared to measurements at RHIC energies. This provides a new insight for understanding the nature of the charge-dependent azimuthal correlations observed at RHIC and LHC energies.
Two-pion correlation functions in Au+Au collisions at sqrt[sNN] = 130 GeV have been measured by the STAR (solenoidal tracker at RHIC) detector. The source size extracted by fitting the correlations grows with event multiplicity and decreases with transverse momentum. Anomalously large sizes or emission durations, which have been suggested as signals of quark-gluon plasma formation and rehadronization, are not observed. The Hanbury Brown-Twiss parameters display a weak energy dependence over a broad range in sqrt[sNN].
The first measurements of light antinucleus production in Au+Au collisions at the Relativistic Heavy-Ion Collider are reported. The observed production rates for d-bar and 3He-bar are much larger than in lower energy nucleus-nucleus collisions. A coalescence model analysis of the yields indicates that there is little or no increase in the antinucleon freeze-out volume compared to collisions at CERN SPS energy. These analyses also indicate that the 3He-bar freeze-out volume is smaller than the d-bar freeze-out volume.
We present the first measurement of midrapidity vector meson phi production in Au+Au collisions at RHIC (sqrt[sNN]=130 GeV) from the STAR detector. For the 11% highest multiplicity collisions, the slope parameter from an exponential fit to the transverse mass distribution is T=379±50(stat)±45(syst) MeV, the yield dN/dy=5.73±0.37(stat)±0.69(syst) per event, and the ratio N phi /Nh- is found to be 0.021±0.001(stat)±0.004(syst). The measured ratio N phi /Nh- and T for the phi meson at midrapidity do not change for the selected multiplicity bins.
An accurate measurement of the 140Ce(n,γ) energy-dependent cross-section was performed at the n_TOF facility at CERN. This cross-section is of great importance because it represents a bottleneck for the s-process nucleosynthesis and determines to a large extent the cerium abundance in stars. The measurement was motivated by the significant difference between the cerium abundance measured in globular clusters and the value predicted by theoretical stellar models. This discrepancy can be ascribed to an overestimation of the 140Ce capture cross-section due to a lack of accurate nuclear data. For this measurement, we used a sample of cerium oxide enriched in 140Ce to 99.4%. The experimental apparatus consisted of four deuterated benzene liquid scintillator detectors, which allowed us to overcome the difficulties present in the previous measurements, thanks to their very low neutron sensitivity. The accurate analysis of the p-wave resonances and the calculation of their average parameters are fundamental to improve the evaluation of the 140Ce Maxwellian-averaged cross-section.
Sphingolipide sind an zahlreichen physiologischen und pathophysiologischen Prozessen im Körper beteiligt. Vor Allem das sowohl auto- als auch paracrinwirkende Sphingosin-1-Phosphat (S1P) spielt dabei eine essentielle Rolle. Ein Großteil der S1P-vermittelten / regulatorischen Effekte beruht auf dessen Wechselwirkung mit den fünf G Protein-gekoppelten S1P-Rezeptoren (S1P1-5). S1P nimmt hierüber Einfluss auf das Schicksal der Zellen (Proliferation, Überleben, Migration), die Zellmobilität, die Angiogenese und das Immunsystem. Viele der über die S1P-Rezeptor-vermittelten Effekte sowie deren Rolle und Funktion in einzelnen Geweben oder Organen sind bis heute noch nicht komplett verstanden bzw. erklärbar. Pharmakologische Tools können einen wichtigen Beitrag zur weiteren Erforschung und zum Verständnis des komplexen Sphingolipidnetzwerks leisten. Ausgehend von einer substituierten Diaryl-1,2,4-oxadiazol-Leitstruktur, die in der Literatur als privilegierte Struktur für S1P1-Rezeptoragonisten gilt, und dem selektiven S1P1-Agonisten SEW2871 wurden verschiedene Liganden mit unterschiedlichen chemischen Gruppen synthetisiert. Nach der Etablierung eines Synthesewegs zu etherverknüpften Aminoethan-diphenyl-1,2,4-oxadiazolen wurden diese in die fluoreszierenden Dansyl-, Isoindolin-, Pyridinium-Dye- und Coumarin-gelabelten Derivate überführt. Außerdem wurde eine einfache und optimierte Syntheseroute zu dem kleinen, umgebungsempfindlichen Fluorophor 4-(Dimethyl-amino)phthalimid (4-DMAP) entwickelt, dass entlang eines linearen Synthesewegs in guten Aus-beuten auch mit den Trifluormethyl- und Methyl-substituierten Diphenyloxadiazol-Grundstrukturen zu fluoreszenzmarkierten Derivaten umgesetzt wurde. Neben den fluoreszenzmarkierten Liganden für den S1P1-Rezeptor wurden zudem drei substituierte Phenyloxadiazolaniline zu den entspre-chenden Acrylamiden umgesetzt, die als kovalente Labeling Tools eingesetzt werden können. Durch die Synthese von Trifluormethyl- und Cyano-substituierten 4-DMAP-markierten Diaryloxa-diazolen sowie von Arylpropansäurederivaten wurde die gewählte Leitstruktur auf Grundlage einer ersten Affinitätstestungen verfeinert. Dabei wurde die zuvor entwickelte Synthese-strategie optimiert. Der Aufbau der Arylpropansäuren erfolgte durch eine Heck-Reaktion mit Acroleindiethylacetal. Durch den Wechsel der Synthesestrategie von 1. Heck-Reaktion und 2. Oxadiazolringschluss zur umgekehrten Vorgehensweise konnte eine Reihe von synthetischen Problemen umgangen werden und die Gesamtausbeute gesteigert werden.
Zwei der fluoreszenzmarkierten S1P1-Liganden mit verfeinerter Grundstruktur zeigten eine durch die Bindung an den S1P1-Rezeptor verursachte Internalisierung des Rezeptors, die durch die GFP-Markierung unter dem Fluoreszenzmikroskop sichtbar gemacht wurde. Diese Internalisierung lieferte weitere Hinweise, dass die beiden Substanzen eine durch Bindung am S1P1-Rezeptor verursachte, agonistische Wirkung haben. Die weitere pharmakologische Charakterisierung aller synthetisierten, funktionellen Liganden im Bereich der Sphingolipide steht noch aus. Leukotriene (LT) sind wichtige Lipidmediatoren, die durch Oxygenierung von Arachidonsäure entstehen. Sie nehmen eine zentrale Rolle ein in der Entstehung und dem Voranschreiten von Entzündungen, allergischen Reaktionen, Asthma, kardiovaskulären Erkrankungen und auch bei Krebserkrankungen. Das Schlüsselenzym der LT-Biosynthese ist das Enzym 5-Lipoxygenase (5-LO). Zur Behandlung von LT-assoziierten Krankheiten sind bis heute nur zwei Wirkstoffe zugelassen, die in den LT-Stoffwechsel eingreifen: der Cys-LT-Rezeptorantagonist Montelukast (Singulair®) und der eisenchelatisierende 5-LO-Inhibitor Zileuton (Zyflo®, nur in den USA zugelassen). Es besteht daher ein großer Bedarf an neuen, selektiven Liganden. C06 ist einer der am besten charakterisierten Vertreter einer neue Klasse an potenten, direkten und selektiven 5-LO-Inhibitoren: den Aryliden-Aryl-Thiazolonen, die ein großes Potential für die Entwicklung neuer anti-Leukotrien Arzneistoffe aufweisen. In-vivo-Experimente haben jedoch gezeigt, dass C06 und seine Derivaten nicht optimale pharmakologische Profile besitzen und zudem nur in geringem Maße im Wässrigen löslich sind. Durch die Optimierung und Etablierung einer mikrowellenassistierte Drei-Komponenten-one-pot-Synthese sowie einer verwandten zweistufigen Synthese zum Aufbau der Aryliden-Aryl-Thiazolone, konnte die Reaktionszeit verringert werden und daher die Isolierung und Aufreinigung vereinfacht werden. Zur Steigerung der Löslichkeit der Aryliden-Aryl-Thiazolone in wässrigen Systemen und zur weiteren Erforschung der SAR wurde einige Derivate mit polaren Substituenten, unterschiedlichen Wasserstoffbrückenbindungs-Eigenschaften, Morpholinderivate und verschiedene heteroaromatische Aryliden-Aryl-Thiazolone hergestellt, wobei die Heteroarylderivate aufgrund ihrer niedrigeren, berechneten Lipophilie (clogP) und höheren berechneter Löslichkeit (clogS) ausgewählt wurden. Für alle synthetisierten Derivate wurde die Inhibition der 5-LO-Produktbildung unter zellfreien (S100) und unter zellulären Bedingungen (PMNL) bestimmt. Zudem wurden für einige Derivate die experimentellen Löslichkeiten in DMSO und in Puffer grob ermittelt. Die Ergebnisse zeigen, dass alle besser löslichen Derivate einen höheren IC50-Wert im zellbasierten Assay aufweisen bzw. die potentesten Substanzen nicht gut im Wässrigen löslich sind. Zur Charakterisierung der unbekannten, allosterischen Bindestelle der Aryliden-Aryl-Thiazolone wurde eine Reihe von zum kovalenten bzw. zum Photoaffinity-Labeling fähigen Aryliden-Aryl-Thiazolonderivaten synthetisiert. Alle Derivate wiesen gute bis sehr gute 5-LO Affinitäten auf und durch Vorversuche konnte die prinzipielle Eignung zum Photoaffinity-Labeling gezeigt werden. Da sowohl die polaren als auch die heteroarylbasierten Aryliden-Aryl-Thiazolone die bekannte kontinuierliche SAR wiederspiegelten und keine hohe Wasserlöslichkeit bei gleichzeitiger hoher 5-LO-Inhibition erreicht werden konnte, wurden die einzelnen Element des Aryliden-Aryl-Thiazolon-grundgerüstes durch individuelle Synthesen variiert. Diese Kernvariations- und die an der Aryliden-einheit variierten Derivate haben die SAR der Aryliden-Aryl-Thiazolone deutlich erweitert und konnten die für die 5-LO-Aktivität wichtigen Elemente identifizieren. Dadurch ist es gelungen, die 2-Aryl-5-aryl(methyl)thiazol-4-ole als 5-LO-Leitstruktur zu erschließen, die sowohl unter zellfreien Bedingungen (S100) als auch im zellbasierten Assay (PMNL) Aktivitäten im nanomolaren Bereich erreichen. Mit den 2-Aryl-5-arylmethylthiazol-4-olen konnte außerdem die Löslichkeit in DMSO und vor allem im Wässrigen, verglichen zu C06, deutlich erhöht werden. ST-1829 ist ein C06-Analogon, dass die Nachteile im pharmakologischen Profil von C06 eliminiert und zu einem neuen, effektiven Wirkstoff in der anti-Leukotrien Therapie weiter entwickelt werden kann.
We report first results on elliptic flow of identified particles at midrapidity in Au+Au collisions at sqrt[sNN] = 130 GeV using the STAR TPC at RHIC. The elliptic flow as a function of transverse momentum and centrality differs significantly for particles of different masses. This dependence can be accounted for in hydrodynamic models, indicating that the system created shows a behavior consistent with collective hydrodynamical flow. The fit to the data with a simple model gives information on the temperature and flow velocities at freeze-out.
The minimum-bias multiplicity distribution and the transverse momentum and pseudorapidity distributions for central collisions have been measured for negative hadrons ( h-) in Au+Au interactions at sqrt[sNN] = 130 GeV. The multiplicity density at midrapidity for the 5% most central interactions is dNh-/d eta | eta = 0 = 280±1(stat)±20(syst), an increase per participant of 38% relative to pp-bar collisions at the same energy. The mean transverse momentum is 0.508±0.012 GeV/c and is larger than in central Pb+Pb collisions at lower energies. The scaling of the h- yield per participant is a strong function of pperp. The pseudorapidity distribution is almost constant within | eta |<1.
We report the first measurement of inclusive antiproton production at midrapidity in Au+Au collisions at sqrt[sNN] = 130 GeV by the STAR experiment at RHIC. The antiproton transverse mass distributions in the measured transverse momentum range of 0.25<pperp<0.95 GeV/c are found to fall less steeply for more central collisions. The extrapolated antiproton rapidity density is found to scale approximately with the negative hadron multiplicity density.
We report results on the ratio of midrapidity antiproton-to-proton yields in Au+Au collisions at sqrt[sNN] = 130 GeV per nucleon pair as measured by the STAR experiment at RHIC. Within the rapidity and transverse momentum range of | y|<0.5 and 0.4<pt<1.0 GeV/c, the ratio is essentially independent of either transverse momentum or rapidity, with an average of 0.65±0.01(stat)±0.07(syst) for minimum bias collisions. Within errors, no strong centrality dependence is observed. The results indicate that at this RHIC energy, although the p-p-bar pair production becomes important at midrapidity, a significant excess of baryons over antibaryons is still present.
Exploring biophysical properties of virus-encoded components and their requirement for virus replication is an exciting new area of interdisciplinary virological research. To date, spatial resolution has only rarely been analyzed in computational/biophysical descriptions of virus replication dynamics. However, it is widely acknowledged that intracellular spatial dependence is a crucial component of virus life cycles. The hepatitis C virus-encoded NS5A protein is an endoplasmatic reticulum (ER)-anchored viral protein and an essential component of the virus replication machinery. Therefore, we simulate NS5A dynamics on realistic reconstructed, curved ER surfaces by means of surface partial differential equations (sPDE) upon unstructured grids. We match the in silico NS5A diffusion constant such that the NS5A sPDE simulation data reproduce experimental NS5A fluorescence recovery after photobleaching (FRAP) time series data. This parameter estimation yields the NS5A diffusion constant. Such parameters are needed for spatial models of HCV dynamics, which we are developing in parallel but remain qualitative at this stage. Thus, our present study likely provides the first quantitative biophysical description of the movement of a viral component. Our spatio-temporal resolved ansatz paves new ways for understanding intricate spatial-defined processes central to specfic aspects of virus life cycles.
Background/Objectives: Sharing the bed with a partner is common among adults and impacts sleep quality with potential implications for mental health. However, hitherto findings are contradictory and particularly polysomnographic data on co-sleeping couples are extremely rare. The present study aimed to investigate the effects of a bed partner's presence on individual and dyadic sleep neurophysiology.
Methods: Young healthy heterosexual couples underwent sleep-lab-based polysomnography of two sleeping arrangements: individual sleep and co-sleep. Individual and dyadic sleep parameters (i.e., synchronization of sleep stages) were collected. The latter were assessed using cross-recurrence quantification analysis. Additionally, subjective sleep quality, relationship characteristics, and chronotype were monitored. Data were analyzed comparing co-sleep vs. individual sleep. Interaction effects of the sleeping arrangement with gender, chronotype, or relationship characteristics were moreover tested.
Results: As compared to sleeping individually, co-sleeping was associated with about 10% more REM sleep, less fragmented REM sleep (p = 0.008), longer undisturbed REM fragments (p = 0.0006), and more limb movements (p = 0.007). None of the other sleep stages was significantly altered. Social support interacted with sleeping arrangement in a way that individuals with suboptimal social support showed the biggest impact of the sleeping arrangement on REM sleep. Sleep architectures were more synchronized between partners during co-sleep (p = 0.005) even if wake phases were excluded (p = 0.022). Moreover, sleep architectures are significantly coupled across a lag of ± 5min. Depth of relationship represented an additional significant main effect regarding synchronization, reflecting a positive association between the two. Neither REM sleep nor synchronization was influenced by gender, chronotype, or other relationship characteristics.
Conclusion: Depending on the sleeping arrangement, couple's sleep architecture and synchronization show alterations that are modified by relationship characteristics. We discuss that these alterations could be part of a self-enhancing feedback loop of REM sleep and sociality and a mechanism through which sociality prevents mental illness.
Nowadays, several options are available to treat patients with conductive or mixed hearing loss. Whenever surgical intervention is not possible or contra-indicated, and amplification by a conventional hearing device (e.g., behind-the-ear device) is not feasible, then implantable hearing devices are an indispensable next option. Implantable bone-conduction devices and middle-ear implants have advantages but also limitations concerning complexity/invasiveness of the surgery, medical complications, and effectiveness. To counsel the patient, the clinician should have a good overview of the options with regard to safety and reliability as well as unequivocal technical performance data. The present consensus document is the outcome of an extensive iterative process including ENT specialists, audiologists, health-policy scientists, and representatives/technicians of the main companies in this field. This document should provide a first framework for procedures and technical characterization to enhance effective communication between these stakeholders, improving health care.