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The ALICE Collaboration reports the first fully-corrected measurements of the N-subjettiness observable for track-based jets in heavy-ion collisions. This study is performed using data recorded in pp and Pb−Pb collisions at centre-of-mass energies of √s=7 TeV and √sNN=2.76\,TeV, respectively. In particular the ratio of 2-subjettiness to 1-subjettiness, τ2/τ1, which is sensitive to the rate of two-pronged jet substructure, is presented. Energy loss of jets traversing the strongly interacting medium in heavy-ion collisions is expected to change the rate of two-pronged substructure relative to vacuum. The results are presented for jets with a resolution parameter of R=0.4 and charged jet transverse momentum of 40≤pT,jet≤60 GeV/c, which constitute a larger jet resolution and lower jet transverse momentum interval than previous measurements in heavy-ion collisions. This has been achieved by utilising a semi-inclusive hadron-jet coincidence technique to suppress the larger jet combinatorial background in this kinematic region. No significant modification of the τ2/τ1 observable for track-based jets in Pb--Pb collisions is observed relative to vacuum PYTHIA6 and PYTHIA8 references at the same collision energy. The measurements of τ2/τ1, together with the splitting aperture angle ΔR, are also performed in pp collisions at √s=7 TeV for inclusive jets. These results are compared with PYTHIA calculations at √s=7 TeV, in order to validate the model as a vacuum reference for the Pb−Pb centre-of-mass energy. The PYTHIA references for τ2/τ1 are shifted to larger values compared to the measurement in pp collisions. This hints at a reduction in the rate of two-pronged jets in Pb--Pb collisions compared to pp collisions.
The pT-differential production cross sections of prompt and non-prompt (produced in beauty-hadron decays) D mesons were measured by the ALICE experiment at midrapidity (|y|<0.5) in proton--proton collisions at s√=5.02 TeV. The data sample used in the analysis corresponds to an integrated luminosity of (19.3±0.4) nb−1. D mesons were reconstructed from their decays D0→K−π+, D+→K−π+π+, and D+s→ϕπ+→K−K+π+ and their charge conjugates. Compared to previous measurements in the same rapidity region, the cross sections of prompt D+ and D+s mesons have an extended pT coverage and total uncertainties reduced by a factor ranging from 1.05 to 1.6, depending on pT, allowing for a more precise determination of their pT-integrated cross sections. The results are well described by perturbative QCD calculations. The fragmentation fraction of heavy quarks to strange mesons divided by the one to non-strange mesons, fs/(fu+fd), is compatible for charm and beauty quarks and with previous measurements at different centre-of-mass energies and collision systems. The bb¯¯¯ production cross section per rapidity unit at midrapidity, estimated from non-prompt D-meson measurements, is dσbb¯¯¯/dy||y|<0.5=34.5±2.4(stat.)+4.7−2.9(tot.syst.) μb. It is compatible with previous measurements at the same centre-of-mass energy and with the cross section predicted by perturbative QCD calculations.
The pT-differential production cross sections of prompt and non-prompt (produced in beauty-hadron decays) D mesons were measured by the ALICE experiment at midrapidity (|y|<0.5) in proton--proton collisions at s√=5.02 TeV. The data sample used in the analysis corresponds to an integrated luminosity of (19.3±0.4) nb−1. D mesons were reconstructed from their decays D0→K−π+, D+→K−π+π+, and D+s→ϕπ+→K−K+π+ and their charge conjugates. Compared to previous measurements in the same rapidity region, the cross sections of prompt D+ and D+s mesons have an extended pT coverage and total uncertainties reduced by a factor ranging from 1.05 to 1.6, depending on pT, allowing for a more precise determination of their pT-integrated cross sections. The results are well described by perturbative QCD calculations. The fragmentation fraction of heavy quarks to strange mesons divided by the one to non-strange mesons, fs/(fu+fd), is compatible for charm and beauty quarks and with previous measurements at different centre-of-mass energies and collision systems. The bb¯¯¯ production cross section per rapidity unit at midrapidity, estimated from non-prompt D-meson measurements, is dσbb¯¯¯/dy||y|<0.5=34.5±2.4(stat.)+4.7−2.9(tot.syst.) μb. It is compatible with previous measurements at the same centre-of-mass energy and with the cross section predicted by perturbative QCD calculations.
The first evidence of spin alignment of vector mesons (K*0 and ϕ) in heavy-ion collisions at the Large Hadron Collider (LHC) is reported. The spin density matrix element ρ00 is measured at midrapidity (|y|< 0.5) in Pb-Pb collisions at a center-of-mass energy (√sNN) of 2.76 TeV
with the ALICE detector. ρ00 values are found to be less than 1/3 (1/3 implies no spin alignment) at low transverse momentum (pT<2 GeV/c) for K*0 and ϕ at a level of 3σ and 2σ, respectively. No significant spin alignment is observed for the K0S meson (spin = 0) in Pb-Pb collisions and for the vector mesons in pp collisions. The measured spin alignment is unexpectedly large but qualitatively consistent with the expectation from models which attribute it to a polarization of quarks in the presence of angular momentum in heavy-ion collisions and a subsequent hadronization by the process of recombination.
The transverse momentum (pT) differential yields of (anti-)3He and (anti-)3H measured in p-Pb collisions at sNN−−−√ = 5.02 TeV with ALICE at the Large Hadron Collider (LHC) are presented. The ratios of the pT-integrated yields of (anti-)3He and (anti-)3H to the proton yields are reported, as well as the pT dependence of the coalescence parameters B3 for (anti-)3He and (anti-)3H. For (anti-)3He, the results obtained in four classes of the mean charged-particle multiplicity density are also discussed. These results are compared to predictions from a canonical statistical hadronization model and coalescence approaches. An upper limit on the total yield of 4He¯ is determined.
Inclusive ψ(2S) production is measured in p-Pb collisions at the centre-of-mass energy per nucleon-nucleon pair sNN−−−√=8.16 TeV, using the ALICE detector at the CERN LHC. The production of ψ(2S) is studied at forward (2.03<ycms<3.53) and backward (−4.46<ycms<−2.96) centre-of-mass rapidity and for transverse momentum pT < 12 GeV/c via the decay to muon pairs. In this paper, we report the integrated as well as the ycms- and pT-differential inclusive production cross sections. Nuclear effects on ψ(2S) production are studied via the determination of the nuclear modification factor that shows a strong suppression at both forward and backward centre-of-mass rapidities. Comparisons with corresponding results for inclusive J/ψ show a similar suppression for the two states at forward rapidity (p-going direction), but a stronger suppression for ψ(2S) at backward rapidity (Pb-going direction). As a function of pT, no clear dependence of the nuclear modification factor is found. The relative size of nuclear effects on ψ(2S) production compared to J/ψ is also studied via the double ratio of production cross sections [σψ(2S)/σJ/ψ]pPb/[σψ(2S)/σJ/ψ]pp between p-Pb and pp collisions. The results are compared with theoretical models that include various effects related to the initial and final state of the collision system and also with previous measurements at sNN−−−√ = 5.02 TeV.
Coherent photoproduction of ρ⁰ vector mesons in ultra-peripheral Pb-Pb collisions at √sNN = 5.02 TeV
(2020)
Cross sections for the coherent photoproduction of ρ0 vector mesons in ultra-peripheral Pb-Pb collisions at sNN−−−√ = 5.02 TeV are reported. The measurements, which rely on the π+π− decay channel, are presented in three regions of rapidity covering the range |y| < 0.8. For each rapidity interval, cross sections are shown for different nuclear-breakup classes defined according to the presence of neutrons measured in the zero-degree calorimeters. The results are compared with predictions based on different models of nuclear shadowing. Finally, the observation of a coherently produced resonance-like structure with a mass around 1.7 GeV/c2 and a width of about 140 MeV/c2 is reported and compared with similar observations from other experiments.
Background: In intensive care units (ICU) octogenarians become a routine patients group with aggravated therapeutic and diagnostic decision-making. Due to increased mortality and a reduced quality of life in this high-risk population, medical decision-making a fortiori requires an optimum of risk stratification. Recently, the VIP-1 trial prospectively observed that the clinical frailty scale (CFS) performed well in ICU patients in overall-survival and short-term outcome prediction. However, it is known that healthcare systems differ in the 21 countries contributing to the VIP-1 trial. Hence, our main focus was to investigate whether the CFS is usable for risk stratification in octogenarians admitted to diversified and high tech German ICUs.
Methods: This multicentre prospective cohort study analyses very old patients admitted to 20 German ICUs as a sub-analysis of the VIP-1 trial. Three hundred and eight patients of 80 years of age or older admitted consecutively to participating ICUs. CFS, cause of admission, APACHE II, SAPS II and SOFA scores, use of ICU resources and ICU- and 30-day mortality were recorded. Multivariate logistic regression analysis was used to identify factors associated with 30-day mortality.
Results: Patients had a median age of 84 [IQR 82–87] years and a mean CFS of 4.75 (± 1.6 standard-deviation) points. More than half of the patients (53.6%) were classified as frail (CFS ≥ 5). ICU-mortality was 17.3% and 30-day mortality was 31.2%. The cause of admission (planned vs. unplanned), (OR 5.74) and the CFS (OR 1.44 per point increase) were independent predictors of 30-day survival.
Conclusions: The CFS is an easy determinable valuable tool for prediction of 30-day ICU survival in octogenarians, thus, it may facilitate decision-making for intensive care givers in Germany.
Trial registration: The VIP-1 study was retrospectively registered on ClinicalTrials.gov (ID: NCT03134807) on May 1, 2017.
Im Zeitraum 1999 bis 2003 wurden im Harz 83 gezüchtete Auerhühner besendert und nach der Auswilderung telemetrisch überwacht. Das Hauptziel war dabei, über Daten zu Überlebenschancen, Raum- und Habitatnutzung und zur Ernährung der Auswilderungstiere eine effektive Erfolgskontrolle zu ermöglichen und Optimierungsvorschläge für zukünftige Auswilderungsbestrebungen geben zu können. Von den mit Sendern ausgestatteten Tieren überlebten ca. 23 % (n = 18) bis zum Sender- oder Kontaktverlust. Die mediane Überlebensdauer betrug 13 Tage, wobei Hennen länger überlebten (18 Tage) als Hähne (12 Tage). Die höchsten Verluste (79 %, n = 48) traten innerhalb der ersten vier Wochen nach der Ausbringung auf. Von 61 registrierten Totfunden entfielen 62 % auf den Fuchs, 10 % auf den Habicht und 7 % auf den Luchs. Neben Totfunden mit unklarer Ursache, verendeten einzelne Tiere im Verkehr, aufgrund von Unterernährung oder wurden von Hunden getötet. Die Hauptgründe für die hohen Verluste unter den ausgewilderten Auerhühnern sind in physiologischen und ethologischen Defiziten aufgrund der Gehegezucht zu suchen. Hier seien insbesondere mangelhafte Feindkenntnis, und die wahrscheinlich unzureichende Anpassung an die Freilandnahrung zu nennen. Zudem waren 5 % der Verluste auf angelockte Prädatoren im Umfeld der Eingewöhnungsvoliere zurückzuführen. Die Auswilderungstiere nutzten Aktionsräume (Suchgebiete) zwischen unter einem bis zu 17.100 ha, wobei die Mehrzahl der Aktionsräume (77 %) bis zu 1.000 ha umfasste. Die ermittelten Aktionsraumgröße und auch die maximale Entfernung zum Auswilderungsort nahmen mit der Ortungsdauer zu. Das mitunter weiträumige Verstreichen der Auswilderungstiere könnte auf die allgemein starke Dispersion juveniler Auerhühner, aber auch auf vom Habitat her ungeeignete Auswilderungsorte zurückzuführen sein. Innerhalb der Aktionsräume etablierten die Vögel räumlich kleinere Nutzungszentren die zumeist bis zum Totfund oder Senderverlust frequentiert blieben. Die Größe der Nutzungszentren (n = 17) variierte zwischen 0,5 ha und bis zu 327 ha. Täglich legten die Vögel in ca. 70 % aller Fälle nicht mehr als 500 m zurück. Etwa 67 % aller Ortungen entfielen auf einen 3-km-Radius um den Aussetzungsort. Maximalwerte verwiesen auf Distanzen bis ca. 22 km (W). Methodisch ist aufgrund der Ergebnisse die Auswilderung direkt aus den Transportkisten ohne Akklimatisierung in Eingewöhnungsvolieren zu empfehlen. So ließen sich zusätzliche Verluste am Auswilderungspunkt vermeiden, und zudem bliebe man flexibel in der Wahl des Auswilderungsortes. Weitere Optimierungsmaßnahmen in der Zucht und Auswilderungsmethodik sind unerlässlich (z. B. frühzeitig intensivierte artgerechte Ernährung, Trainingsprogramme, angemessene Krankheitsprophylaxe), ohne deren erfolgreiche Umsetzung die weitere Auswilderung von Gehegetieren nicht weiter verantwortbar bleibt.
Von 1999 bis 2003 kamen im Nationalpark Harz (Niedersachsen) 83 gezüchtete juvenile Auerhühner frei, die zuvor mit Sendern ausgestattet und anschließend regelmäßig geortet wurden. Es wurde geprüft, ob die ausgewilderten Auerhühner ein ähnliches Nahrungsspektrum haben wie Wildvögel. Der Hintergrund dabei sind Erkenntnisse darüber, dass gezüchtete Hühnervögel aufgrund der hochverdaulichen und nährstoffreichen Volierennahrung ernährungsphysiologisch schlecht auf ein Leben im Freiland vorbereitet sind. Es wurden 109 Losungsproben gesammelt und die darin enthaltenen Nahrungsreste mikroskopisch aufbereitet, mit Hilfe einer Vergleichssammlung und der arttypischen Epidermiskennzeichen bestimmt und ihre Anteile geschätzt. Als Hauptnahrungskomponenten der im Herbst ausgewilderten Auerhühner sind für die Monate Oktober bis Februar Fichte (34 %), Heidelbeere (26 %) und Kräuter (20 %) zu nennen. Bei den im Frühjahr frei gelassenen Vögeln dominierten Fichte (56 %) und Gräser (20 %). Der Koniferenanteil bleibt jedoch in den Herbst- und insbesondere in den Wintermonaten hinter den Erwartungen zurück, besteht doch die Ernährung wild lebender Auerhühner im Winter nahezu ausschließlich aus Nadeln. Betrachtet man die drei Auswilderungstermine im Herbst (1999, 2002 und 2003) separat, fällt auf, dass der Fichtenanteil in den Monaten Dezember bis Februar mit minimal 18 % bis maximal 64 % auf äußerst niedrigem Niveau schwankt. Eine Umstellung auf die Winternadelnahrung, wie sie bei Wildvögeln bereits in den Herbstmonaten erfolgt, konnte nur anhand von Einzelproben nachgewiesen werden und verlief deutlich zeitversetzt (Februar). Günstige Witterungsbedingungen bis weit in die Wintermonate hinein (Verfügbarkeit der Krautschicht als Nahrungsquelle) und ernährungsphysiologische Defizite (geringe Verdauungsleistung) werden als Ursachen dafür diskutiert. Da das Hauptziel von solchen Artenschutzprogrammen die Ausbringung überlebensfähiger Individuen sein muss, ist zukünftig verstärkt darauf zu achten, dass die dafür notwendigen Grundlagen garantiert sind. Eine Voraussetzung dabei ist die Entwicklung umsetzbarer Fütterungsprogramme für Auswilderungszuchten und deren erfolgreiche Etablierung. Gelingen diese nicht, ist der weitere Einsatz von Zuchtvögeln für Ansiedlungsprojekte nicht zu befürworten.