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Noneequilibrium models (three-fluid hydrodynamics and UrQMD) use to discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions. It is demonstrated that these two models - although they do treat the most interesting early phase of the collisions quite differently(thermalizing QGP vs. coherent color fields with virtual particles) - both yields a reasonable agreement with a large variety of the available heavy ion data.
Rubus raduloides (ROG.) SUDRE, eine bislang nur von England, Wales und Schottland bekannte Brombeerart, ist ebenso auf dem Kontinent (in den Niederlanden, Belgien und in der Bundesrepublik Deutschland) weit verbreitet, doch hier bisher verkannt und mit anderen Arten verwechselt. Nomenklatorische Fragen, die Verbreitung und Ökologie werden behandelt, und darüber hinaus wird eine detaillierte Beschreibung mit Abbildungen dieser auch in Großbritannien oft falsch interpretierten Art gegeben, um weitere Fehldeutungen zukünftig zu verhindern.
Das Pruno-Rubetum elegantispinosi (Pruno-Rubetalia) wird als neue Gebüschgesellschaft auf kalkreicheren Böden in Hecken Niedersachsens und Westfalens beschrieben. Darüber hinaus wird die Syntaxonomie der Rhamno-Prunetea behandelt. Es wird gezeigt, daß die Rubi (Pseudo-Phanerophyta) mit ihren nur zweijährigen Schößlingen nicht in der Lage sind, sich in geschlossenen, von echten ausdauernden Sträuchern (Nano- Phanerophyta) gebildeten Gebüschen zu behaupten und daher nur als charakteristischer «ubus-Mantel dieser echten Prunetalia-Gebüsche auftreten, wo sie als eine Art "Klammergesellschaft" sowohl die echten Prunetalia wie auch die vorgelagerten Säume (Trifolio- Geranieta, Alliarietalia) zum Teil miteinander verbinden. Im Interesse einer saubereren nyntaxonomischen Fassung der (subatlantischen) Rhamno-Prunetea sind daher (besonders an breiteren Hecken und in ausgedehnteren Gebüschen) innere brombeer- und weitgehend auch krautfreie Bereiche (Prunetalia s.str.) von den äußeren Pruno-Rubetalia zu unters::: heiden, die die Mantelzone der Prunetalia s. str. darstellen, oder auch insgesamt durch schmale Hecken, Waldmänteloder durch noch offene Ptoruerstad.en der Prunetalia s. str. repräsentiert werden können.
Die in Europa vorkommenden Sommergrünen Brombeeren (Rubus subgenus Rubus sectio Rubus subsectio Rubus) werden in vier Serien untergliedert: Series Nessenses H. E. Weber ser. nov. (Typus: Rubus nessensis Hall), Series Rubus ser. nov. (Typus: Rubus fruticosus L. = R. plicatus Weihe & Nees), Series Canadenses (L.H. Bailey) H. E.Weber ser. nov. (Typus: Rubus canadensis L.) und Series Alleghenienses (L. H. Bailey) H. E. Weber ser. nov. (Typus: Rubus allegheniensis Porter). Die Series Rubus wird in zwei Subserien unterteilt: Subseries Rubus (Typus: Rubus fruticosus L.) subser. nov. und Subseries Subrhamnifolii (Focke) H. E. Weber subser. nov. (Typus: Rubus montanus Wirtgen = R. senticosus Koehler ex Weihe). Die Taxonomie und Nomenklatur dieser infragenerischen Taxa sind behandelt.
The cell—cell signaling gene CDH13 is associated with a wide spectrum of neuropsychiatric disorders, including attention-deficit/hyperactivity disorder (ADHD), autism, and major depression. CDH13 regulates axonal outgrowth and synapse formation, substantiating its relevance for neurodevelopmental processes. Several studies support the influence of CDH13 on personality traits, behavior, and executive functions. However, evidence for functional effects of common gene variation in the CDH13 gene in humans is sparse. Therefore, we tested for association of a functional intronic CDH13 SNP rs2199430 with ADHD in a sample of 998 adult patients and 884 healthy controls. The Big Five personality traits were assessed by the NEO-PI-R questionnaire. Assuming that altered neural correlates of working memory and cognitive response inhibition show genotype-dependent alterations, task performance and electroencephalographic event-related potentials were measured by n-back and continuous performance (Go/NoGo) tasks. The rs2199430 genotype was not associated with adult ADHD on the categorical diagnosis level. However, rs2199430 was significantly associated with agreeableness, with minor G allele homozygotes scoring lower than A allele carriers. Whereas task performance was not affected by genotype, a significant heterosis effect limited to the ADHD group was identified for the n-back task. Heterozygotes (AG) exhibited significantly higher N200 amplitudes during both the 1-back and 2-back condition in the central electrode position Cz. Consequently, the common genetic variation of CDH13 is associated with personality traits and impacts neural processing during working memory tasks. Thus, CDH13 might contribute to symptomatic core dysfunctions of social and cognitive impairment in ADHD.
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.
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.
J/ψ production as a function of charged-particle multiplicity in p–Pb
collisions at √sNN = 8.16 TeV
(2021)
Inclusive J/ψ yields and average transverse momenta in p-Pb collisions at a center-of-mass energy per nucleon pair sNN−−−√ = 8.16 TeV are measured as a function of the charged-particle pseudorapidity density with ALICE. The J/ψ mesons are reconstructed at forward (2.03<ycms<3.53) and backward (−4.46<ycms<−2.96) center-of-mass rapidity in their dimuon decay channel while the charged-particle pseudorapidity density is measured around midrapidity. The J/ψ yields at forward and backward rapidity normalized to their respective average values increase with the normalized charged-particle pseudorapidity density, the former showing a weaker increase than the latter. The normalized average transverse momenta at forward and backward rapidity manifest a steady increase from low to high charged-particle pseudorapidity density with a saturation beyond the average value.