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The polarization of Λ and Λ¯ hyperons along the beam direction has been measured relative to the second and third harmonic event planes in isobar Ru+Ru and Zr+Zr collisions at √sNN = 200 GeV. This is the first experimental evidence of the hyperon polarization by the triangular flow originating from the initial density fluctuations. The amplitudes of the sine modulation for the second and third harmonic results are comparable in magnitude, increase from central to peripheral collisions, and show a mild pT dependence. The azimuthal angle dependence of the polarization follows the vorticity pattern expected due to elliptic and triangular anisotropic flow, and qualitatively disagree with most hydrodynamic model calculations based on thermal vorticity and shear induced contributions. The model results based on one of existing implementations of the shear contribution lead to a correct azimuthal angle dependence, but predict centrality and pT dependence that still disagree with experimental measurements. Thus, our results provide stringent constraints on the thermal vorticity and shear-induced contributions to hyperon polarization. Comparison to previous measurements at RHIC and the LHC for the second-order harmonic results shows little dependence on the collision system size and collision energy.
Four new species of the genus Catonidia Uhler, 1896, C. triangula sp. nov., C. saccata sp. nov., C. trilobata sp. nov. and C. uncinata sp. nov. from China (Fujian, Guizhou, Yunnan and Hainan provinces), are described and illustrated, giving the genus 14 species in total. A checklist and key to all known species of Catonidia are provided, as well as a map of their geographic distributions.
By analyzing the large-angle Bhabha scattering events e+e− → (γ)e+e− and diphoton events e+e− → (γ)γγ for the data sets collected at center-of-mass (c.m.) energies between 2.2324 and 4.5900 GeV (131 energy points in total) with the upgraded Beijing Spectrometer (BESIII) at the Beijing Electron-Positron Collider (BEPCII), the integrated luminosities have been measured at the different c.m. energies, individually. The results are important inputs for the R value and J/ψ resonance parameter measurements.
Based on an e+e− collision data sample corresponding to an integrated luminosity of 2.93 fb−1 collected with the BESIII detector at √s=3.773 GeV, the first amplitude analysis of the singly Cabibbo-suppressed decay D+→K+K0Sπ0 is performed. From the amplitude analysis, the K∗(892)+K0S component is found to be dominant with a fraction of (57.1±2.6±4.2)%, where the first uncertainty is statistical and the second systematic. In combination with the absolute branching fraction B(D+→K+K0Sπ0) measured by BESIII, we obtain B(D+→K∗(892)+K0S)=(8.69±0.40±0.64±0.51)×10−3, where the third uncertainty is due to the branching fraction B(D+→K+K0Sπ0). The precision of this result is significantly improved compared to the previous measurement. This result also differs from most of theoretical predictions by about 4σ, which may help to improve the understanding of the dynamics behind.
Fungi belonging to the Rhytismatales (Ascomycota) are parasites or endophytes of plants, some are saprophytes. Their fruiting bodies are localized in different organs of the host plants belonging to many different families of gymnosperms and angiosperms. Many species of Rhytismatales are known on species of Pinaceae, Ericaceae, and Poaceae. These fungi usually have ascomata that are more or less embedded in host tissue and open by longitudinal or radial splits. They have a more or less carbonized covering stroma, thin-walled, iodine negative asci, and ascospores usually covered by gelatinous sheaths.
In the present study, two lists of species of Rhytismatales in China are presented. One is based on literature and includes 103 species in 15 genera. The second one contains the names of the species in the present study, 57 species in 20 genera based on 90 specimens I collected in the Yunnan and Anhui province in China during July to August in 2001. 31 species in the second list are new species or new records for China, so we presently know 134 species in 22 genera of Rhytismatales for China. 28 new species of Rhytismatales are proposed, 21 species from the Yunnan province and seven from the Anhui province. Among them, three new species are proposed in three new genera, Nematococcomyces, New Genus 1, and New Genus 2, respectively. The 28 new species are Cerion sp., Coccomyces spp. 1-2, Colpoma spp. 1-2, Hypoderma spp. 1-6, Lirula sp., Lophodermella sp., Lophodermium spp. 1-5, Nematococcomyces rhododendri C.-L. Hou, M. Piepenbr. & Oberw., Neococcomyces sp., New Genus 1 sp., New Genus 2 sp., Rhytisma spp. 1-2, Soleella sp., Terriera spp. 1-2, and Therrya sp. The genus Davisomycella is proposed as a synonym of Lophodermella based on observations of the morphology, ecology, and the infected organ. The four genera Cerion, Naemacyclus, Terriera, and Therrya, and three species, Hypoderma rubi, Lophodermium uncinatum, and Naemacyclus pinastri, are reported for the first time for China. All the new taxa, the newly recorded ones, as well as six species which had not been illustrated in detail before, are carefully described and illustrated by line drawings in the present study.
The results show that species of Rhytismatales are highly diverse especially in the natural vegetation in high mountainous areas in China. Most species of Rhytismatales are conspicuously host specific. The diversity of Rhytismatales is closely related to that of the preferred hosts, which are members of Pinaceae, Ericaceae, and Cupressaceae. Based on the detailed morphological observations, the significance of different morphological characteristics for a natural classification of Rhytismatales is discussed. Genera are traditionally defined by character states of a few characteristics, namely the opening patterns of ascomata, the depth of ascomata in the host tissue, and asci and ascospore shape. Data from collections in the field, detailed morphological investigation, and molecular data show, however, that the ecology, the infected organ, the host relationship, and many other characteristics have to be combined to circumscribe natural groups.
The discussion of the systematic significance of morphological characteristics is complemented by molecular data. In the present study, partial nuclear large subunit rDNA sequences of 52 specimens representing 38 species are used to analyse phylogenetic relationships for members of Rhytismatales.
Most species of Rhytismatales are placed in a monophyletic group corresponding to the Rhytismatales in the Maximum Parsimony analysis. The delimitation of the Rhytismatales from the Helotiales is, however, difficult. Cyclaneusma minus should be transferred from the Rhytismatales to the Helotiales, and Cudonia circinans and Spathularia flavida from the Helotiales to the Rhytismatales. These tranfers have previously been proposed based on SSU rDNA analysis by other authors. New Genus 1 sp. has morphological characteristics typical for species of Rhytismatales. In the LSU rDNA analysis, however, it is more closely related to Helotiales rather than toRhytismatales. Therefore New Genus 1 sp. is placed in the Helotiales.
Tryblidiopsis pinastri is morphologically intermediate between members of Rhytismataceae and Cudoniaceae. LSU rDNA sequences in the present study show that T. pinastri is more closely related to species of Cudoniaceae. Therefore, this species is removed from the Rhytismataceae to the Cudoniaceae. The delimitation of further families could not be resolved in the present analysis.
Though many new morphological, ecological, and molecular phylogenetic findings are contributed for the first time, the systematic conclusions at generic, family, and order level can only be fragmentary in the present study. With more collections and more molecular data of the worldwide 450 known and many more unknown species of Rhytismatales at hand, a natural system combining morphological and molecular analysis can be elaborated.
Using 2.93 fb−1 of 𝑒+𝑒− collision data taken at a center-of-mass energy of 3.773 GeV with the BESIII detector, we report the first measurements of the absolute branching fractions of 14 hadronic 𝐷0(+) decays to exclusive final states with an 𝜂, e.g., 𝐷0→𝐾−𝜋+𝜂, 𝐾0𝑆𝜋0𝜂, 𝐾+𝐾−𝜂, 𝐾0𝑆𝐾0𝑆𝜂, 𝐾−𝜋+𝜋0𝜂, 𝐾0𝑆𝜋+𝜋−𝜂, 𝐾0𝑆𝜋0𝜋0𝜂, and 𝜋+𝜋−𝜋0𝜂; 𝐷+→𝐾0𝑆𝜋+𝜂, 𝐾0𝑆𝐾+𝜂, 𝐾−𝜋+𝜋+𝜂, 𝐾0𝑆𝜋+𝜋0𝜂, 𝜋+𝜋+𝜋−𝜂, and 𝜋+𝜋0𝜋0𝜂. Among these decays, the 𝐷0→𝐾−𝜋+𝜂 and 𝐷+→𝐾0 𝑆𝜋+𝜂 decays have the largest branching fractions, which are ℬ(𝐷0→𝐾−𝜋+𝜂) = (1.853±0.025stat±0.031syst)% and ℬ(𝐷+→𝐾0𝑆𝜋+𝜂) = (1.309±0.037stat±0.031syst)%, respectively. The charge-parity asymmetries for the six decays with highest event yields are determined, and no statistically significant charge-parity violation is found.
An amplitude analysis of the 𝐾𝑆𝐾𝑆 system produced in radiative 𝐽/𝜓 decays is performed using the (1310.6±7.0)×106 𝐽/𝜓 decays collected by the BESIII detector. Two approaches are presented. A mass-dependent analysis is performed by parametrizing the 𝐾𝑆𝐾𝑆 invariant mass spectrum as a sum of Breit-Wigner line shapes. Additionally, a mass-independent analysis is performed to extract a piecewise function that describes the dynamics of the 𝐾𝑆𝐾𝑆 system while making minimal assumptions about the properties and number of poles in the amplitude. The dominant amplitudes in the mass-dependent analysis include the 𝑓0(1710), 𝑓0(2200), and 𝑓′2(1525). The mass-independent results, which are made available as input for further studies, are consistent with those of the mass-dependent analysis and are useful for a systematic study of hadronic interactions. The branching fraction of radiative 𝐽/𝜓 decays to 𝐾𝑆𝐾𝑆 is measured to be (8.1±0.4)×10−4, where the uncertainty is systematic and the statistical uncertainty is negligible.
Using a data sample of 𝑒+𝑒− collisions corresponding to an integrated luminosity of 567 pb−1 collected at a center-of-mass energy of √𝑠=4.6 GeV with the BESIII detector, we measure the absolute branching fraction of the inclusive semileptonic Λ+𝑐 decay with a double-tag method. We obtain ℬ(Λ+𝑐→𝑋𝑒+𝜈𝑒)=(3.95±0.34±0.09)%, where the first uncertainty is statistical and the second systematic. Using the known Λ+𝑐 lifetime and the charge-averaged semileptonic decay width of nonstrange charmed mesons (𝐷0 and 𝐷+), we obtain the ratio of the inclusive semileptonic decay widths Γ(Λ+𝑐→𝑋𝑒+𝜈𝑒)/¯Γ(𝐷→𝑋𝑒+𝜈𝑒)=1.26±0.12.
Elliptic flow of heavy-flavor decay electrons in Au+Au collisions at √sNN = 27 and 54.4 GeV at RHIC
(2023)
We report on new measurements of elliptic flow (v2) of electrons from heavy-flavor hadron decays at mid-rapidity (|y|<0.8) in Au+Au collisions at sNN−−−√ = 27 and 54.4 GeV from the STAR experiment. Heavy-flavor decay electrons (eHF) in Au+Au collisions at sNN−−−√ = 54.4 GeV exhibit a non-zero v2 in the transverse momentum (pT) region of pT< 2 GeV/c with the magnitude comparable to that at sNN−−−√=200 GeV. The measured eHF v2 at 54.4 GeV is also consistent with the expectation of their parent charm hadron v2 following number-of-constituent-quark scaling as other light and strange flavor hadrons at this energy. These suggest that charm quarks gain significant collectivity through the evolution of the QCD medium and may reach local thermal equilibrium in Au+Au collisions at sNN−−−√=54.4 GeV. The measured eHF v2 in Au+Au collisions at sNN−−−√= 27 GeV is consistent with zero within large uncertainties. The energy dependence of v2 for different flavor particles (π,ϕ,D0/eHF) shows an indication of quark mass hierarchy in reaching thermalization in high-energy nuclear collisions.
Elliptic flow of heavy-flavor decay electrons in Au+Au collisions at √sNN = 27 and 54.4 GeV at RHIC
(2023)
We report on new measurements of elliptic flow (v2) of electrons from heavy-flavor hadron decays at mid-rapidity (|y|<0.8) in Au+Au collisions at sNN−−−√ = 27 and 54.4 GeV from the STAR experiment. Heavy-flavor decay electrons (eHF) in Au+Au collisions at sNN−−−√ = 54.4 GeV exhibit a non-zero v2 in the transverse momentum (pT) region of pT< 2 GeV/c with the magnitude comparable to that at sNN−−−√=200 GeV. The measured eHF v2 at 54.4 GeV is also consistent with the expectation of their parent charm hadron v2 following number-of-constituent-quark scaling as other light and strange flavor hadrons at this energy. These suggest that charm quarks gain significant collectivity through the evolution of the QCD medium and may reach local thermal equilibrium in Au+Au collisions at sNN−−−√=54.4 GeV. The measured eHF v2 in Au+Au collisions at sNN−−−√= 27 GeV is consistent with zero within large uncertainties. The energy dependence of v2 for different flavor particles (π,ϕ,D0/eHF) shows an indication of quark mass hierarchy in reaching thermalization in high-energy nuclear collisions.