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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.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at sNN−−−√ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the ν in the 0-5\% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a possible minimum around sNN−−−√ = 27 GeV. The physics implications on the QCD phase structure are discussed.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at sNN−−−√ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the ν in the 0-5\% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a possible minimum around sNN−−−√ = 27 GeV. The physics implications on the QCD phase structure are discussed.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at √sNN = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40%) collisions. Moreover, the ν in the 0-5% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around √sNN = 27 GeV. The physics implications on the QCD phase structure are discussed.
Observation of directed flow of hypernuclei Λ³H and Λ⁴H in √sNN = 3 GeV Au+Au collisions at RHIC
(2023)
We report here the first observation of directed flow (v1) of the hypernuclei 3ΛH and 4ΛH in mid-central Au+Au collisions at sNN−−−√ = 3 GeV at RHIC. These data are taken as part of the beam energy scan program carried out by the STAR experiment. From 165 × 106 events in 5%-40% centrality, about 8400 3ΛH and 5200 4ΛH candidates are reconstructed through two- and three-body decay channels. We observe that these hypernuclei exhibit significant directed flow. Comparing to that of light nuclei, it is found that the midrapidity v1 slopes of 3ΛH and 4ΛH follow baryon number scaling, implying that the coalescence is the dominant mechanism for these hypernuclei production in such collisions.
The linear and mode-coupled contributions to higher-order anisotropic flow are presented for Au+Au collisions at √sN N = 27, 39, 54.4, and 200 GeV and compared to similar measurements for Pb+Pb collisions at the Large Hadron Collider (LHC). The coefficients and the flow harmonics’ correlations, which characterize the linear and mode-coupled response to the lower-order anisotropies, indicate a beam energy dependence consistent with an influence from the specific shear viscosity (η/s). In contrast, the dimensionless coefficients, mode-coupled response coefficients, and normalized symmetric cumulants are approximately beam-energy independent, consistent with a significant role from initialstate effects. These measurements could provide unique supplemental constraints to (i) distinguish between different initial-state models and (ii) delineate the temperature (T ) and baryon chemical potential (μB ) dependence of the specific shear viscosity η s (T ,μB ).
The linear and mode-coupled contributions to higher-order anisotropic flow are presented for Au+Au collisions at sNN−−−√ = 27, 39, 54.4, and 200 GeV and compared to similar measurements for Pb+Pb collisions at the Large Hadron Collider (LHC). The coefficients and the flow harmonics' correlations, which characterize the linear and mode-coupled response to the lower-order anisotropies, indicate a beam energy dependence consistent with an influence from the specific shear viscosity (η/s). In contrast, the dimensionless coefficients, mode-coupled response coefficients, and normalized symmetric cumulants are approximately beam-energy independent, consistent with a significant role from initial-state effects. These measurements could provide unique supplemental constraints to (i) distinguish between different initial-state models and (ii) delineate the temperature (T) and baryon chemical potential (μB) dependence of the specific shear viscosity ηs(T,μB).
Cortical tracking of stimulus features (such as the envelope) is a crucial tractable neural mechanism, allowing us to investigate how we process continuous music. We here tested whether cortical and behavioural tracking of beat, typically related to rhythm processing, are modulated by pitch predictability. In two experiments (n=20, n=52), participants’ ability to tap along to the beat of musical sequences was measured for tonal (high pitch predictability) and atonal (low pitch predictability) music. In Experiment 1, we additionally measured participants’ EEG and analysed cortical tracking of the acoustic envelope and of pitch surprisal (using IDyOM). In both experiments, finger-tapping performance was better in the tonal than the atonal condition, indicating a positive effect of pitch predictability on behavioural rhythm processing. Neural data revealed that the acoustic envelope was tracked stronger while listening to atonal than tonal music, potentially reflecting listeners’ violated pitch expectations. Our findings show that cortical envelope tracking, beyond reflecting musical rhythm processing, is modulated by pitch predictability (as well as musical expertise and enjoyment). Stronger cortical surprisal tracking was linked to overall worse envelope tracking, and worse finger-tapping performance for atonal music. Specifically, the low pitch predictability in atonal music seems to draw attentional resources resulting in a reduced ability to follow the rhythm behaviourally. Overall, cortical envelope and surprisal tracking were differentially related to behaviour in tonal and atonal music, likely reflecting differential processing under conditions of high and low predictability. Taken together, our results show diverse effects of pitch predictability on musical rhythm processing.
A new, more precise measurement of the Λ hyperon lifetime is performed using a large data sample of Pb–Pb collisions at √sNN p ¼ 5.02 TeV with ALICE. The Λ and Λ¯ hyperons are reconstructed at midrapidity using their two-body weak decay channel Λ → p þ π− and Λ¯ → p¯ þ πþ. The measured value of the Λ lifetime is τΛ ¼ ½261.07 0.37ðstat:Þ 0.72ðsyst:Þ ps. The relative difference between the lifetime of Λ and Λ¯ , which represents an important test of CPT invariance in the strangeness sector, is also measured. The obtained value ðτΛ − τΛ¯Þ=τΛ ¼ 0.0013 0.0028ðstat:Þ 0.0021ðsyst:Þ is consistent with zero within the uncertainties. Both measurements of the Λ hyperon lifetime and of the relative difference between τΛ and τΛ¯ are in agreement with the corresponding world averages of the Particle Data Group and about a factor of three more precise.
First measurement of Λ+c production down to pT = 0 in pp and p-Pb collisions at √𝑠NN = 5.02 TeV
(2023)
The production of prompt +c baryons has been measured at midrapidity in the transverse momentum interval 0 < pT < 1 GeV/c for the first time, in pp and p–Pb collisions at a center-of-mass energy per nucleon-nucleon collision √sNN = 5.02 TeV. The measurement was performed in the decay channel +c → pK0S by applying new decay reconstruction techniques using a Kalman-Filter vertexing algorithm and adopting a machine-learning approach for the candidate selection. The pT -integrated +c production cross sections in both collision systems were determined and used along with the measured yields in Pb–Pb collisions to compute the pT -integrated nuclear modification factors RpPb and RAA of +c baryons, which are compared to model calculations that consider nuclear modification of the parton distribution functions. The +c /D0 baryon-to-meson yield ratio is reported for pp and p–Pb collisions. Comparisons with models that include modified hadronization processes are presented, and the implications of the results on the understanding of charm hadronization in hadronic collisions are discussed. A significant (3.7σ) modification of the mean transverse momentum of + c baryons is seen in p–Pb collisions with respect to pp collisions, while the pT -integrated +c /D0 yield ratio was found to be consistent between the two collision systems within the uncertainties.
This thesis investigates the structure of the translocase of the outer membrane (TOM) complex in mitochondria, focusing on the TOM holo complex through single-particle electron cryo-microscopy (cryoEM) complemented by mass spectrometry and computational structure prediction. Mitochondria, crucial for energy production in eukaryotic cells, import most of their proteins from the cytoplasm. These proteins enter through the TOM complex, which in its core form consists of a membrane-embedded homodimer of Tom40 pores, two Tom22 cytoplasmic receptors, and six small TOM stabilizing subunits (Tom7, Tom6, and Tom5). The holo complex includes two additional subunits, Tom70 and Tom20, whose stoichiometry and positioning are less understood due to their easy dissociation during isolation of the complex. CryoEM analysis revealed the high-resolution structure of the Neurospora crassa TOM core complex at 3.3 Å, containing all core subunits, and the presence of a central phospholipid causing the Tom40 dimer to tilt to 20°. Furthermore, a 4 Å resolution map indicated the binding of a precursor protein as it transitions through the translocation barrel. Finally, at 6-7 Å resolution, the structure of the TOM holo complex highlighted Tom20's flexibility as it interacts with the core complex, emphasizing its role in protein translocation. This work provides significant insights into the architecture and functioning of the TOM complex, contributing to the understanding of mitochondrial protein import mechanisms.
Mitochondria perform essential energetic, metabolic and signalling functions within the cell. To fulfil these, the integrity of the mitochondrial proteome has to be preserved. Therefore, each mitochondrial subcompartment harbours its own system for protein quality control. However, if the capacity of mitochondrial chaperones and proteases is overloaded, mitochondrial misfolding stress (MMS) occurs. Upon this stress condition, mitochondria communicate with the nucleus to increase the transcription of nuclear encoded mitochondrial chaperones and proteases. This proteotoxic stress pathway was termed the mitochondrial unfolded protein response (UPRmt) aiming at restoring protein homeostasis. Despite being discovered over 25 years ago, the signalling molecules released by stressed mitochondria as well as the corresponding receptor and transcription factor remain poorly understood. With this study, we aimed at characterising the underlying signalling events and mechanisms of how mitochondria react to misfolded proteins. First, we aimed to establish different methods to induce MMS that triggers the transcriptional induction of mitochondrial chaperones and proteases detected by quantitative polymerase chain reaction. We were able to induce UPRmt signalling by overexpression of an aggregation-prone protein and by knock-down or inhibition of mitochondrial protein quality control components. To study the signalling in a time-resolved manner, we focused on the usage of the mitochondrial HSP90 inhibitor GTPP and the mitochondrial LONP1 protease inhibitor CDDO.
Early time point RNA sequencing analysis of cells stressed with GTPP or CDDO revealed upregulated genes in response to oxidative stress. Indeed, measurements of mitochondrial superoxide with the fluorescent dye MitoSOX showed increased levels of reactive oxygen species (ROS) upon MMS induction. In contrast, there was no induction of mitochondrial chaperones and proteases when combining MMS with antioxidants. Compartment-specific targeting of the hydrogen peroxide sensor HyPer7 revealed increased ROS levels in the intermembrane space and matrix of mitochondria, followed by elevated ROS levels in the cytosol at later time points. The importance of cytosolic ROS for the signalling was supported by preventing UPRmt induction with an inhibitor blocking the outer mitochondrial membrane pore. Thus, ROS were identified as an essential UPRmt signal.
To understand which cytosolic factor is modified by ROS, redox proteomics was performed. Here, reversible changes on cysteine residues of the HSP40 co-chaperone DNAJA1 were observed upon MMS. Consequently, transcriptional induction of UPRmt genes was abolished by DNAJA1 knock-down. To understand the function of DNAJA1 during UPRmt signalling, quantitative interaction proteomics upon MMS revealed an increased binding to mitochondrial proteins and its interaction partner HSP70. Immunoprecipitation confirmed a ROS-dependent interaction between HSP40 and HSP70. Increased binding to mitochondrial proteins represented a cytosolic interaction of DNAJA1 with mitochondrial precursor proteins, whose accumulation was confirmed by western blot. Moreover, a fluorescent protein targeted to mitochondria accumulated in the cytosol during GTPP treatment, confirming a reduced import efficiency upon MMS. Preventing the accumulation of precursors by a translation inhibitor or depletion of a general mitochondrial transcription factor resulted in reduced UPRmt activation. Thus, DNAJA1 is essential for UPRmt signalling, since its oxidation by mitochondrial ROS and its enhanced recruitment to mitochondrial precursors allows the integration of both MMS-induced signals.
To link these findings to an increased transcription of mitochondrial chaperones and proteases, we screened for transcription factors accumulating in the nucleus upon MMS by cellular fractionation mass spectrometry. We demonstrated that specifically HSF1 accumulates in nuclei of cells stressed with GTPP or CDDO. Depletion of HSF1 by knock-down or knock-out resulted in the abrogation of the UPRmt-specific transcriptional response. HSF1 activation was visualised by nuclear accumulation on western blot, a process inhibited by ROS and precursor suppression. Moreover, DNAJA1 depletion prevented HSF1 activation. Ultimately, we proved by immunoprecipitation that the inhibitory interaction between HSF1 and HSP70 is reduced upon MMS.
Thus, we conclude that MMS increases mitochondrial ROS that are released into the cytosol. In addition, the import efficiency is reduced upon MMS, resulting in the accumulation of non-imported mitochondrial precursor proteins in the cytosol. Both signals are recognised via DNAJA1 oxidation and substrate binding. The concurrent recruitment of HSP70 to DNAJA1 results in the loss of the inhibitory HSP70-HSF1 interaction. Thus, active HSF1 can migrate to the nucleus to initiate transcription of mitochondrial chaperones and proteases. These findings are in accordance with observations in yeast, where mistargeted mitochondrial proteins activate cellular stress responses. Our results highlight a surprising interconnection and dependence of the mitochondrial and the cytosolic proteostasis network, in which the UPRmt is activated by a combination of two mitochondria-specific proteotoxic stress signals.
The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at √sNN = 5.02 TeV is presented in this article. The measurements are carried out at midrapidity (y|< 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different center-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.
Diese Versuchsreihe beschäftigte sich mit der Fragestellung, ob günstige Handelsmarken- Zigaretten mehr Feinstaub als teure Markenzigaretten emittieren. Dabei wurde der Passivrauch untersucht, welcher durch das Verrauchen verschiedener Zigarettenmarken entstand. Feinstaub stellt heutzutage den wichtigsten einzelnen gesundheitsschädlichen Faktor in Innenräumen dar. Das Augenmerk liegt dabei hauptsächlich auf den feinen Partikeln (PM2,5, PM1). Tumore, chronische Atemwegserkrankungen und eine erhöhte Mortalität stellen nur einen Teil der massiven gesundheitlichen Folgen durch Feinstaub dar. Vulnerable Bevölkerungsgruppen wie Kinder und alte Personen sind besonders durch Passivrauch gefährdet. Die Ergebnisse der Versuchsreihe dienen als Grundlage, um den gesundheitsschädlichen Einfluss des Passivrauchs zu interpretieren. Günstige Handelsmarken-Zigaretten weisen, unter anderem wegen des beständig ansteigenden Zigarettenpreises als auch der anhaltenden Inflation in Deutschland, einen wachsenden Marktanteil auf. Daher müssen sie auch weiterhin in wissenschaftlichen Untersuchungen mit einbezogen werden.
Drei teure sowie drei günstige Zigarettenmarken wurden miteinander und mit der Referenzzigarette 3R4F der Universität Kentucky verglichen. Zu den teuren Marken zählten Marlboro, Camel und Nil. Die günstigeren Handelsmarken-Zigaretten waren Giants, Goldfield und Jakordia. Die Rauchpumpe „Automatic environmental tobacco smoke emitter“ (AETSE) ermöglichte in einem definierten Raum der abgeschlossenen Rauchkammer, Passivrauch zu erzeugen, ohne die menschliche Gesundheit zu gefährden. Ein standardisiertes Rauchprotokoll garantierte dabei reproduzierbare und vergleichbare Ergebnisse. Das Laser Aerosolspektrometer (LAS) Modell 1.109 der Firma Grimm wies eine Messspanne von 0,25 μm bis 32 μm auf. So konnte der Feinstaub gemessen und gruppiert werden. Obwohl der Versuchsaufbau nicht vollkommen realitätsgetreu war, entstand ein adäquater Vergleich der Feinstaubemissionen von (Handels-)Markenzigaretten.
PM10 und PM2,5 wurden erhoben, weil sie die von der EU und WHO standardisierten Messwerte für die Luftverschmutzung durch Feinstaub sind. Die Messung von PM1 rechtfertigt sich durch die stärker gesundheitsschädigende Komponente von Partikeln dieser Größenordnung. Für diese drei Größenfraktionen wurden die mittlere Konzentration Cmean sowie die Area Under The Curve (AUC) ermittelt. Die AUC stellt dabei die Höhe der Gesamtexposition durch Feinstaub dar.
Die Ergebnisse dieser Versuchsreihe zeigen, dass PM1 den größten Anteil der Feinstaubemission der getesteten Zigaretten ausmachte. Alle Zigarettenmarken haben in einem abgeschlossenen Raum Feinstaubmengen in gesundheitsgefährdender Menge produziert. Die Handelsmarke Jakordia emittierte beim Verrauchen generell weniger Feinstaub als alle anderen Zigarettenmarken. Im Allgemeinen konnte kein Unterschied zwischen den günstigen Handels- und den teuren Markenzigaretten festgestellt werden. Es ist wissenschaftlich belegt, dass sich jede Feinstaubkonzentration negativ auf die Gesundheit auswirkt. Die Ergebnisse können dementsprechend in Gänze unter dem Gesichtspunkt der Gesundheitsschädlichkeit eingestuft werden.
Aufgrund veralteter und unspezifischer, beziehungsweise fehlender Angaben zu den Inhaltsstoffen der einzelnen Zigarettensorten, konnte die Ursache der Unterschiede zwischen Jakordia und den anderen Marken nicht geklärt werden. Die Zigarettenhersteller müssen verpflichtet werden, die detaillierten Zusammensetzungen der Tabakprodukte den Behörden wie dem BMEL oder dem Bundesgesundheitsministerium zugänglich zu machen. Dies wäre ein wichtiger Bestandteil für die zukünftige Forschung und Risikobewertung der verschiedenen Inhalts- und Zusatzstoffe.
Generating predictions about environmental regularities, relying on these predictions, and updating these predictions when there is a violation from incoming sensory evidence are considered crucial functions of our cognitive system for being adaptive in the future. The violation of a prediction can result in a prediction error (PE) which affects subsequent memory processing. In our preregistered studies, we examined the effects of different levels of PE on episodic memory. Participants were asked to generate predictions about the associations between sequentially presented cue-target pairs, which were violated later with individual items in three PE levels, namely low, medium, and high PE. Hereafter, participants were asked to provide old/new judgments on the items with confidence ratings, and to retrieve the paired cues. Our results indicated a better recognition memory for low PE than medium and high PE levels, suggesting a memory congruency effect. On the other hand, there was no evidence of memory benefit for high PE level. Together, these novel and coherent findings strongly suggest that high PE does not guarantee better memory.
Aim: Replicate the analysis conducted by Prof. Dr. Alexander W. Schmidt-Catran (Goethe University Frankfurt), Prof. Dr. Malcolm Fairbrother (Umea University), and Prof. Dr. Hans-Jürgen Andreß (University of Cologne) that was published in a special issue on Cross-National Comparative Research in the German academic journal Kölner Zeitschrift für Soziologie und Sozialpsychologie in 2019. Result: Almost all calculations, tables and graphs from Schmidt-Catran et al. (2019) could be replicated sufficiently well in R.
This article studies two African American examples of provincialising Europe "from the inside", James Baldwin's essay "Stranger in the Village" and Vincent O. Carter's "The Bern Book", both set in 1950's Switzerland. It investigates how these texts reverse the ethnographic gaze at the "other" and use the rural Swiss scenario to imagine Europe as historically backward. While the authors differ in their intentions, both acts of provincialisation leave the superiority of European high culture intact.
This contribution gathers eight interviews with international scholars of different generations and disciplines who study Black European literatures: Elisabeth Bekers, Jeannot Moukouri Ekobe, Polo B. Moji, Deborah Nyangulu, Jeannette Oholi, Anne Potjans, Nadjib Sadikou, and Dominic Thomas. The aim is to make literary research on Black Europe more visible to scholars in comparative literature and to contribute to a discussion on research perspectives, theories, and future challenges and needs.