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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.
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.
The elliptic (v2) and triangular (v3) azimuthal anisotropy coefficients in central 3He+Au, d+Au, and p+Au collisions at sNN−−−√ = 200 GeV are measured as a function of transverse momentum (pT) at mid-rapidity (|η|<0.9), via the azimuthal angular correlation between two particles both at |η|<0.9. While the v2(pT) values depend on the colliding systems, the v3(pT) values are system-independent within the uncertainties, suggesting an influence on eccentricity from sub-nucleonic fluctuations in these small-sized systems. These results also provide stringent constraints for the hydrodynamic modeling of these systems.
The elliptic (v2) and triangular (v3) azimuthal anisotropy coefficients in central 3He+Au, d+Au, and p+Au collisions at sNN−−−√ = 200 GeV are measured as a function of transverse momentum (pT) at mid-rapidity (|η|<0.9), via the azimuthal angular correlation between two particles both at |η|<0.9. While the v2(pT) values depend on the colliding systems, the v3(pT) values are system-independent within the uncertainties, suggesting an influence on eccentricity from sub-nucleonic fluctuations in these small-sized systems. These results also provide stringent constraints for the hydrodynamic modeling of these systems.
Off-central heavy-ion collisions are known to feature magnetic fields with magnitudes and characteristic gradients corresponding to the scale of the strong interactions. In this work, we employ equilibrium lattice simulations of the underlying theory, QCD, involving similar inhomogeneous magnetic field profiles to achieve a better understanding of this system. We simulate three flavors of dynamical staggered quarks with physical masses at a range of magnetic fields and temperatures, and extrapolate the results to the continuum limit. Analyzing the impact of the field on the quark condensate and the Polyakov loop, we find non-trivial spatial features that render the QCD medium qualitatively different as in the homogeneous setup, especially at temperatures around the transition. In addition, we construct leading-order chiral perturbation theory for the inhomogeneous background and compare its prediction to our lattice results at low temperature. Our findings will be useful to benchmark effective theories and low-energy models of QCD for a better description of peripheral heavy-ion collisions.
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 compares Chika Unigwe's novel "On Black Sisters' Street" and Sudabeh Mortezai's film "Joy", both about Nigerian women trafficked for sex work to Belgium and Austria respectively. They share a genre genealogy with slave narratives but are primarily concerned with European (neo-)colonialism. Drawing on postcolonial and intersectional theory as well as imagology, this article analyses the Black female re-imagination and strategic exoticisation of Europe in the two narratives.
In relativistic heavy-ion collisions, a global spin polarization, PH, of Λ and Λ¯ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing PH with decreasing sNN−−−√. A splitting between Λ and Λ¯ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of sNN−−−√=19.6 and 27 GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of PΛ¯−PΛ<0.24% and PΛ¯−PΛ<0.35%, respectively, at a 95% confidence level. We derive an upper limit on the naïve extraction of the late-stage magnetic field of B<9.4⋅1012 T and B<1.4⋅1013 T at sNN−−−√=19.6 and 27 GeV, respectively, although more thorough derivations are needed. Differential measurements of PH were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of |y|<1 and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.
Purpose: To evaluate intermediate and long-term visual outcomes and safety of a phakic intraocular posterior chamber lens with a central hole (ICL V4c) for myopic eyes.
Methods: Retrospective, consecutive case study of patients that uneventfully received a ICL V4c for myopia correction, with a 5-year postoperative follow-up. Department of Ophthalmology, Goethe University Frankfurt, Germany.
Results: From 241 eyes that underwent ICL implantation, we included 45 eyes with a mean age at surgery of 33 years ± 6 (18–48 years), with a 5 years follow-up. CDVA improved from 0.05logMAR ± 0.15 CDVA preoperatively to − 0.00 ± 0,07 at 5 years and did not change significantly from 3 to 5 years’ time (p = 0.266). The mean spherical equivalent (SE) improved from -10.13D ± 3.39 to − 0.45D ± 0.69. The change in endothelial cell count showed a mean decrease of 1.9% per year throughout the follow-up. Safety and efficacy index were 1.16 and 0.78, respectively. Cataract formation was seen in 2 of 241 eyes (0.8%), but in none of the 45 eyes that finished the 5-year follow-up.
Conclusions: Our data show a good intermediate and long-term stability, efficiency, and safety of ICL V4c phakic lenses in myopic eyes comparable to other known literature.
The category of abelian varieties over Fq is shown to be anti-equivalent to a category of Z-lattices that are modules for a non-commutative pro-ring of endomorphisms of a suitably chosen direct system of abelian varieties over Fq. On full subcategories cut out by a finite set w of conjugacy classes of Weil q-numbers, the anti-equivalence is represented by what we call w-locally projective abelian varieties.
Background/aim: The aim of this study was to analyze a population of patients who had suffered from traumatic dental injuries (TDIs) by using different patient-, trauma- and treatment-related parameters.
Material and methods: All dental records of patients ≥ 3 years old who had presented at the dental emergency service between Jan 1, 2009 and Dec 31, 2016 for the treatment of dental trauma were analyzed. A total of 2758 patients were invited for a recall examination at the Department for Dental Surgery and Implantology, ZZMK Carolinum, Goethe University Frankfurt, Germany; of these, 269 patients attended their recall appointments.
Results: The enrolled patient population consisted of 1718 males and 1040 females, with a mean age of 19.63 years (median 12.00 ± 17.354 years). A total of 4909 injured teeth were assessed, with a mean of 1.78 injured teeth per patient (median 2.00 ± 1.279). Males were found to be more frequently affected by TDIs compared to females (1.65:1). The majority of these injuries occurred in the first two decades of life (66.1%; n = 1824). The majority of the patients presented for initial treatment within 24 h of their accident (95.7%). The most frequent TDIs were isolated luxation injuries 49.4% (n = 2426) and isolated crown fractures 30% (n = 1472). Combination injuries were diagnosed in 20.6% of the cases (n = 1011).
Conclusions: Based on the findings of the present analysis, it can be concluded that males were more frequently affected by TDIs than females. Most patients had suffered from TDI before they had turned 10 years of age. Overall, the enamel–dentin fracture was found to be the most frequent injury, followed by concussions and lateral luxations.
Eine barrierefreie Teilnahme am alltäglichen Leben stellt für Menschen mit aktiver Epilepsie häufig eine Herausforderung dar. Epileptische Anfälle können in Kindergarten, Schule und am Arbeitsplatz sowie im häuslichen Umfeld Unsicherheit und Überforderung hervorrufen. Individuell erstellte Pläne für Betreuende, Angehörige, Aufsichtspersonen und den Rettungsdienst sollen im Falle eines akuten Anfalls geeignete Handlungsanweisungen geben. Bisher gibt es hierfür im deutschsprachigen Raum keine standardisierten Vorlagen. Mit den Handlungsplänen bei epileptischen Anfällen für Laien (HEAL) bzw. Therapeuten (HEAT) werden hier 2 Formulare vorgestellt, die zum einen eine standardisierte Grundlage bieten und andererseits leicht auf den individuellen Bedarf angepasst werden können.
Predator-prey interactions are vital for organismal survival. They shape anti-predator mechanisms and often depend on sensory abilities. Tadpoles use chemical cues, such as injury cues (alarm cues), to assess predation risks and modify their life-history, morphology, and behaviours accordingly. However, the prevalence of chemically mediated anti-predator responses in species with distinct ecological niches (e.g. within phytotelmata) remains unknown, hindering our understanding of the ecological significance and evolution of alarm substances. Therefore, our study aimed to investigate chemically mediated anti-predator responses in tadpoles of two Neotropical poison dart frogs, Ranitomeya sirensis and Epipedobates anthonyi (and compare their responses to two Palearctic model organisms, Rana temporaria and Bufo bufo, which are known to utilise alarm substances). Through behavioural bioassays, we exposed predator-naïve tadpoles to extracts of each species (i.e. con- and heterospecific cues), including water as a control (i.e. five treatments per species). We assessed changes in their activity before and after stimulus introduction. Our results show that E. anthonyi did not respond to any of the stimuli, whereas R. sirensis displayed increased activity levels exclusively in response to conspecific cues, but not to heterospecific cues. With this, our findings suggest a specialized recognition system in R. sirensis, potentially directed at conspecific competitors but likely unrelated to anti-predator mechanisms. In contrast, E. anthonyi may be insensitive to injury cues or utilize alternative sensory modalities to respond to acute predation events. This study sheds light on the chemical alarm response system of Neotropical poison dart frog tadpoles, providing foundational understanding of how dendrobatids react to injury cues. It prompts questions about the ecological significance and evolutionary implications of chemical communication in species facing extreme resource limitation during development and underscores the importance of comparative research for understanding chemical communication in diverse aquatic ecosystems.
The little-known Roman gold mining site "Gralheira" is located near the well-explored mine of Tresminas. The 2.5 km long, almost dead straight archaeological monument from the first and second centuries AD is currently under threat from possible mining activities on the one hand and from modern waste disposal in the pits on the other. Since 2019, the Roman mining traces have been investigated by means of intensive field inspections, terrestrial 3d laser scanning and aerial photography. The following article will present first impressions and findings on this structure, as well as questions and preliminary interpretations.
Annotationes Epigraphicae XIII. Zu einigen Inschriften aus der römischen Provinz Gallia Lugdunensis
(2023)
Die seit einigen Jahren andauernde Arbeit an einem kommentierenden Onomastikon für die römische Provinz Gallia Lugdunensis, das in absehbarer Zeit erscheinen soll, lenkte die Aufmerksamkeit des Autors auf mehrere bemerkenswerte Inschriften aus der zentralgallischen Provinz, die ausführlichere Betrachtungen rechtfertigen. Alle folgenden Anmerkungen zu 15 ausgewählten Inschriften beziehen sich auf epigraphische und onomastische Denkwürdigkeiten, die in wesentlich kürzerer Form auch in dem angekündigten Namenskatalog verschriftlicht wurden.
Using data samples with an integrated luminosity of 6.4~fb−1 collected by the BESIII detector operating at the BEPCII storage ring, the process of e+e−→γϕJ/ψ is studied. The processes of e+e−→ϕχc1,c2, χc1,c2→γJ/ψ are observed with a significance of more than 10σ. The s√-dependent cross section of e+e−→ϕχc1,c2 is measured between 4.600 and 4.951~GeV, and evidence of a resonance structure is found for the first time in the ϕχc2 process. We also search for the processes of e+e−→γX(4140), γX(4274) and γX(4500) via the γϕJ/ψ final state, but no obvious structures are found. The upper limits on the production cross section times the branching fraction for these processes at the 90% confidence level are reported.
Observation of χcJ → 3(K⁺K⁻)
(2023)
By analyzing (27.12±0.14)×108 ψ(3686) events collected with the BESIII detector operating at the BEPCII collider, the decay processes χcJ→3(K+K−) (J=0,1,2) are observed for the first time with statistical significances of 8.2σ, 8.1σ, and 12.4σ, respectively. The product branching fractions of ψ(3686)→γχcJ, χcJ→3(K+K−) are presented and the branching fractions of χcJ→3(K+K−) decays are determined to be Bχc0→3(K+K−)=(10.7±1.8±1.1)×10−6, Bχc1→3(K+K−)=(4.2±0.9±0.5)×10−6, and Bχc2→3(K+K−)=(7.2±1.1±0.8)×10−6, where the first uncertainties are statistical and the second are systematic.
Coercion or privatization? Crisis and planned economies in the debates of the early Frankfurt School
(2023)
The 1930s–1940s underwent profound structural economic and political turmoil following the collapse of the nineteenth century liberal market economies. The intellectual debates of the time were dominated by the question of whether Marx’s theory of the tendency of rate of profit to fall was true, or what consequence could be imagined in the survival of capitalist societies. Placed in the middle of such debates was also the reorganization of national productions into war economies. By means of reconstructive analysis, the paper provides a critical overview of the debates that took place within the circle of the Frankfurt School during those years. It also advances an interpretive thesis suggesting that remedies to capitalist crises of the time turned state powers into privatized, illiberal coercive entities. Coercion and privatization reinforced each other. This general tendency is well illustrated by the famous Pollock-Neumann debate. These intellectuals expressed views not only intended to shed light on the historical period of time, but also to formulate long-term considerations on the authoritarian trends embedded in our contemporary democracies. Through historical reconstruction, the paper’s aim is to identify a long-term structural thread of transformation starting from the transformation of the German economy in 1930s and touching upon post Second World War problems of states’ restructuring along privatization/coercion divides.
Background: Multiple studies have focused on medical and pharmacological treatments and outcome predictors of patients with status epilepticus (SE). However, a sufficient understanding of recurrent episodes of SE is lacking. Therefore, we reviewed recurrent SE episodes to investigate their clinical characteristics and outcomes in patients with relapses.
Methods: In this retrospective, multicenter study, we reviewed recurrent SE patient data covering 2011 to 2017 from the university hospitals of Frankfurt and Marburg, Germany. Clinical characteristics and outcome variables were compared among the first and subsequent SE episodes using a standardized form for data collection.
Results: We identified 120 recurrent SE episodes in 80 patients (10.2% of all 1177 episodes). The mean age at the first SE episode was 62.2 years (median 66.5; SD 19.3; range 21–91), and 42 of these patients were male (52.5%). A mean of 262.4 days passed between the first and the second episode. Tonic–clonic seizure semiology and a cerebrovascular disease etiology were predominant in initial and recurrent episodes. After subsequent episodes, patients showed increased disability as indicated by the modified Rankin Scale (mRS), and 9 out of 80 patients died during the second episode (11.3%). Increases in refractory and super-refractory SE (RSE and SRSE, respectively) were noted during the second episode, and the occurrence of a non-refractory SE (NRSE) during the first SE episode did not necessarily provide a protective marker for subsequent non-refractory episodes. An increase in the use of intravenous-available anti-seizure medication (ASM) was observed in the treatment of SE patients. Patients were discharged from hospital with a mean of 2.8 ± 1.0 ASMs after the second SE episode and 2.1 ± 1.2 ASMs after the first episode. Levetiracetam was the most common ASM used before admission and on discharge for SE patients.
Conclusions: This retrospective, multicenter study used the mRS to demonstrate worsened outcomes of patients at consecutive SE episodes. ASM accumulations after subsequent SE episodes were registered over the study period. The study results underline the necessity for improved clinical follow-ups and outpatient care to reduce the health care burden from recurrent SE episodes.
We report a search for a dark photon using 14.9~fb−1 of e+e− annihilation data taken at center-of-mass energies from 4.13 to 4.60~GeV with the BESIII detector operated at the BEPCII storage ring. The dark photon is assumed to be produced in the radiative annihilation process of e+e− and to predominantly decay into light dark matter particles, which escape from the detector undetected. The mass range from 1.5 to 2.9~GeV is scanned for the dark photon candidate, and no significant signal is observed. The mass dependent upper limits at the 90% confidence level on the coupling strength parameter ϵ for a dark photon coupling with an ordinary photon vary between 1.6×10−3 and 5.7×10−3.
Improved measurement of the branching fractions of the inclusive decays D⁺ → Kₛ⁰X and D⁰ → Kₛ⁰X
(2023)
By analyzing 2.93 fb−1 of e+e− collision data taken at the center-of-mass energy of 3.773 GeV with the BESIII detector, the branching fractions of the inclusive decays D+→K0SX and D0→K0SX are measured to be (32.78±0.13±0.27)% and (20.54±0.12±0.18)%, respectively, where the first uncertainties are statistical and the second are systematic. These results are consistent with the world averages of previous measurements, but with improved precision.
We consider ground state solutions u ∈ H2(RN) of biharmonic (fourth-order) nonlinear Schrodinger equations of the form ¨2u + 2au + bu − |u| p−2u = 0 in RN with positive constants a, b > 0 and exponents 2 < p < 2∗, where 2∗ = 2N N−4 if N > 4 and 2∗ = ∞ if N ≤ 4. By exploiting a connection to the adjoint Stein–Tomas inequality on the unit sphere and by using trial functions due to Knapp, we prove a general symmetry breaking result by showing that all ground states u ∈ H2(RN) in dimension N ≥ 2 fail to be radially symmetric for all exponents 2 < p < 2N+2 N−1 in a suitable regime of a, b > 0. As applications of our main result, we also prove symmetry breaking for a minimization problem with constrained L2-mass and for a related problem on the unit ball in RN subject to Dirichlet boundary conditions.
Eine barrierefreie Teilnahme am alltäglichen Leben stellt für Menschen mit aktiver Epilepsie häufig eine Herausforderung dar. Epileptische Anfälle können in Kindergarten, Schule und am Arbeitsplatz sowie im häuslichen Umfeld Unsicherheit und Überforderung hervorrufen. Individuell erstellte Pläne für Betreuende, Angehörige, Aufsichtspersonen und den Rettungsdienst sollen im Falle eines akuten Anfalls geeignete Handlungsanweisungen geben. Bisher gibt es hierfür im deutschsprachigen Raum keine standardisierten Vorlagen. Mit den Handlungsplänen bei epileptischen Anfällen für Laien (HEAL) bzw. Therapeuten (HEAT) werden hier 2 Formulare vorgestellt, die zum einen eine standardisierte Grundlage bieten und andererseits leicht auf den individuellen Bedarf angepasst werden können.
We report directed flow (v1) of multistrange baryons (Ξ and Ω) and improved v1 data for K−, p¯, Λ¯ and ϕ in Au+Au collisions at sNN−−−√=27 and 200 GeV from the STAR at the Relativistic Heavy Ion Collider (RHIC). We focus on particles whose constituent quarks are not transported from beam rapidity rather produced in the collisions. In midcentral collisions, we observe a coalescence sum rule for hadron combinations with identical quark content and a difference (``splitting'') in the slope of v1 vs. rapidity for combinations having nonidentical quark content. The splitting strength appears to increase with the electric charge difference and strangeness content difference of the constituent quarks in the combinations, consistent with an electromagnetic effect. The peripheral collision statistics are insufficient to draw firm conclusions.
Rationale and objectives: To provide a detailed analysis of injury patterns of the spine following blunt trauma and establish the role of supplementary MRI by evaluating discrepancies in the detection rates of damaged structures in CT and MRI.
Method: 216 patients with blunt trauma to the spine who underwent CT followed by supplementary MRI were included in this study. Two board-certified radiologists blinded to clinical symptoms and injury mechanisms independently interpreted all acquired CT and MRI images. The interpretation was performed using a dedicated catalogue of typical findings associated with spinal trauma and assessed for spinal stability using the AO classification systems.
Results: Lesions to structures associated with spinal instability were present in 31.0% in the cervical spine, 12.3% in the thoracic spine, and 29.9% in the lumbar spine. In all spinal segments, MRI provided additional information regarding potentially unstable injuries. Novel information derived from supplementary MRI changed clinical management in 3.6% of patients with injury to the cervical spine. No change in clinical management resulted from novel information on the thoracolumbar spine. Patients with injuries to the vertebral body, intervertebral disc, or spinous process were significantly more likely to benefit from supplementary MRI.
Conclusion: In patients that sustained blunt spinal trauma, supplementary MRI of the cervical spine should routinely be performed to detect injuries that require surgical treatment, whereas CT is the superior imaging modality for the detection of unstable injuries in the thoracolumbar spine.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2023)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane. This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions. A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of \(R=0.4\) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb+Pb collision data.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2023)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane.This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions.A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of \(R=0.4\) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb-Pb collision data.
In order to effectively address global environmental problems, it is important that future decision-makers in society are aware of the safe operation space for humans, which is limited by the planetary boundaries. Until now, however, there has been a lack of international studies examining how the planet's boundaries are perceived. In this study, we investigated how students of environmental and sustainability studies in 35 countries (n = 4140) assess the planetary boundaries. Based on the rating, using spectral clustering, the 35 countries were assigned to five different clusters. Four indicators (Human Development Index, Legatum Prosperity Index, Natural Resources Income and Forest Area) were used to provide explanations for the clustering result. The indices allow a distinction between the clusters and provide initial explanations for the clustering. The results provide important insights for today's decision-makers, as possible measures for action in the individual countries can be derived from the findings.
Post-merger gravitational-wave signal from neutron-star binaries: a new look at an old problem
(2023)
The spectral properties of the post-merger gravitational-wave signal from a binary of neutron stars encodes a variety of information about the features of the system and of the equation of state describing matter around and above nuclear saturation density. Characterising the properties of such a signal is an “old” problem, which first emerged when a number of frequencies were shown to be related to the properties of the binary through “quasi-universal” relations. Here we take a new look at this old problem by computing the properties of the signal in terms of the Weyl scalar ψ4. In this way, and using a database of more than 100 simulations, we provide the first evidence for a new instantaneous frequency, f ψ4 0, associated with the instant of quasi timesymmetry in the postmerger dynamics, and which also follows a quasi-universal relation. We also derive a new quasi-universal relation for the merger frequency f h mer, which provides a description of the data that is four times more accurate than previous expressions while requiring fewer fitting coefficients. Finally, consistently with the findings of numerous studies before ours, and using an enlarged ensamble of binary systems we point out that the ℓ = 2, m = 1 gravitational-wave mode could become comparable with the traditional ℓ = 2, m = 2 mode on sufficiently long timescales, with strain amplitudes in a ratio |h 21|/|h 22| ∼ 0.1 − 1 under generic orientations of the binary, which could be measured by present detectors for signals with large signal-to-noise ratio or by third-generation detectors for generic signals should no collapse occur.
Post-merger gravitational-wave signal from neutron-star binaries: a new look at an old problem
(2023)
The spectral properties of the post-merger gravitational-wave signal from a binary of neutron stars encodes a variety of information about the features of the system and of the equation of state describing matter around and above nuclear saturation density. Characterizing the properties of such a signal is an “old” problem, which first emerged when a number of frequencies were shown to be related to the properties of the binary through “quasiuniversal” relations. Here we take a new look at this old problem by computing the properties of the signal in terms of the Weyl scalar ψ4. In this way, and using a database of more than 100 simulations, we provide the first evidence for a new instantaneous frequency, y f0 4, associated with the instant of quasi-time-symmetry in the dynamics, and which also follows a quasi-universal relation. We also derive a new quasi-universal relation for the merger frequency f h mer, which provides a description of the data that is 4 times more accurate than previous expressions while requiring fewer fitting coefficients. Finally, consistent with the findings of numerous studies before ours, and using an enlarged ensemble of binary systems, we point out that the ℓ = 2, m = 1 gravitational-wave mode could become comparable with the traditional ℓ = 2, m = 2 mode on sufficiently long timescales, with strain amplitudes in a ratio |h21|/|h22| ∼ 0.1–1 under generic orientations of the binary, which could be measured by present detectors for signals with a large signal-to-noise ratio or by third-generation detectors for generic signals should no collapse occur.
The amplification of magnetic fields plays an important role in explaining numerous astrophysical phenomena associated with binary neutron star mergers, such as mass ejection and the powering of short gamma-ray bursts. Magnetic fields in isolated neutron stars are often assumed to be confined to a small region near the stellar surface, while they are normally taken to fill the whole star in numerical modeling of mergers. By performing high-resolution, global, and high-order general-relativistic magnetohydrodynamic simulations, we investigate the impact of a purely crustal magnetic field and contrast it with the standard configuration consisting of a dipolar magnetic field with the same magnetic energy but filling the whole star. While the crust configurations are very effective in generating strong magnetic fields during the Kelvin–Helmholtz-instability stage, they fail to achieve the same level of magnetic-field amplification of the full-star configurations. This is due to the lack of magnetized material in the neutron-star interiors to be used for further turbulent amplification and to the surface losses of highly magnetized matter in the crust configurations. Hence, the final magnetic energies in the two configurations differ by more than 1 order of magnitude. We briefly discuss the impact of these results on astrophysical observables and how they can be employed to deduce the magnetic topology in merging binaries.
The nucleus reuniens drives hippocampal goal‑directed trajectory sequences for route planning
(2023)
Goal-directed spatial navigation requires accurate estimates of one’s position and destination, as well as careful planning of a route between them to avoid known obstacles in the environment. Despite its general importance across species, the neural circuitry supporting the ability for route planning remains largely unclear. Previous studies described that place cells in the hippocampal CA1 encode the animal's next movement direction (Wood et al., 2000; Ito et al., 2015) and upcoming navigational routes (Pfeiffer & Foster, 2013). However, it has been shown that part of the CA1 activity representing the animal’s future behaviors is not necessarily generated in the hippocampus, but is derived from the medial prefrontal cortex (PFC) via the nucleus reuniens of the thalamus (RE) (Ito et al., 2015). Notably, the importance of the PFC in navigation has been demonstrated in several studies, including the recent finding of a goal map in the orbitofrontal cortex (Basu et al., 2021). Therefore, I hypothesized that information flow from the PFC to CA1 via the RE plays a key role in route planning.
To assess the animals' route planning ability, I designed a new navigation task in which a rat has to navigate to a fixed target location from various starting positions in an arena. Furthermore, by adding an L-shaped wall in the maze and removing all light sources in the experimental room, this task forced the animals to plan a wall-avoiding route without relying on direct sensory perceptions. I confirmed that rats could learn this task successfully, memorizing the wall location and taking a smooth wall-avoidance route. To test the role of the RE, I inactivated RE neurons by expressing the inhibitory opsin SwiChR++, which resulted in a significant deficit in the animal’s route planning ability, taking a longer non-smooth path to the destination. By contrast, this manipulation did not affect navigation performance when a straight goal-directed route was available, suggesting a specific role of the RE in route planning. I further found that DREADDs-mediated inactivation of neurons in the bilateral hippocampi resulted in a similar deficit in route planning ability, implying cooperation between the RE and the hippocampus.
I finally examined the activity of hippocampal CA1 neurons with and without RE inactivation. While neurons in the hippocampus exhibited brief trajectory sequences corresponding to the animal’s subsequent goal-directed journey, I found that this goal-directed bias of trajectory events was significantly reduced by RE inactivation, likely associated with route-planning deficits in these animals.
Altogether, this dissertation demonstrates the role of the RE from both behavioral and neural coding perspectives, identifying a pivotal circuit element supporting the animal’s route-planning ability.
We have investigated the systematic differences introduced when performing a Bayesian-inference analysis of the equation of state (EOS) of neutron stars employing either variable- or constant-likelihood functions. The former has the advantage of retaining the full information on the distributions of the measurements, making exhaustive usage of the data. The latter, on the other hand, has the advantage of a much simpler implementation and reduced computational costs. In both approaches, the EOSs have identical priors and have been built using the sound speed parameterization method so as to satisfy the constraints from X-ray and gravitational waves observations, as well as those from chiral effective theory and perturbative quantum chromodynamics. In all cases, the two approaches lead to very similar results and the 90% confidence levels essentially overlap. Some differences do appear, but in regions where the probability density is extremely small and are mostly due to the sharp cutoff on the binary tidal deformability L˜ 720 set in the constant-likelihood approach. Our analysis has also produced two additional results. First, an inverse correlation between the normalized central number density, nc,TOV/ns, and the radius of a maximally massive star, RTOV. Second, and most importantly, it has confirmed the relation between the chirp mass and the binary tidal deformability. The importance of this result is that it relates chirp, which is measured very accurately, and L˜ , which contains important information on the EOS. Hence, when chirp is measured in future detections, our relation can be used to set tight constraints on L˜ .
Using 2.93 fb−1 of e+e− collision data collected with the BESIII detector at the center-of-mass energy 3.773 GeV, we perform the first amplitude analysis of the decay D+ → π+π0π0 and determine the relative magnitudes and phases of different intermediate processes. The absolute branching fraction of D+ → π+π0π0 is measured to be (2.888 ± 0.058stat. ± 0.069syst.)%. The dominant intermediate processes are D+ → a1(1260)+(→ ρ+π0) and D+ → *0ρ+, with branching fractions of (8.66 ± 1.04stat. ± 1.39syst.) × 10−3 and (9.70 ± 0.81stat. ± 0.53syst.) × 10−3, respectively.
We report a new measurement of transverse single-spin asymmetries for dijet production in collisions of polarized protons at s√ = 200 GeV. Possible correlations between the proton spin and the transverse momenta of its partons, mutually orthogonal, with each perpendicular to the proton momentum direction, are probed at high Q2 ≈160 GeV2. The associated Sivers observable ⟨kT⟩, the average parton transverse momentum, is extracted using simple kinematics. Nonzero Sivers effects are observed for the first time in proton-proton collisions, but only when the jets are sorted by their net charge, which enhances the u- or d-quark contributions to separate data samples. This also enables a determination of the individual partonic contributions to the observed asymmetries.
We report the first measurements of cumulants, up to 4th order, of deuteron number distributions and proton-deuteron correlations in Au+Au collisions recorded by the STAR experiment in phase-I of Beam Energy Scan (BES-I) program at the Relativistic Heavy Ion Collider (RHIC). Deuteron cumulants, their ratios, and proton-deuteron mixed cumulants are presented for different collision centralities covering a range of center of mass energy per nucleon pair sNN−−−√ = 7.7 to 200 GeV. It is found that the cumulant ratios at lower collision energies favor a canonical ensemble over a grand canonical ensemble in thermal models. An anti-correlation between proton and deuteron multiplicity is observed across all collision energies and centralities, consistent with the expectation from global baryon number conservation. The UrQMD model coupled with a phase-space coalescence mechanism qualitatively reproduces the collision-energy dependence of cumulant ratios and proton-deuteron correlations.
Using a sample of (10.09 ± 0.04) × 109 J/ψ decays collected with the BESIII detector, partial wave analyses of the decay J/ψ → γK0SK0Sπ0 are performed within the K0SK0Sπ0 invariant mass region below 1.6 GeV/c2. The covariant tensor amplitude method is used in both mass independent and mass dependent approaches. Both analysis approaches exhibit dominant pseudoscalar and axial vector components, and show good consistency for the other individual components. Furthermore, the mass dependent analysis reveals that the K0SK0 Sπ0 invariant mass spectrum for the pseudoscalar component can be well described with two isoscalar resonant states using relativistic Breit-Wigner model, i.e., the η(1405) with a mass of 1391.7±0.7+11.3 −0.3 MeV/c 2 and a width of 60.8±1.2+5.5 −12.0 MeV, and the η(1475) with a mass of 1507.6±1.6+15.5−32.2 MeV/c2 and a width of 115.8±2.4 +14.8 −10.9 MeV. The first and second uncertainties are statistical and systematic, respectively. Alternate models for the pseudoscalar component are also tested, but the description of the K0SK0Sπ0invariant mass spectrum deteriorates significantly.
This work aimed to investigate the regulation and activity of 5-lipoxygenase (5-LO), the central enzyme in leukotriene biosynthesis, in two colorectal cancer cell lines. The leukotriene pathway is positively correlated with the progression of several solid malignancies; however, factors regulating 5-LO expression and activity in tumors are poorly understood.
Cancer development, as well as cancer progression, are strongly dependent on the tumor microenvironment. In the conventional monolayer culture of cancer cell lines, cell-matrix and cell-cell interactions present in native tumors are absent. Furthermore, it is already known that various colon cancer cell lines dysregulate several important signaling pathways due to 3D growth. Therefore, the expression of the leukotriene cascade in HT-29 and HCT-116 colorectal cancer cells was investigated within a three-dimensional context using multicellular tumor spheroids to mimic a more physiological environment compared to conventional cell culture. Especially the expression of 5-LO, cPLA2α, and LTA4 hydrolase was altered due to threedimensional (3D) cell growth, which was investigated by qPCR and Western blot analysis. High cellular density in monolayer cultures led to similar results. The observed 5-LO upregulation was found inversely correlated with cell proliferation, determined by cell cycle analysis, and activation of PI3K/mTORC-2- and MEK-1/ERK-dependent pathways, determined using pharmacological pathway inhibition, stable shRNA knockdown cell lines, and analysis via qPCR and Western blot analysis. Following, the transcription factor E2F1 and its target gene MYBL2 were identified to play a role in the repression of 5-LO during cell proliferation. For this purpose, several stable MYBL2 over-expression and ALOX5 reporter cell lines were prepared and analyzed. Since 5-LO was already identified as a direct p53 target gene, the influence of p53, which is variably expressed in the cell lines (HT-29, p53 R273H mut; HCT-116 p53 wt; HCT-116 p53 KO), was investigated as well. Furthermore, HCT-116 cells carrying a p53 knockout were investigated. The PI3K/mTORC-2- and MEK-1/ERK-dependent suppression of 5-LO was also found in tumor cells from other origins (Capan-2, Caco-2, MCF-7), which was determined using pharmacological pathway inhibition and following analysis via qPCR. This suggests that the identified mechanism might apply to other tumor entities as well.
5-LO activity was previously described as attenuated in HT-29 and HCT-116 cells compared to polymorphonuclear leukocytes, which express a highly active 5-LO. However, the present study showed that the enzyme activity is indeed low but inducible in HT-29 and HCT-116 cells. Of note, the general lipid mediator profile and the mediator concentrations were comparable to those of M2 macrophages. Finally, the analysis of substrate availability in HT-29 and HCT-116 cells revealed a vast difference between formed metabolite concentrations and supplemented fatty acid concentrations, indicating that the substrates are either transformed into lipoxygenase-independent metabolites or are esterified into the cellular membrane.
In summary, the data presented in this work demonstrate that 5-LO expression and activity are tightly regulated in HT-29 and HCT-116 cells and fine-tuned due to environmental conditions. The cells suppress 5-LO during proliferation but upregulate the expression and activity of the enzyme under cellular stress-triggering conditions. This implies a possible role of 5-LO in manipulating the tumor stroma to support a tumor-promoting microenvironment.
Weltweit gibt es laut WHO ca. 58 Millionen Menschen mit einer chronischen Hepatitis-C-Virus (HCV) Infektion und jährlich stecken sich ca. 1,5 Millionen Menschen neu mit diesem Virus an (Stand 2019). Da die Folge einer chronischen Hepatitis-C-Virus Infektion eine potenziell tödlich verlaufende Leberzirrhose oder die Entwicklung eines Hepatozellulären Karzinoms sein können, ist eine frühe Diagnose und eine adäquate Therapie eine wichtige Aufgabe in der Medizin.
Die bisherige Therapie erfolgte mittels pegyliertem Interferon und Ribavirin und seit einigen Jahren auch interferonfrei mittels Direkter Antiviraler Agenzien (DAA). Vor allem beim älteren Therapieregime konnten viele Nebenwirkungen und häufiger auch ein Therapieversagen auftreten, sodass ein leicht zu gewinnender Biomarker nützlich wäre, der die Patienten mit Therapieversagen frühzeitig und im besten Fall sogar vor Therapiebeginn detektieren kann.
In der vorliegenden Arbeit wurden die Spiegel von extrazellulär im Blut zirkulierender, leberspezifischer microRNA miR-122 auf Eigenschaften als solche potenzielle Biomarker untersucht. Dazu wurden die Patientenseren von insgesamt 60 Patienten mit chronischer Hepatitis-C-Virus Infektion analysiert, die mittels pegyliertem Interferon und Ribavirin behandelt wurden. Vor, während und nach der Therapie wurden verschiedene Laborparameter sowie die miR 122 in den Patientenseren bestimmt. 20 dieser Patienten zeigten ein dauerhaftes Ansprechen auf die Therapie (sustained virological response = SVR), 20 zeigten nach einem initialen Therapieansprechen ein Rückfall der Erkrankung (Relapse) und 20 Patienten sprachen gar nicht auf die Therapie an (Non-Responder = NR).
Zunächst wurden die sogenannten Baseline-Charakteristika der Patienten vor Therapiebeginn untersucht. Dabei konnten wir jedoch keinen Unterschied zwischen den Patientengruppen hinsichtlich der Alanin-Aminotransferase (ALT) und Aspartat-Aminotransferase (AST), zwei Laborparameter zur Bestimmung einer Leberschädigung, sowie der HCV-RNA, ein Parameter zur Bestimmung der Viruslast bei Patienten mit einer HCV-Infektion, feststellen.
Auch die miR-122-Spiegel zeigten vor Therapiebeginn keinen signifikanten Unterschied zwischen den drei Patientengruppen. Daraus wurde geschlossen, dass man die miR-122 vor Therapiebeginn nicht als prognostischen Marker für einen Therapieerfolg verwenden kann.
Beim Vergleich der miR-122-Spiegel mit den Laborparametern konnte eine signifikante Korrelation zwischen der miR-122 und der ALT, AST und der Gamma-Glutamyl-Transferase (GGT) festgestellt werden. Die miR-122 scheint somit ähnlich wie die anderen Laborparameter eine Leberzellschädigung widerzuspiegeln.
Nach dem Therapiebeginn konnte bereits ab Woche 4 ein signifikanter Unterschied zwischen den SVR und Non-Respondern sowie zwischen den Relapsepatienten und den Non-Respondern festgestellt werden. Jedoch war der Unterschied zwischen den SVR und den Relapse-Patienten nicht signifikant, sodass man weiterhin keine Unterscheidung dieser beiden Patientengruppen machen konnte.
Auch die ALT- und HCV-RNA-Spiegel zeigten einen ähnlichen Verlauf. In den Gruppen der SVR und Relapse-Patienten zeigte sich im Laufe der Therapie ein Rückgang der Parameter wohingegen die Gruppe der Non-Responder keine signifikante Dynamik aufwies.
Zum Schluss wurden die miR-122-Spiegel 12 bzw. 24 Wochen nach Therapieende bestimmt, dem sogenannten Zeitpunkt des Follow-Up bei dem der Therapieerfolg laut Leitlinie mit Hilfe der HCV-RNA-Messung bestimmt wird. Dabei konnte ein signifikanter Unterschied zwischen den miR-122-Spiegeln bei den SVR-Patienten und den anderen beiden Patientengruppen festgestellt werden.
In Zusammenschau dieser Ergebnisse kann man sagen, dass die miR-122 gut geeignet ist um ähnlich wie die HCV-RNA den Therapieverlauf widerzuspiegeln. Als prognostischer Parameter bzw. Biomarker für ein Therapieansprechen ist sie jedoch nicht geeignet, da keine Unterscheidung zwischen den einzelnen Patientengruppen vor Therapiebeginn möglich ist und während der Therapie lediglich die Non-Responder und nicht die Relapse-Patienten detektiert werden können.
The family of cubic noncentrosymmetric 3-4-3 compounds has become a fertile ground for the discovery of novel correlated metallic and insulating phases. Here, we report the synthesis of a new heavy fermion compound, Ce3Bi4Ni3. It is an isoelectronic analog of the prototypical Kondo insulator Ce3Bi4Pt3 and of the recently discovered Weyl-Kondo semimetal Ce3Bi4Pd3. In contrast to the volume-preserving Pt-Pd substitution, structural and chemical analyses reveal a positive chemical pressure effect in Ce3Bi4Ni3 relative to its heavier counterparts. Based on the results of electrical resistivity, Hall effect, magnetic susceptibility, and specific heat measurements, we identify an energy gap of 65-70 meV, about 8 times larger than that in Ce3Bi4Pt3 and about 45 times larger than that of the Kondo-insulating background hosting the Weyl nodes in Ce3Bi4Pd3. We show that this gap as well as other physical properties do not evolve monotonically with increasing atomic number, i.e., in the sequence Ce3Bi4Ni3-Ce3Bi4Pd3-Ce3Bi4Pt3, but instead with increasing partial electronic density of states of the d orbitals at the Fermi energy. To understand under which condition topological states form in these materials is a topic for future studies.
Dieser Arbeit lag die Fragestellung zugrunde, welchen Einfluss die jeweilige Transfusionsstrategie auf AML-Patienten unter intensiver Induktionschemotherapie hat.
Dafür wurde ein am Universitätsklinikum Frankfurt zwischen 2007 und 2018 behandeltes Kollektiv von 352 Patienten untersucht. So erfolgte hier bis ins Jahr 2015 hinein die Transfusion eines EK ab einem Hb-Wert <8g/dl und nach Änderung des Transfusionstriggers ab einem Hb <7g/dl. AML-Patienten aus dem Jahr 2015 – dem Jahr der Änderung der Transfusionsregel – wurden von weiterer Untersuchung ausgeschlossen, um zwei klar abgrenzbare Kohorten erhalten zu können.
Es zeigte sich, dass die weniger restriktive Transfusionskohorte unter Induktionschemotherapie einen durchschnittlich um 1g/dl höheren Hb-Wert aufwies und früher als die restriktive Kohorte transfundiert wurde. Die Anzahl an Fiebertagen, CRP-Werte, Aufenthalte auf Intensivstation sowie die Dauer des Krankenhausaufenthaltes betrachtend, zeigte sich hingegen kein signifikanter Unterscheid zwischen beiden Kohorten.
Basierend auf unserer Arbeit ergeben sich keine Hinweise dafür, dass die restriktive Transfusionspraxis einer weniger restriktiven für AML-Patienten unterlegen ist. Limitierend auf die Aussagekraft der Ergebnisse wirken sich dabei die retrospektive Natur der Arbeit sowie die zeitliche Verschiebung der Behandlungszeiträume beider Kohorten aus.
Ergebnisse der bislang ausstehenden randomisierten Studien, die den Einfluss unterschiedlicher Transfusionsregimes auf Patienten mit hämatologischen Krankheiten untersuchen, sind in Bälde zu erwarten. Die bereits vorliegenden Pilotstudien und Ergebnisse der TRIST-Studie decken sich mit der von uns beobachteten Nicht-Unterlegenheit der restriktiven Transfusionspraxis für ein hämatoonkologisches Patientenkollektiv, sodass es abzuwarten gilt, ob sich dies auch in weiteren größeren randomisierten und kontrollierten Studien beweisen kann.
Im Fokus der vorliegenden Arbeit stand die Fragestellung, inwieweit ORF10 von B. recurrentis, dem Erreger des Läuserückfallfiebers, mit verschiedenen Komplementkomponenten interagieren kann.
Mit funktionellen Komplementtests konnte gezeigt werden, dass ORF10 den klassischen, den alternativen sowie den Lektin-Weg inhibiert, wobei sich die stärkste Inhibition gegenüber dem alternativen Weg manifestierte. Darüber hinaus ließ sich in einem Zell-basierten Hämolyse-Assay eine Inhibition des terminalen Komplementweges durch ORF10 nachweisen.
Die durchgeführten Bindungsanalysen mit verschiedenen Komplementkomponenten führten zu dem Ergebnis, dass ORF10 mit C1q, C1s, C3, C3b, C4b und C5 interagiert und diese Protein-Protein-Interaktion mit den Komplementkomponenten C1q, C3, C3b und C4b durch einen dosisabhängigen Verlauf charakterisiert ist. Eine Bindung von C1r, C2, C4, FB, FH sowie FI konnte jedoch nicht nachgewiesen werden.
Auf Basis der modellierten Struktur von ORF10 wurden mithilfe der In-vitro-Mutagenese drei verschiedene Varianten generiert, die jedoch nicht affinitätschromatographisch aus E. coli-Zelllysaten isoliert werden konnten und deshalb nicht für weiterführende funktionelle Analysen zur Verfügung standen.
Die Ergebnisse der Serumbakterizidie-Tests mit einem „gain of function“-Borrelienstamm, welcher ORF10 heterolog produzieren sollte, ergaben, dass keine erhöhte Resistenz gegenüber Humanserum nachgewiesen werden konnte. Inwieweit ORF10 bei der intrinsischen Serumresistenz von B. recurrentis beteiligt ist, lässt sich abschließend nicht vollumfänglich erklären.
The quantum entangled J=ψ → ΣþΣ¯ − pairs from ð1.0087 0.0044Þ × 1010 J=ψ events taken by the BESIII detector are used to study the nonleptonic two-body weak decays Σþ → nπþ and Σ¯ − → n¯π−. The CP-odd weak decay parameters of the decays Σþ → nπþ (αþ) and Σ¯ − → n¯π− (α¯−) are determined to be 0.0481 0.0031stat 0.0019syst and −0.0565 0.0047stat 0.0022syst, respectively. The decay parameter α¯− is measured for the first time, and the accuracy of αþ is improved by a factor of 4 compared to the previous results. The simultaneously determined decay parameters allow the first precision CP symmetry test for any hyperon decay with a neutron in the final state with the measurement of ACP ¼ ðαþ þ α¯−Þ=ðαþ − α¯−Þ ¼ −0.080 0.052stat 0.028syst. Assuming CP conservation, the average decay parameter is determined as hαþi¼ðαþ − α¯−Þ=2 ¼ −0.0506 0.0026stat 0.0019syst, while the ratios αþ=α0 and α¯−=α¯ 0 are −0.0490 0.0032stat 0.0021syst and −0.0571 0.0053stat 0.0032syst, where α0 and α¯ 0 are the decay parameters of the decays Σþ → pπ0 and Σ¯ − → p¯ π0, respectively.
We search for the semi-leptonic decays Λ + c → Λπ+π−e+νe and Λ + c → pK0 Sπ−e+νe in a sample of 4.5 fb−1 of e+e− annihilation data collected in the center-of-mass energy region between 4.600 GeV and 4.699 GeV by the BESIII detector at the BEPCII. No significant signals are observed, and the upper limits on the decay branching fractions are set to be B(Λ+c → Λπ+π−e+νe ) < 3.9 × 10−4 and B(Λ + c → pK0Sπ−e+νe ) < 3.3 × 10−4 at the 90% confidence level, respectively.
Using (1.0087±0.0044)×1010 𝐽/𝜓 events collected by the BESIII detector at the BEPCII collider, we report the first search for the baryon and lepton number violating decays Ξ0→𝐾−𝑒+ with Δ(𝐵−𝐿)=0 and Ξ0→𝐾+𝑒− with |Δ(𝐵−𝐿)|=2, where 𝐵 (𝐿) is the baryon (lepton) number. While no signal is observed, the upper limits on the branching fractions of these two decays are set to ℬ(Ξ0→𝐾−𝑒+)<3.6×10−6 and ℬ(Ξ0→𝐾+𝑒−)<1.9×10−6 at the 90% confidence level, respectively. These results offer a direct probe of baryon number violating interactions involving a strange quark.
Based on (10.09±0.04)×109 J/ψ events collected with the BESIII detector operating at the BEPCII collider, a partial wave analysis of the decay J/ψ→ϕπ0η is performed. We observe for the first time two new structures on the ϕη invariant mass distribution, with statistical significances of 24.0σ and 16.9σ; the first with JPC = 1+−, mass M = (1911 ± 6 (stat.) ± 14 (sys.))~MeV/c2, and width Γ= (149 ± 12 (stat.) ± 23 (sys.))~MeV, the second with JPC = 1−−, mass M = (1996 ± 11 (stat.) ± 30 (sys.))~MeV/c2, and width Γ = (148 ± 16 (stat.) ± 66 (sys.))~MeV. These measurements provide important input for the strangeonium spectrum. In addition, the f0(980)−a0(980)0 mixing signal in J/ψ→ϕf0(980)→ϕa0(980)0 and the corresponding electromagnetic decay J/ψ→ϕa0(980)0 are measured with improved precision, providing crucial information to understand the nature of a0(980)0 and f0(980).
Ein intaktes Arbeitsgedächtnis ermöglicht es, Informationen, z.B. visuellen oder auditorischen Ursprungs temporär zu speichern, zu manipulieren und weiterzuverarbeiten. Es bildet die Grundlage zum Lernen, zum Begreifen und zum Verstehen von Sprache und somit die Grundlage zum tagtäglichen Funktionieren.
Beeinträchtigungen des Arbeitsgedächtnisses sind mit schlechten (Arbeits-) Leistungen, eingeschränkter zwischenmenschlicher Kommunikation, niedrigerem gesellschaftlichem Funktionsniveau und Arbeitslosigkeit vergesellschaftet und somit folgenschwer.
Psychiatrische Erkrankungen aus dem schizophrenen Spektrum, die unipolare Depression oder das Aufmerksamkeitsdefizit-Hyperaktivitätssyndrom (ADHS) gehen gehäuft mit kognitiven Beeinträchtigungen einher. Auch die bipolare affektive Störung zählt zu den psychiatrischen Erkrankungen, die mit kognitiver Beeinträchtigung assoziiert ist.
Das Ziel der Studie war es, darzustellen, dass kognitive Einschränkungen von Patienten, die an einer bipolaren affektiven Störung leiden, unter den exekutiven Funktionen insbesondere das Arbeitsgedächtnis betreffen und diese auch in euthymer Stimmungslage zu erfassen sind.
Hierzu wurde mittels einer Aufgabe zur Farbveränderung vier verschiedener Kreise, die um ein zentral platziertes, schwarzes Kreuz angeordnet waren, das visuelle Arbeitsgedächtnis anhand der Merkfähigkeit der Patienten, deren euthyme Stimmungslage mit den Ratingskalen MADRS und YMRS bestätigt wurde, im Vergleich zu einer Gruppe gesunder Kontrollprobanden, die mit der Patientengruppe in den Faktoren Alter, Geschlechterverteilung, prämorbide Intelligenz, Schulbildung und Händigkeit vergleichbar war, überprüft.
Anhand der erzielten Ergebnisse wurde die Arbeitsgedächtniskapazität K nach Pashler bestimmt. Es ergab sich eine bei mittlerer Effektstärke signifikant geringere Arbeitsgedächtniskapazität in der Gruppe der remittierten Patienten mit bipolarer affektiver Störung im Vergleich zur Kontrollgruppe gesunder Probanden.
Ein Einfluss der zum Zeitpunkt der Testung in der Patientengruppe angewandten Psychopharmaka auf die Arbeitsgedächtniskapazität konnte ausgeschlossen werden, sodass die ermittelten Defizite nicht als eine Form von Medikamentennebenwirkungen erklärt werden konnten. Interessanterweise betrug die mediane Erkrankungsdauer in der Patientengruppe drei Jahre, sodass davon auszugehen ist, dass die Ausprägung von Defiziten des Arbeitsgedächtnisses keinen langen Krankheitsverlauf bedingt, sondern bereits zu Beginn der Erkrankung vorhanden sein könnte.
Somit konnte die Studie darlegen, dass kognitive Defizite, insbesondere Störungen des Arbeitsgedächtnisses mit daraus resultierender signifikant erniedrigter Arbeitsgedächtniskapazität, bei Patienten mit bipolarer affektiver Störung in euthymer Stimmungslage bereits zu einem frühen Zeitpunkt des Krankheitsverlaufs bestehen, die eine Folge der Erkrankung selbst sind und keine Nebenwirkung von psychopharmazeutischer Medikation darstellen. Den Grund für das Auftreten kognitiver Defizite bei Patienten mit bipolarer affektiver Störung liefert diese Studie nicht, sie impliziert dennoch, dass das Verständnis und die Berücksichtigung kognitiver Störungen bei der bipolaren affektiven Störung zukünftig ein wichtiges Therapieziel darstellen sollte um das funktionelle Outcome von Patienten, die an dieser Störung leiden, entscheidend zu verbessern und somit eine Teilnahme am tagtäglichen Funktionieren weiterhin ermöglicht wird.
In die Zukunft blickend sollten unsere Ergebnisse mithilfe weiterer Untersuchungen validiert werden, insbesondere in Bezug auf genetische Komponenten, die die Arbeitsgedächtniskapazität regulieren. Es sollten Faktoren identifiziert werden, die eine reduzierte Arbeitsgedächtniskapazität bei Patienten mit bipolarer affektiver Störung bedingen. Die vorliegende Studie beantwortet nämlich nicht die Frage, wie genetische Faktoren und Umweltfaktoren die Arbeitsgedächtniskapazität auf kognitiver und neurophysiologischer Ebene beeinflussen könnten.
Angesichts der erwähnten Relevanz eines intakten Arbeitsgedächtnisses für die Funktionsfähigkeit der Patienten sollten zukünftige Studien prüfen, ob prokognitive Interventionen wie die kognitive Remediation oder sogar medikamentöse Therapieoptionen diese Defizite verbessern könnten.
Metastatic rhabdomyosarcoma (RMS) is one of the most challenging tumor entities in pediatric oncology caused by treatment resistances and immune escape. Novel chimeric antigen receptor (CAR) immunotherapies as specific, effective and safe treatment provide antitumor cytotoxicity by soluble factors and ligands/receptor signals. Besides its intrinsic potential as innate immune cell the ErbB2-sprecific CAR-engineered natural killer (NK)-92 cell line NK-92/5.28.z also provides CAR-mediated cytotoxicity, resulting in a high lytic capacity against 2D and 3D RMS cell structures in vitro. Also in a xenograft model using immune deficient NOD/Scid/IL2Rγ-/- (NSG) mice inhibited NK-92/5.28.z the tumor growth as long as the cells were administered and therefore prolonged the survival of the animals. The NK-92/5.28.z were distributed by the blood circulation and subsequently infiltrated the tumor tissue. Due to the malignant origin of the NK-92 cell line the cells must be irradiated prior to the use in patients. While the irradiation hampered the proliferation of NK-92/5.28.z cells, the cytotoxicity against RMS cells in vitro is retained for at least 24 hours. In the xenograft model irradiated NK-92/5.28.z cells inhibited the tumor growth but to a lower extent than untreated cells, as irradiated cells have only a limited life span in vivo no durable persistence and remission was achieved. Therefore, combinatorial approaches were focused and while blocking of the PD-1/PD-L1 axis did not resulted in a significantly enhanced tumor cell lysis, the combinatorial treatment with proteasome inhibitor bortezomib exhibited a significant enhanced cytotoxicity against RMS cells at least in vitro. Bortezomib itself induces caspase mediated apoptosis and also the upregulates the expression of TRAIL receptor DR5. The corresponding ligand TRAIL is expressed on the surface of the NK-92/5.28.z and pursuing experiments with purified TRAIL and bortezomib revealed a synergism. NK-92/5.28.z as an off-the-shelf product is therefore feasible for the therapy of metastatic RMS, but it might be necessary to support the cytotoxicity by additive agents like proteasome inhibitor bortezomib to archive durable remission.
Another cell population suitable for RMS CAR-immunotherapy are cytokine induced killer (CIK) cells, a heterogenous cell population generated from autologous PBMCs consisting of T, NK and T-NK cells. Lentivirally transduced ErbB2-specific CAR-CIK cells were previously shown to inhibit the tumor engraftment in a RMS xenograft model. However, lentiviral transduced adoptive immunotherapies bear risks for the transfer in patients, therefore the Sleeping Beauty Transposon System (SBTS) as a non-viral method, which integrates the CAR coding DNA by a cut-and-paste mechanism from a minicircle (MC) into the CIK cells genome is more feasible for the generation of CAR-CIK cells. The Sleeping beauty transposase mRNA and the MC were transferred in the cell by nucleofection, different factors influence the transfection efficiency and viability of the CIK cells in this harsh procedure. In preliminary experiments with MC Venus, a MC encoding eGFP, the highest transfection efficiency with the best proliferative capacity was achieved with cells on day 3 of CIK culture and without the addition of autologous monocytes as feeder cells. For the CAR construct the protocol was further improved by adjusting crucial factors, for this construct the best results were achieved on day 0, without irradiated PBMCs as feeder cells and cultivation in X-Vivo10 medium supplemented with human fresh frozen plasma. The X-Vivo10 medium enhanced the percentage of NK- and T-NK cells significantly compared to CAR-CIK cells cultured in RPMI. Since the gene transfer by SBTS resulted in CAR-CIK cells stably expressing a CAR in all subpopulations, resulting in a significantly enhanced cytotoxicity against RMS cells in vitro, these cells were compared to lentiviral transduced CAR-CIK cells in vitro and in vivo. While the SBTS CAR-CIK cells were superior to viral CAR-CIK cells in 2D short-term assays, the viral cells showed higher lytic capacity in 3D spheroid long-term assays. In a RMS xenograft model lentiviral CAR-CIK cells significantly prolonged the survival of mice and persisted, whereas SBTS CAR-CIKs did not favor the overall survival compared to untreated controls and also did not persist. Phenotypic analysis revealed a highly cytotoxic CD8+ and late effector memory dominant phenotype for SBTS CAR-CIK cells supporting short-term cytotoxicity but also more prone for exhaustion, while viral CAR-CIK cells showed a more balanced phenotype for memory and cytotoxicity. Therefore, the SBTS is feasible for the ErbB2-CAR gene transfer in CAR-CIK resulting in a stable CAR-expression with high short-term cytotoxicity, but these cells are also more prone to exhaustion and the protocol might be adapted further to prevent this limitation for in vivo application.
This work underlines the hard-to-treat characteristics of metastatic RMS, but also shows some approaches for further evaluation like the combination of NK-92/5.28.z cells with bortezomib and the feasibility of the generation of CAR-CIK cells via SBTS.
First study of reaction Ξ⁰n → Ξ⁻ p using Ξ⁰-nucleus scattering at an electron-positron collider
(2023)
Using ð1.0087 0.0044Þ × 1010 J=ψ events collected with the BESIII detector at the BEPCII storage ring, the process Ξ0n → Ξ−p is studied, where the Ξ0 baryon is produced in the process J=ψ → Ξ0Ξ¯ 0 and the neutron is a component of the 9 Be, 12C, and 197Au nuclei in the beam pipe. A clear signal is observed with a statistical significance of 7.1σ. The cross section of the reaction Ξ0 þ 9 Be → Ξ− þ p þ 8 Be is determined to be σðΞ0 þ 9 Be → Ξ− þ p þ 8 BeÞ¼ð22.1 5.3stat 4.5sysÞ mb at the Ξ0 momentum of 0.818 GeV=c, where the first uncertainty is statistical and the second is systematic. No significant H-dibaryon signal is observed in the Ξ−p final state. This is the first study of hyperon-nucleon interactions in electron-positron collisions and opens up a new direction for such research.
Based on (10.09±0.04)×109 J/ψ events collected with the BESIII detector operating at the BEPCII collider, a partial wave analysis of the decay J/ψ→ϕπ0η is performed. We observe for the first time two new structures on the ϕη invariant mass distribution, with statistical significances of 24.0σ and 16.9σ; the first with JPC = 1+−, mass M = (1911 ± 6 (stat.) ± 14 (sys.))~MeV/c2, and width Γ= (149 ± 12 (stat.) ± 23 (sys.))~MeV, the second with JPC = 1−−, mass M = (1996 ± 11 (stat.) ± 30 (sys.))~MeV/c2, and width Γ = (148 ± 16 (stat.) ± 66 (sys.))~MeV. These measurements provide important input for the strangeonium spectrum. In addition, the f0(980)−a0(980)0 mixing signal in J/ψ→ϕf0(980)→ϕa0(980)0 and the corresponding electromagnetic decay J/ψ→ϕa0(980)0 are measured with improved precision, providing crucial information to understand the nature of a0(980)0 and f0(980).
Precision measurements of the semileptonic decays 𝐷+𝑠→𝜂𝑒+𝜈𝑒 and 𝐷+𝑠→𝜂′𝑒+𝜈𝑒 are performed with 7.33 fb−1 of 𝑒+𝑒− collision data collected at center-of-mass energies between 4.128 and 4.226 GeV with the BESIII detector. The branching fractions obtained are ℬ(𝐷+𝑠→𝜂𝑒+𝜈𝑒) = (2.255±0.039stat±0.051syst)% and ℬ(𝐷+𝑠→𝜂′𝑒+𝜈𝑒)=(0.810±0.038stat±0.024syst)%. Combining these results with the ℬ(𝐷+→𝜂𝑒+𝜈𝑒) and ℬ(𝐷+→𝜂′𝑒+𝜈𝑒) obtained from previous BESIII measurements, the 𝜂−𝜂′ mixing angle in the quark flavor basis is determined to be 𝜙P=(40.0±2.0stat±0.6syst)°. Moreover, from the fits to the partial decay rates of 𝐷+𝑠→𝜂𝑒+𝜈𝑒 and 𝐷+𝑠→𝜂′𝑒+𝜈𝑒, the products of the hadronic transition form factors 𝑓𝜂(′)+(0) and the modulus of the 𝑐→𝑠 Cabibbo-Kobayashi-Maskawa matrix element |𝑉𝑐𝑠| are determined by using different hadronic transition form factor parametrizations. Based on the two-parameter series expansion, the products 𝑓𝜂+(0)|𝑉𝑐𝑠| = 0.4519±0.0071stat±0.0065syst and 𝑓𝜂′+(0)|𝑉𝑐𝑠| = 0.525±0.024stat±0.009syst are extracted. All results determined in this work supersede those measured in the previous BESIII analyses based on the 3.19 fb−1 subsample of data at 4.178 GeV.
The process e+e−→Σ+Σ¯− is studied from threshold up to 3.04 GeV/c2 via the initial-state radiation technique using data with an integrated luminosity of 12.0 fb−1, collected at center-of-mass energies between 3.773 and 4.258 GeV with the BESIII detector at the BEPCII collider. The pair production cross sections and the effective form factors of Σ are measured in eleven Σ+Σ¯− invariant mass intervals from threshold to 3.04 GeV/c2. The results are consistent with the previous results from Belle and BESIII. Furthermore, the branching fractions of the decays J/ψ→Σ+Σ¯− and ψ(3686)→Σ+Σ¯− are determined and the obtained results are consistent with the previous results of BESIII.
With data samples collected with the BESIII detector at seven energy points at √s = 3.68 − 3.71 GeV, corresponding to an integrated luminosity of 333 pb−1, we present a study of the Λ transverse polarization in the e+e− → ΛΛ¯ reaction. The signifcance of polarization by combining the seven energy points is found to be 2.6σ including the systematic uncertainty, which implies a non-zero phase between the transition amplitudes of the ΛΛ¯ helicity states. The modulus ratio and the relative phase of EM-psionic form factors combined with all energy points are measured to be RΨ = 0.71+0.10−0.10 ± 0.03 and ∆ΦΨ = 23+8.8−8.0 ± 1.6◦, where the frst uncertainties are statistical and the second systematic.
We present the first observation of the singly Cabibbo-suppressed decay Λ+c→ΛK+π0 with a significance of 5.7σ and the first evidence of Λ+c→ΛK+π+π− decay with a significance of 3.1σ, based on e+e− annihilation data recorded by the BESIII detector at the BEPCII collider. The data correspond to an integrated luminosity of 6.4 fb−1, in the center-of-mass energy range from 4.600 GeV to 4.950 GeV. We determine the branching fractions of Λ+c→ΛK+π0 and Λ+c→ΛK+π+π− relative to their Cabibbo-favored counterparts to be B(Λ+c→ΛK+π0)B(Λ+c→Λπ+π0)=(2.09±0.39stat.±0.07syst.)×10−2 and B(Λ+c→ΛK+π+π−)B(Λ+c→Λπ+π+π−)=(1.13±0.41stat.±0.06syst.)×10−2, respectively. Moreover, by combining our measured result with the world average of B(Λ+c→Λπ+π0), we obtain the branching fraction B(Λ+c→ΛK+π0)=(1.49±0.27stat.±0.05syst.±0.08ref.)×10−3. This result significantly departs from theoretical predictions based on quark SU(3) flavor symmetry, which is underpinned by the presumption of meson pair S-wave amplitude dominance.
We search for an axion-like particle (ALP) a through the process ψ(3686)→π+π−J/ψ, J/ψ→γa, a→γγ in a data sample of (2.71±0.01)×109 ψ(3686) events collected by the BESIII detector. No significant ALP signal is observed over the expected background, and the upper limits on the branching fraction of the decay J/ψ→γa and the ALP-photon coupling constant gaγγ are set at 95% confidence level in the mass range of 0.165≤ma≤2.84GeV/c2. The limits on B(J/ψ→γa) range from 8.3×10−8 to 1.8×10−6 over the search region, and the constraints on the ALP-photon coupling are the most stringent to date for 0.165≤ma≤1.468GeV/c2.
Using a sample of (10087±44)×106 J/ψ events, which is about fifty times larger than that was previously analyzed, a further investigation on the J/ψ→γ3(π+π−) decay is performed. A significant distortion at 1.84 GeV/c2 in the line-shape of the 3(π+π−) invariant mass spectrum is observed for the first time, which is analogous to the behavior of X(1835) and could be resolved by two overlapping resonant structures, X(1840) and X(1880). The new state X(1880) is observed with a statistical significance of 14.7σ. The mass and width of X(1880) are determined to be 1882.1±1.7±0.7 MeV/c2 and 30.7±5.5±2.4 MeV, respectively, which indicates the existence of a pp¯ bound state.
The Cabbibo-favored decay Λ+c→Ξ0K+π0 is studied for the first time using 6.1 fb−1 of e+e− collision data at center-of-mass energies between 4.600 and 4.840 GeV, collected with the BESIII detector at the BEPCII collider. With a double-tag method, the branching fraction of the three-body decay Λ+c→Ξ0K+π0 is measured to be (7.79±1.46±0.71)×10−3, where the first and second uncertainties are statistical and systematic, respectively. The branching fraction of the two-body decay Λ+c→Ξ(1530)0K+ is (5.99±1.04±0.29)×10−3, which is consistent with the previous result of (5.02±0.99±0.31)×10−3. In addition, the upper limit on the branching fraction of the doubly Cabbibo-suppressed decay Λ+c→nK+π0 is 7.1×10−4 at the 90% confidence level. The upper limits on the branching fractions of Λ+c→Σ0K+π0 and ΛK+π0 are also determined to be 1.8×10−3 and 2.0×10−3, respectively.
The Cabbibo-favored decay Λ+c→Ξ0K+π0 is studied for the first time using 6.1 fb−1 of e+e− collision data at center-of-mass energies between 4.600 and 4.840 GeV, collected with the BESIII detector at the BEPCII collider. With a double-tag method, the branching fraction of the three-body decay Λ+c→Ξ0K+π0 is measured to be (7.79±1.46±0.71)×10−3, where the first and second uncertainties are statistical and systematic, respectively. The branching fraction of the two-body decay Λ+c→Ξ(1530)0K+ is (5.99±1.04±0.29)×10−3, which is consistent with the previous result of (5.02±0.99±0.31)×10−3. In addition, the upper limit on the branching fraction of the doubly Cabbibo-suppressed decay Λ+c→nK+π0 is 7.1×10−4 at the 90% confidence level. The upper limits on the branching fractions of Λ+c→Σ0K+π0 and ΛK+π0 are also determined to be 1.8×10−3 and 2.0×10−3, respectively.
Based on 4.5 fb−1 data taken at seven center-of-mass energies ranging from 4.600 to 4.699 GeV with the BESIII detector at the BEPCII collider, we measure the branching fractions of Λ + c → Σ + + hadrons relative to Λ + c → Σ +π +π −. Combining with the world average branching fraction of Λ + c → Σ +π +π −, their branching fractions are measured to be (0.377 ± 0.042 ± 0.020 ± 0.021)% for Λ + c → Σ +K+K−, (0.200 ± 0.023 ± 0.011 ± 0.011)% for Λ + c → Σ+K+π−, (0.414 ± 0.080 ± 0.030 ± 0.023)% for Λ + c → Σ +φ and (0.197 ± 0.036 ± 0.009 ± 0.011)% for Λ + c → Σ +K+K−(non-φ). In all the above results, the first uncertainties are statistical, the second are systematic and the third are from external input of the branching fraction of Λ + c → Σ +π +π −. Since no signal for Λ + c → Σ +K+π−π 0 is observed, the upper limit of its branching fraction is determined to be 0.13% at the 90% confidence level.
Evidence for the singly Cabibbo suppressed decay Λ+c→pπ0 is reported for the first time with a statistical significance of 3.7σ based on 6.0 fb−1 of e+e− collision data collected at center-of-mass energies between 4.600 and 4.843 GeV with the BESIII detector at the BEPCII collider. The absolute branching fraction of Λ+c→pπ0 is measured to be (1.56+0.72−0.58±0.20)×10−4. Combining with the branching fraction of Λ+c→nπ+, (6.6±1.2±0.4)×10−4, the ratio of the branching fractions Λ+c→nπ+ and Λ+c→pπ0 is calculated to be 4.2+2.2−1.9; this is an important input for the understanding of the decay mechanisms of charmed baryons. In addition, the absolute branching fraction of Λ+c→pη is measured to be (1.63±0.31stat±0.11syst)×10−3, which is consistent with previous measurements.
Quantum-correlated 𝐷¯𝐷 pairs collected by the BESIII experiment at the 𝜓(3770) resonance corresponding to an integrated luminosity of 2.93 fb−1 are used to study the 𝐷0→𝐾0𝑆𝜋+𝜋−𝜋0 decay mode. The 𝐶𝑃-even fraction of 𝐷0→𝐾0𝑆𝜋+𝜋−𝜋0 decays is determined to be 0.235±0.010±0.002, where the first uncertainty is statistical and the second is systematic.
The epitranscriptome embodies many new and largely unexplored functions of RNA. A major roadblock in the epitranscriptomics field is the lack of transcriptome-wide methods to detect more than a single RNA modification type at a time, identify RNA modifications in individual molecules, and estimate modification stoichiometry accurately. We address these issues with CHEUI (CH3 (methylation) Estimation Using Ionic current), a new method that concurrently detects N6-methyladenosine (m6A) and 5-methylcytidine (m5C) in individual RNA molecules from the same sample, as well as differential methylation between any two conditions. CHEUI processes observed and expected nanopore direct RNA sequencing signals with convolutional neural networks to achieve high single-molecule accuracy and outperforms other methods in detecting m6A and m5C sites and quantifying their stoichiometry. CHEUI’s unique capability to identify two modification types in the same sample reveals a non-random co-occurrence of m6A and m5C in mRNA transcripts in cell lines and tissues. CHEUI unlocks an unprecedented potential to study RNA modification configurations and discover new epitranscriptome functions.
Parallel global edge switching for the uniform sampling of simple graphs with prescribed degrees
(2023)
The uniform sampling of simple graphs matching a prescribed degree sequence is an important tool in network science, e.g. to construct graph generators or null-models. Here, the Edge Switching Markov Chain (ES-MC) is a common choice. Given an arbitrary simple graph with the required degree sequence, ES-MC carries out a large number of small changes, called edge switches, to eventually obtain a uniform sample. In practice, reasonably short runs efficiently yield approximate uniform samples.
In this work, we study the problem of executing edge switches in parallel. We discuss parallelizations of ES-MC, but find that this approach suffers from complex dependencies between edge switches. For this reason, we propose the Global Edge Switching Markov Chain (G-ES-MC), an ES-MC variant with simpler dependencies. We show that G-ES-MC converges to the uniform distribution and design shared-memory parallel algorithms for ES-MC and G-ES-MC. In an empirical evaluation, we provide evidence that G-ES-MC requires not more switches than ES-MC (and often fewer), and demonstrate the efficiency and scalability of our parallel G-ES-MC implementation.
The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon γdir and neutral-pion (π0) triggers in p+p and central Au+Au collisions at sNN−−−√=200 GeV over a broad kinematic range, for jet resolution parameters R=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The magnitude of suppression is similar for γdir- and π0-triggered data, which constrains the color-charge and path-length dependence of jet quenching. Theoretical model calculations incorporating jet quenching do not fully describe the measurements.
Einleitung: Allergisches Asthma bronchiale ist eine chronische Atemwegserkrankung, deren Prävalenz zunimmt. Angesichts der immensen gesellschaftlichen und individuellen Belastung durch Asthma ist es dringend erforderlich, neue Strategien zur Behandlung der Krankheit zu entwickeln. Immunologisch ist allergisches Asthma durch ein Ungleichgewicht zwischen TH2-Zellen und TH1-Zellen gekennzeichnet, das durch regulatorische T-Zellen (Tregs) reguliert wird. Tregalizumab ist ein monoklonaler IgG-Antikörper, der Tregs selektiv aktiviert. Ziel der vorliegenden Arbeit war es daher, die Wirkung von Tregalizumab auf die allergeninduzierte allergische Entzündung bei Patienten mit Hausstaubmilbenallergie anhand eines bronchialen Provokationsmodells zu untersuchen.
Methoden: In einer prospektiven, randomisierten, doppelblinden und placebokontrollierten Studie wurden 42 Probanden mit allergischem Asthma und Hausstaubmilbenallergie zwölf Wochen lang mit Tregalizumab 100 mg oder Placebo behandelt. Bronchiale Provokation mit HSM wurde vor (V4) und nach (V17) Tregalizumab-Gabe durchgeführt. Induziertes Sputum (Visite V5, V16, V18) und peripheres Blut (Visite V4, V5, V18) wurden entnommen und Zelldifferenzierung, Zytokine und Transkriptionsfaktoren wurden durch Mikroskopie, Durchflusszytometrie bzw. RT-PCR bewertet.
Ergebnisse: Sowohl in der Verum- als auch in der Placebogruppe zeigte sich zwischen Visite V5 (24 Stunden nach Provokation) und vier Wochen nach Provokation bei Visite V16 (p<0,05) ein signifikanter Rückgang des Anteils eosinophiler Granulozyten (wie auch des ECP-Levels). Interessanterweise konnte bei V18 (24 Stunden nach Provokation) nur in der Placebogruppe ein signifikanter Anstieg beobachtet werden (p<0,01). Die Konzentration des TH-2-Zytokins IL-5 nahm zwischen V5 und V16 in der Verumgruppe signifikant ab (p<0,05). Zwischen V16 und V18 konnte wiederum nur in der Placebogruppe ein signifikanter Anstieg festgestellt werden (p<0,01). Dieser spätere Effekt wurde auch auf Protein- und Transkriptionsebene und im peripheren Blut sowie bei der Expression des Transkriptionsfaktors FoxP3 gefunden. Auf der Ebene der TH-1-Zytokine konnten keine signifikanten Veränderungen festgestellt werden.
Diskussion: Der Anteil eosinophiler Granulozyten, die Konzentration von IL-5 in Blut und Sputum sowie die Konzentration von ECP im Sputum haben sich als gute Parameter zur Beurteilung der Entzündungsreaktion bei unseren Studienteilnehmern erwiesen. Wir haben gezeigt, dass allergische Entzündungen, die durch das Provokationsmodell verursacht wurden, durch die analysierten Parameter im Sputum, aber auch im Blut gut überwacht werden konnten. Ein klinischer Effekt von Tregalizumab konnte in dieser Studie jedoch nicht festgestellt werden und dieses Ergebnis stimmt gut mit der Analyse der Entzündungsparameter im induzierten Sputum überein.
Flow coefficients (v2 and v3) are measured in high-multiplicity p+Au, d+Au, and 3He+Au collisions at a center-of-mass energy of √sNN = 200 GeV using the STAR detector. The measurements are conducted using two-particle correlations with a pseudorapidity requirement of |η|< 0.9 and a pair gap of |Δη|>1.0. The primary focus of this paper is on the analysis procedures and methods employed, especially the subtraction of non-flow contributions. Four well-established non-flow subtraction methods are applied to determine vn, and their validity is verified using the HIJING event generator. The vn values are compared across the three collision systems at similar multiplicities, which allows for cancellation of final state effects and isolation of the impact of the initial geometry. While the v2 values display differences among these collision systems, the v3 values are largely similar, consistent with the expectations of subnucleon fluctuations in the initial geometry. The ordering of vn differs quantitatively from previous measurements obtained using two-particle correlations with a larger rapidity gap; this difference could be partially attributed to the effects of flow decorrelations in the rapidity direction.
We report a measurement of exclusive J/ψ photoproduction in Au+Au ultra-peripheral collisions at sNN−−−√=200 GeV using the STAR detector. For the first time, i) the rapidity correlation between J/ψ photoproduction and neutron emission from nuclear breakups has been experimentally measured; ii) nuclear suppression factors are measured for both the coherent and incoherent J/ψ production. At photon-nucleon center-of-mass energy of 25.0 GeV, the coherent and incoherent J/ψ cross sections of Au nuclei are found to be 71±10% and 36±7%, respectively, of that of free protons. The stronger suppression observed in the incoherent production provides a new experimental handle to study the initial-state parton density in heavy nuclei. Data are compared with theoretical models quantitatively.
We report results on an elastic cross section measurement in proton-proton collisions at a center-of-mass energy s√=510 GeV, obtained with the Roman Pot setup of the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The elastic differential cross section is measured in the four-momentum transfer squared range 0.23≤−t≤0.67 GeV2. We find that a constant slope B does not fit the data in the aforementioned t range, and we obtain a much better fit using a second-order polynomial for B(t). The t dependence of B is determined using six subintervals of t in the STAR measured t range, and is in good agreement with the phenomenological models. The measured elastic differential cross section dσ/dt agrees well with the results obtained at s√=546 GeV for proton--antiproton collisions by the UA4 experiment. We also determine that the integrated elastic cross section within the STAR t-range is σfidel=462.1±0.9(stat.)±1.1(syst.)±11.6(scale) μb.
We measure triangular flow relative to the reaction plane at 3 GeV center-of-mass energy in Au+Au collisions at RHIC. A significant v3 signal is observed for protons, whose magnitude increases for higher rapidity, higher transverse momentum, and more peripheral collisions. The triangular flow is essentially rapidity-odd with a rapidity slope at mid-rapidity, dv3/dy|(y=0), opposite in sign compared to the slope for directed flow. No significant v3 signal is observed for charged pions and kaons. Comparisons with models suggest that a mean field potential is required to describe these results, and that the triangular shape of the participant nucleons is the result of stopping and nuclear geometry.
The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon γdir and neutral-pion (π0) triggers in p+p and central Au+Au collisions at sNN−−−√=200 GeV over a broad kinematic range, for jet resolution parameters R=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The magnitude of suppression is similar for γdir- and π0-triggered data, which constrains the color-charge and path-length dependence of jet quenching. Theoretical model calculations incorporating jet quenching do not fully describe the measurements.
The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon γdir and neutral-pion (π0) triggers in p+p and central Au+Au collisions at √sNN=200 GeV over a broad kinematic range, for jet resolution parameters R=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The magnitude of suppression is similar for γdir- and π0-triggered data, which constrains the color-charge and path-length dependence of jet quenching. Theoretical model calculations incorporating jet quenching do not fully describe the measurements.
The longitudinal and transverse spin transfers to Λ (Λ¯¯¯¯) hyperons in polarized proton-proton collisions are expected to be sensitive to the helicity and transversity distributions, respectively, of (anti-)strange quarks in the proton, and to the corresponding polarized fragmentation functions. We report improved measurements of the longitudinal spin transfer coefficient, DLL, and the transverse spin transfer coefficient, DTT, to Λ and Λ¯¯¯¯ in polarized proton-proton collisions at √s = 200 GeV by the STAR experiment at RHIC. The data set includes longitudinally polarized proton-proton collisions with an integrated luminosity of 52 pb−1, and transversely polarized proton-proton collisions with a similar integrated luminosity. Both data sets have about twice the statistics of previous results and cover a kinematic range of |ηΛ(Λ¯¯¯¯)| < 1.2 and transverse momentum pT,Λ(Λ¯¯¯¯) up to 8 GeV/c. We also report the first measurements of the hyperon spin transfer coefficients DLL and DTT as a function of the fractional jet momentum z carried by the hyperon, which can provide more direct constraints on the polarized fragmentation functions.
We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity (|y|< 0.7) in Au+Au collisions at sNN−−−√=200 GeV. Invariant yields of HFEs are measured for the transverse momentum range of 3.5<pT<9 GeV/c in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in p+p collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.
We report a measurement of exclusive J/ψ photoproduction in Au+Au ultra-peripheral collisions at sNN−−−√=200 GeV using the STAR detector. For the first time, i) the rapidity correlation between J/ψ photoproduction and neutron emission from nuclear breakups has been experimentally measured; ii) nuclear suppression factors are measured for both the coherent and incoherent J/ψ production. At photon-nucleon center-of-mass energy of 25.0 GeV, the coherent and incoherent J/ψ cross sections of Au nuclei are found to be 71±10% and 36±7%, respectively, of that of free protons. The stronger suppression observed in the incoherent production provides a new experimental handle to study the initial-state parton density in heavy nuclei. Data are compared with theoretical models quantitatively.
Measurements of exclusive J/ψ, ψ(2s), and electron-positron (e+e−) pair photoproduction in Au+Au ultra-peripheral collisions are reported by the STAR experiment at √sNN=200 GeV. We report several first measurements at the Relativistic Heavy-Ion Collider, which are i) J/ψ photoproduction with large momentum transfer up to 2.2 (GeV/c)2, ii) coherent J/ψ photoproduction associated with neutron emissions from nuclear breakup, iii) the rapidity dependence of incoherent J/ψ photoproduction, iv) the ψ(2s) photoproduction cross section at mid-rapidity, and v) e+e− pair photoproduction up to high invariant mass of 6 GeV/c2. For measurement ii), the coherent J/ψ total cross section of γ∗+Au→J/ψ+Au as a function of the center-of-mass energy Wγ∗N has been obtained without photon energy ambiguities. The data are quantitatively compared with the Monte Carlo models STARlight, Sartre, BeAGLE, and theoretical calculations of gluon saturation with color glass condensate, nuclear shadowing with leading twist approximation, Quantum Electrodynamics, and the Next-to-Leading Order perturbative QCD. At the photon-nucleon center-of-mass energy of 25.0 GeV, the coherent and incoherent J/ψ cross sections of Au nuclei are found to be 71±10% and 36±7%, respectively, of that of free protons. These data provide an important experimental constraint for nuclear parton distribution functions and a unique opportunity to advance the understanding of the nuclear modification effect at the top RHIC energy.
Production of protons and light nuclei in Au+Au collisions at √sNN = 3 GeV with the STAR detector
(2023)
We report the systematic measurement of protons and light nuclei production in Au+Au collisions at √sNN = 3 GeV by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The transverse momentum (pT) spectra of protons (p), deuterons (d), tritons (t), 3He, and 4He are measured from mid-rapidity to target rapidity for different collision centralities. We present the rapidity and centrality dependence of particle yields (dN/dy), average transverse momentum (⟨pT⟩), yield ratios (d/p, t/p,3He/p, 4He/p), as well as the coalescence parameters (B2, B3). The 4π yields for various particles are determined by utilizing the measured rapidity distributions, dN/dy. Furthermore, we present the energy, centrality, and rapidity dependence of the compound yield ratios (Np×Nt/N2d) and compare them with various model calculations. The physics implications of those results on the production mechanism of light nuclei and on QCD phase structure are discussed.
We report on the charged-particle multiplicity dependence of net-proton cumulant ratios up to sixth order from √s = 200 GeV p+p collisions at the Relativistic Heavy Ion Collider (RHIC). The measured ratios C4/C2, C5/C1, and C6/C2 decrease with increased charged-particle multiplicity and rapidity acceptance. Neither the Skellam baselines nor PYTHIA8 calculations account for the observed multiplicity dependence. In addition, the ratios C5/C1 and C6/C2 approach negative values in the highest-multiplicity events. The negative ratios in the most central p+p collisions at 200 GeV, similar to those observed in central Au+Au 200 GeV collisions, imply the formation of thermalized QCD matter.
We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity (|y|< 0.7) in Au+Au collisions at sNN−−−√=200 GeV. Invariant yields of HFEs are measured for the transverse momentum range of 3.5<pT<9 GeV/c in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in p+p collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.
For the search of the chiral magnetic effect (CME), STAR previously presented the results from isobar collisions (9644Ru+9644Ru, 9640Zr+9640Zr) obtained through a blind analysis. The ratio of results in Ru+Ru to Zr+Zr collisions for the CME-sensitive charge-dependent azimuthal correlator (Δγ), normalized by elliptic anisotropy (v2), was observed to be close to but systematically larger than the inverse multiplicity ratio. The background baseline for the isobar ratio, Y=(Δγ/v2)Ru(Δγ/v2)Zr, is naively expected to be (1/N)Ru(1/N)Zr; however, genuine two- and three-particle correlations are expected to alter it. We estimate the contributions to Y from those correlations, utilizing both the isobar data and HIJING simulations. After including those contributions, we arrive at a final background baseline for Y, which is consistent with the isobar data. We extract an upper limit for the CME fraction in the Δγ measurement of approximately 10% at a 95% confidence level on in isobar collisions at sNN−−−√=200 GeV.
Matter-antimatter asymmetry is a research topic of fundamental interest, as it is the basis for the existence of the matter world, which survived annihilation with antimatter in the early Universe. High energy nuclear collisions create conditions similar to the Universe microseconds after the Big Bang, with comparable amounts of matter and antimatter. Much of the antimatter created escapes the rapidly expanding fireball without annihilation, making such collisions an effective experimental tool to create heavy antimatter nuclear objects and study their properties. In this paper, we report the first observation of the antimatter hypernucleus 4Λ¯H¯¯¯¯, composed of an Λ¯, an antiproton and two antineutrons. The discovery was made through its two-body decay after production in ultrarelativistic heavy ion collisions by the STAR experiment at the Relativistic Heavy Ion Collider. In total, 15.6 candidate 4Λ¯H¯¯¯¯ antimatter hypernuclei are obtained with an estimated background count of 6.4. Lifetimes of the antihypernuclei 3Λ¯H¯¯¯¯ and 4Λ¯H¯¯¯¯ are measured and compared with lifetimes of their corresponding hypernuclei, testing the symmetry between matter and antimatter. Various production yield ratios among (anti)hypernuclei and (anti)nuclei are also measured and compared with theoretical model predictions, shedding light on their production mechanism.
Using 15.6 fb−1 of e+e− collision data collected at twenty-four center-of-mass energies from 4.0 to 4.6 GeV with the BESIII detector, the helicity amplitudes of the process e+e− → π+π−ω are analyzed for the first time. Born cross section measurements of two-body intermediate resonance states with statistical significance greater than 5σ are presented, such as f0(500), f0(980), f2(1270), f0(1370), b1(1235)±, and ρ(1450)±. In addition, evidence of a resonance state in e+e− → π+π−ω production is found. The mass of this state obtained by line shape fitting is about 4.2 GeV/c2, which is consistent with the production of ψ(4160) or Y(4220).
We present our recent results on antiheavy-antiheavy-light-light tetraquark systems using lattice QCD. Our study of the b¯b¯us four-quark system with quantum numbers JP=1+ and the b¯c¯ud four-quark systems with I(JP)=0(0+) and I(JP)=0(1+) utilizes scattering operators at the sink to improve the extraction of the low-lying energy levels. We found a bound state for b¯b¯us with Ebind,b¯b¯us=(−86±22±10)MeV, but no indication for a bound state in both b¯c¯ud channels. Moreover, we show preliminary results for b¯b¯ud with I(JP)=0(1+), where we used scattering operators both at the sink and the source. We found a bound state and determined its infinite-volume binding energy with a scattering analysis, resulting in Ebind,b¯b¯ud=(−103±8)MeV.
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.
In natural environments, background noise can degrade the integrity of acoustic signals, posing a problem for animals that rely on their vocalizations for communication and navigation. A simple behavioral strategy to combat acoustic interference would be to restrict call emissions to periods of low-amplitude or no noise. Using audio playback and computational tools for the automated detection of over 2.5 million vocalizations from groups of freely vocalizing bats, we show that bats (Carollia perspicillata) can dynamically adapt the timing of their calls to avoid acoustic jamming in both predictably and unpredictably patterned noise. This study demonstrates that bats spontaneously seek out temporal windows of opportunity for vocalizing in acoustically crowded environments, providing a mechanism for efficient echolocation and communication in cluttered acoustic landscapes.
Wahrnehmung wurde zu Beginn des 20. Jahrhunderts bestimmt als "Organ unseres ursprünglichen Welt-Erlebens." Das ursprüngliche Welterleben war das des Flaneurs, der mit allen Sinnen Umwelt wahrnimmt, um sich zu situieren und aus dieser Verortung Sicherheit und Anderssein zu gewinnen; die Verortung war aber auch über die Individualebene hinaus von politischer, sozialer, ökonomischer und kultureller Bedeutung. Man greift nicht zu hoch, wenn der Vormärz als Zeitspanne betrachtet wird, in der eine vollere Realität in sehr spezifischer Weise greifbar wurde. Die Vielschichtigkeit der Vormärz-Welt war dabei eine konstanter Innovation, die eine Initiierung jener Selbstbilder bedeutete, die über das Wahrnehmen bestätigt wurden, das selbst ein anderes geworden war. Nicht mehr informierte Wahrnehmung über die tautologisch so genannten sozialen Tatsachen; sie schuf diese vielmehr um und damit neu - das Organ des Welterlebens wirkte hier auf die Welt ein und musste Erlebnisse nicht mehr erleiden. Die Erfahrung der Welt-Erlebnisse bestand auch darin, die Sinne als sinnenöffnend zu sehen, indem die theoretische Vorrangstellung des Informationsaspekts der Wahrnehmung zurücktrat und Indices von Engagement, Eingreifen und Emanzipation deutlich werden konnten. Dies bedeutete, eine Form des "Wirklichkeitskontakts" zu suchen, die bisher nicht bestanden hatte. War der Kontakt vorher so geschehen, dass die Sinne eine bestätigende Funktion den sozialen und politischen Valeurs gegenüber einnahmen, die bezogen auf Emanzipationsprozesse und deren Möglichkeit einer Schließung gleichkam, öffnete nun die Veränderung der Wahrnehmung neue Formen des Wirklichkeitskontakts. In diesem Kontakt war vor allem entscheidend, dass nun die Bedingungen der Wahrnehmung ersichtlich wurden, sich als veränderbar auswiesen und nicht mehr im umfassenden Konstrukt "Wahrnehmung" aufgingen.
Wahrnehmung wurde zu Beginn des 20. Jahrhunderts bestimmt als "Organ unseres ursprünglichen Welt-Erlebens." Das ursprüngliche Welterleben war das des Flaneurs, der mit allen Sinnen Umwelt wahrnimmt, um sich zu situieren und aus dieser Verortung Sicherheit und Anderssein zu gewinnen; die Verortung war aber auch über die Individualebene hinaus von politischer, sozialer, ökonomischer und kultureller Bedeutung. Man greift nicht zu hoch, wenn der Vormärz als Zeitspanne betrachtet wird, in der eine vollere Realität in sehr spezifischer Weise greifbar wurde. Die Vielschichtigkeit der Vormärz-Welt war dabei eine konstanter Innovation, die eine Initiierung jener Selbstbilder bedeutete, die über das Wahrnehmen bestätigt wurden, das selbst ein anderes geworden war. Nicht mehr informierte Wahrnehmung über die tautologisch so genannten sozialen Tatsachen; sie schuf diese vielmehr um und damit neu - das Organ des Welterlebens wirkte hier auf die Welt ein und musste Erlebnisse nicht mehr erleiden. Die Erfahrung der Welt-Erlebnisse bestand auch darin, die Sinne als sinnenöffnend zu sehen, indem die theoretische Vorrangstellung des Informationsaspekts der Wahrnehmung zurücktrat und Indices von Engagement, Eingreifen und Emanzipation deutlich werden konnten. Dies bedeutete, eine Form des "Wirklichkeitskontakts" zu suchen, die bisher nicht bestanden hatte. War der Kontakt vorher so geschehen, dass die Sinne eine bestätigende Funktion den sozialen und politischen Valeurs gegenüber einnahmen, die bezogen auf Emanzipationsprozesse und deren Möglichkeit einer Schließung gleichkam, öffnete nun die Veränderung der Wahrnehmung neue Formen des Wirklichkeitskontakts. In diesem Kontakt war vor allem entscheidend, dass nun die Bedingungen der Wahrnehmung ersichtlich wurden, sich als veränderbar auswiesen und nicht mehr im umfassenden Konstrukt "Wahrnehmung" aufgingen.
Pericytes are capillary-associated mural cells involved in the maintenance and the stability of the vascular network. This thesis aims to investigate the role of pericytes in the heart in the context of ageing and disease. We highlight the malignant effects of the remodelling in the heart and stress the focus on the role of cardiac pericytes in this context. We show that ageing reduces pericyte coverage and that myocardial infarction (MI) causes an activation of these cells. Single-nuclei and single-cell RNA sequencing analysis of murine hearts further revealed that the expression of the Regulator of G-protein signalling 5 (Rgs5) is reduced in cardiac pericytes both in ageing and transiently at day 1 and day 3 after MI. The loss of RGS5 in pericytes drives an entropic state of these mural cells characterized by morphological changes, excessive extracellular deposition and enhanced Gaq mediated GPCR signalling. The deletion of RGS5 in pericytes causes cardiac systolic dysfunction, induces myocardial fibrosis, and drives the activation of cardiac fibroblasts in a TGFb-dependent manner. In conclusion, our results describe the importance of pericytes maintaining cardiac homeostasis, identify RGS5 as a key regulator of this process and propose pericytes as crucial mediators of cardiac fibrosis and possible therapeutic targets to prevent cardiovascular disease.
The prefrontal cortex (PFC) is considered the cognitive center of the mammalian brain. It is involved in a variety of cognitive functions such as decision making, working memory, goal-directed behavior, processing of emotions, flexible action selection, attention, and others (Fuster, 2015). In rodents, these functions are associated with the medial prefrontal cortex (mPFC). Experiments in mice and rats have shown that neurons in the mPFC are necessary for successful performance of many cognitive tasks. Moreover, measurements of neural activity in the mPFC show excitation or inhibition in different cells in relation to specific aspects of the tasks to be solved. To date, however, it is largely unknown whether prefrontal neurons are stably activated during the same behaviors within a task and whether similar aspects are represented by the same neurons in different tasks. In addition, it is unclear how specifically neurons are activated, for example, whether cells that are activated in response to reward are activated in a different task without reward in a different situation or remain inactive. To address these questions, we recorded the same neurons in the mPFC of mice over the course of several weeks while the animals performed various behaviors.
To do this, we expressed GCaMP6 in pyramidal neurons in the mPFC of mice. A small lens was implanted in the same location and a miniature microscope ("miniscope") was used to record neural activity. Later the extracted neurons got aligned based on their shape and position across multiple days and sessions. The mice performed five different behavioral tests while neural activity was measured: A spatial working memory test in a T-maze, exploration of the elevated plus maze (EPM), a novel object recognition (NO) test including free open field (OF) exploration, a social interaction (SI) test and discriminatory auditory fear conditioning (FC). Each task was repeated at least twice to check for stable task encoding across sessions. Behavioral performance and neural correlates to specific task events were similar to earlier studies across all tasks. We utilized generalized linear models (GLM) to determine which behavioral variables most strongly influence neural activity in the mPFC. The position of the mouse in the environment was found to explain most of the variance in neural activity, together with movement speed they were the strongest predictors of neural activity across all tasks. Reward time points in the working memory test, the conditioned stimulus after fear conditioning, or head direction in general were also strongly encoded in the mPFC.
Many of the recorded neurons showed a stable spatial activity profile across multiple sessions of the same task. Similarly, cells that coded for position in one task tended to code for position in other tasks. Not only did the same cells code for position across multiple tasks, but cells also coded for movement speed and head direction. This indicates that at least these general behavioral variables are each represented by the same neurons in the mPFC. Interestingly, the stability of position or speed coding did not depend on the time between two sessions, but only on whether it was within the same or across different tasks. Within the same task, stability was slightly higher than across different tasks.
To find out whether task-specific behavioral aspects were also stably encoded in the mPFC, difference scores as the difference in neural activity between two task aspects like left- and right-choice trials or exposed and enclosed locations were calculated. Many cells encoded these aspects stably across different sessions of each task. Both the left-right differences in the different phases of the working memory test, the open-closed-arm differences in the elevated plus maze, the different activity between center and corners in the open field, the social target-object differences in the social interaction test, and the differences between the two tones during fear conditioning were all stably encoded across the population of mPFC cells. Only the distinction between the novel and the familiar object during object recognition was not stably encoded, but also the preference for the novel object was not present in the second session of novel object exploration.
There was also an overlap in coding for different aspects within a task across multiple sessions. For example, cells stably encoded left-right differences in the T-maze between different sessions as a function of walking direction across different phases of working memory, an aspect that we could already show within one session (Vogel, Hahn et al., 2022). During fear conditioning, the same cells showed a discrimination between CS+ and CS- that also responded to the start of CS+.
Consistency in the neurons activity across different tasks was also found, but only between tasks with similar demands, the elevated plus-maze and free exploration of the open field. Cells that were more active in the open arms also showed more activity in the center of the open field and vice versa. This could be an indicator that the cells were coding for anxiety or exposure across those tasks, indicating that neurons in the mPFC also stably encode general task aspects independent of the specific environment. However, it remains unclear what exactly these neurons encode; in the case of a general fear signal, one would also expect activation during fear conditioning which could not be found.
Overall, we found that neurons in the mPFC of mice encoded multiple general behavioral variables across multiple tasks and task-specific variables were encoded stably within each of the tested tasks. However, we found little task-specific variables that were systematically encoded by the same neurons with the exception being the elevated plus-maze and open field exploration, two tasks with similar features.
Long non-coding RNAs are a very versatile class of molecules that can have important roles in regulating a cells function, including regulating other genes on the transcriptional level. One of these mechanisms is that RNA can directly interact with DNA thereby recruiting additional components such as proteins to these sites via an RNA:dsDNA triplex formation. We genetically deleted the triplex forming sequence (FendrrBox) from the lncRNA Fendrr in mice and found that this FendrrBox is partially required for Fendrr function in vivo. We found that the loss of the triplex forming site in developing lungs causes a dysregulation of gene programs associated with lung fibrosis. A set of these genes contain a triplex site directly at their promoter and are expressed in lung fibroblasts. We biophysically confirmed the formation of an RNA:dsDNA triplex with target promoters in vitro. We found that Fendrr with the Wnt signalling pathway regulates these genes, implicating that Fendrr synergizes with Wnt signalling in lung fibrosis.
Die Ergebnisse der Studie und die Diversität der Datenbanken ist groß.
Für 12 Datenbanken wurde ein Punktesystem mit elf Items entworfen, um die Qualität der einzelnen Datenbanken zu objektivieren. Keine Datenbank konnte alle Bewertungskriterien erfüllen. Der insgesamt schlechte Punktedurchschnitt ist ein Indikator für die Mängel der aktuell verfügbaren Datenbanken. Außerdem konnten wir einen Qualitätsunterschied zwischen kostenpflichtigen und kostenfreien Datenbanken beweisen und mussten im Zuge dieser Ergebnisse die Frage stellen, ob kostenfreie Datenbanken überhaupt nützlich sind. Zwischen den kostenpflichtigen Datenbanken fallen die Qualitätsunterschiede weniger gravierend aus, wenngleich Stärken und Schwächen sich deutlich unterscheiden. Die häufigsten Wechselwirkungen wurden in allen Datenbanken mit großem Abstand zwischen rein psychiatrischen Interaktionspaaren erfasst. Dieses zeigt, wie wechselwirkungsreich Psychopharmaka sind und dass psychiatrische Patienten besonders vulnerabel sind. Die Nutzung digitaler Hilfsmittel scheint bei Betrachtung der hohen Anzahl ausgegebener Warnmeldungen unabdingbar zu sein, dennoch existiert große Uneinheitlichkeit bei der Bewertung der einzelnen Interaktionen. Die Vorstellung, dass zwei Kliniker bei Nutzung zweier unterschiedlicher Datenbanken zu völlig unterschiedlichen Empfehlungen kommen, fällt nicht schwer. Gleichzeitig könnte die Kooperation von Heilberuflern, die unterschiedliche Datenbanken verwenden, die Chance auf zusätzlichen Informationsgewinn und Austausch erhöhen, was im Umkehrschluss in einer erhöhten Arzneimitteltherapiesicherheit resultiert. In Studien konnte der positive Effekt interdisziplinärer Zusammenarbeit bereits bewiesen werden.
Zusammenfassend konnten umfangreiche Differenzen zwischen allen untersuchten Datenbanken aufgezeigt werden. Um den Anforderungen des klinischen Alltags zu genügen, müssen digitale Unterstützungssysteme weiterentwickelt werden.
Die „ideale Datenbank“ gibt es bisher nicht – das lässt sich durch unser Punktesystem beweisen. Um im klinischen Alltag Patientensicherheit zu gewährleisten ist die Nutzung einer einzelnen Datenbank bisher nicht ausreichend.
Die Gewährung der Patientensicherheit sollte unser oberstes Ziel sein und um dieses zu erreichen, bedarf es vieler Komponenten. Neben der Nutzung und vor allem Weiterentwicklung digitaler Unterstützungssysteme sollte auch der zwischenmenschliche Austausch weiter gefördert werden. Interdisziplinäre Zusammenarbeit im Sinne pharmazeutischer Dienstleistungen zur Medikationsanalyse könnten ein zusätzliches Instrument zur Vermeidung arzneimittelbezogener Probleme werden.
Zukünftig werden unsere Patienten am meisten von optimaler Nutzung weiterentwickelter Technologien, sowie wachsendem zwischenmenschlichem Austausch profitieren.
Off-central heavy-ion collisions are known to feature magnetic fields with magnitudes and characteristic gradients corresponding to the scale of the strong interactions. In this work, we employ equilibrium lattice simulations of the underlying theory, QCD, involving similar inhomogeneous magnetic field profiles to achieve a better understanding of this system. We simulate three flavors of dynamical staggered quarks with physical masses at a range of magnetic fields and temperatures, and extrapolate the results to the continuum limit. Analyzing the impact of the field on the quark condensate and the Polyakov loop, we find non-trivial spatial features that render the QCD medium qualitatively different as in the homogeneous setup, especially at temperatures around the transition. In addition, we construct leading-order chiral perturbation theory for the inhomogeneous background and compare its prediction to our lattice results at low temperature. Our findings will be useful to benchmark effective theories and low-energy models of QCD for a better description of peripheral heavy-ion collisions.
Off-central heavy-ion collisions are known to feature magnetic fields with magnitudes and characteristic gradients corresponding to the scale of the strong interactions. In this work, we employ equilibrium lattice simulations of the underlying theory, QCD, involving similar inhomogeneous magnetic field profiles to achieve a better understanding of this system. We simulate three flavors of dynamical staggered quarks with physical masses at a range of magnetic fields and temperatures, and extrapolate the results to the continuum limit. Analyzing the impact of the field on the quark condensate and the Polyakov loop, we find non-trivial spatial features that render the QCD medium qualitatively different as in the homogeneous setup, especially at temperatures around the transition. In addition, we construct leading-order chiral perturbation theory for the inhomogeneous background and compare its prediction to our lattice results at low temperature. Our findings will be useful to benchmark effective theories and low-energy models of QCD for a better description of peripheral heavy-ion collisions.
Das Ziel in der vorliegenden systematischen Literaturrecherche ist es, den aktuellen Stand des Wissens über die Erfolgsfaktoren von Einzelzahnimplantaten, bei denen eine Sofortbelastung auf den provisorischen Implantatkronen zum Antagonisten erfolgt, wiederzugeben. In diesem Rahmen wurden Zusammenhänge zwischen der Implantatüberlebensrate, der Primärstabilität, der Implantatregion, des Implantatdesigns und des Implantationszeitpunktes getrennt nach okklusalem Belastungsprotokoll (mit versus ohne antagonistische Okklusionskontakte auf den provisorischen Implantatkronen) und der postoperativen Verhaltensweisen der Patienten analysiert. Der Prozess der systematischen Literaturrecherche wurde nach den PRISMA-Guidelines für den Suchzeitraum von 2012 bis 2022 durchgeführt.
Um die Forschungsfrage zu beantworten, wurde eine qualitative Analyse in deskriptiver Form durchgeführt.
In den analysierten Studien, wurde am häufigsten ein Eindrehmoment von ≥ 35 Ncm als Kriterium für eine Sofortbelastung gewählt. Die meisten Implantate wurden in der Oberkieferregion 15 bis 25 inseriert. Bei den Implantatkronen mit antagonistischen Okklusionskontakten fielen die Überlebensraten insgesamt niedriger aus als in den Studien, in denen die Implantatkronen ohne antagonistische Okklusionskontakte eingegliedert wurden. Die Überlebensraten waren weitestgehend vergleichbar mit den Ergebnissen konventioneller Belastungsprotokolle. Die Datenlage anhand dieser Recherche spricht zurzeit für die Realisierung der Sofortbelastung von provisorischen Implantatkronen ohne antagonistische Okklusionskontakte in Verbindung mit postoperativen Verhaltensmaßnahmen.
Life and biological resilience rely on the execution of precise gene expression profiles. A key mechanism to ensure cellular homeostasis is the regulation of protein synthesis. Recent studies have unveiled an intrinsic regulatory capacity of ribosomes, previously considered mere executors of mRNA translation. Neurons in particular finely regulate protein synthesis, at both global and local levels. This sustains their complex morphology and allows them to rapidly transmit, integrate, and respond to external stimuli. In this thesis, I investigated the neuronal ribosome and how subcellular environments and physiological perturbations shape it, by profiling its molecular composition, functional interconnections, and cellular distribution.
First, I used genetic engineering, biochemical purification, and mass spectrometry, to characterize in an unbiased manner the translation machinery specifically from excitatory and inhibitory neurons of the mouse cortex. I found that neuronal ribosomes commonly interact with RNA-binding proteins, components of the cytoskeleton, and proteins associated with the endoplasmic reticulum and vesicles. In line with the requirement for local protein synthesis in the distal parts of neurons, we observed that neuronal ribosomes preferentially interact with proteins involved in cellular transport. Remarkably, I observed a strong association between ribosomes and pre-synaptic vesicles, which suggests a potential regulatory interaction between local translation and neuronal activity.
Intriguingly, I and others have observed mRNAs encoding for core ribosomal proteins (RPs) among the genes most enriched in neuronal processes. This observation challenges two historical assumptions of ribosome biology: (1) new RPs are incorporated only into newly forming ribosomes, and (2) this incorporation occurs only in the nucleus and perinuclear region. In my PhD, I aimed to directly test these two assumptions and if proven wrong ask whether and why neurons would localize RP mRNAs far from their known assembly site.
Employing a combination of metabolic labeling and highly sensitive mass spectrometry techniques, I discovered that a subset of RPs rapidly and dynamically binds on and off mature ribosomes. Strikingly, this incorporation does not depend on the supply of new ribosomes from the nucleus. Therefore, my data refuted the assumption that ribosomes are built and degraded as a unit and revealed a more dynamic view of these machines, which can actively exchange core components. In particular, I found that the association of certain exchanging RPs is influenced by location (e.g., cell body versus neurites) and cellular state (e.g., post-oxidative stress). Neurons may use this mechanism to repair and/or specialize their protein synthesis machinery in a rapid and context-dependent manner.
Finally, I asked whether some steps of ribosome biogenesis could also take place in distal processes. Although most steps of ribosome assembly occur within the nucleus, the final stages of maturation are known to occur in the cytosol. By combining several imaging and biochemical approaches, I found that cytosolic (but not nuclear) pre-ribosomal particles are present in neuronal processes. Through the incorporation of new RPs into these immature particles, neurons may be able to locally “turn on” previously incompetent ribosomes. This may enable regions near synapses to enhance and customize their translational capacity, independently of the central pool of ribosomes from the cell body. Indeed, I observed that synaptic plasticity induces a maturation of cytosolic pre-ribosomes.
In summary, this thesis shows how neuronal ribosomes can sense cellular states, respond by adjusting their core composition, and in doing so influence the local capacity for protein synthesis. By overturning long-held assumptions in ribosome biology, this work highlights new molecular mechanisms of gene expression and enriches our understanding of the rapid and dynamic strategies cells employ to operate, thrive, and adaptively respond to environmental changes.