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Das Handschriftenfragment Bergen, Universitetsbiblioteket, MS 1550.5 (im Folgenden: MS 1550.5) veranschaulicht das Schicksal vieler Mittelaltercodices der frühen Neuzeit in Norwegen. Die meisten für liturgische Zwecke genutzten Codices wurden als Palimpseste für verschiedene Aktenstücke, Verstärkung in Buchrücken, Fütterung von Brieftaschen u.ä. wiederverwendet. Das hier vorgestellte Pergamentstück mit den Maßen 305 × 175 mm erhielt in der Forschung bereits weitreichende Aufmerksamkeit. Der Fokus lag allerdings auf der lateinischen Textüberlieferung. Der vorliegende Artikel zielt nun darauf ab, das Fragment in Zusammenhang mit seiner Wiederverwendung als altnorwegische Urkunde zu kontextualisieren und mittels einer vollständigen Beschreibung des Fragments dessen Rezeptionsgeschichte zu beleuchten.
Current research on theory and practice of digital libraries: best papers from TPDL 2019 & 2020
(2022)
This volume presents a special issue on selected papers from the 2019 & 2020 editions of the International Conference on Theory and Practice of Digital Libraries (TPDL). They cover different research areas within Digital Libraries, from Ontology and Linked Data to quality in Web Archives and Topic Detection. We first provide a brief overview of both TPDL editions, and we introduce the selected papers.
Current research on theory and practice of digital libraries: best papers from TPDL 2019 & 2020
(2022)
This volume presents a special issue on selected papers from the 2019 & 2020 editions of the International Conference on Theory and Practice of Digital Libraries (TPDL). They cover different research areas within Digital Libraries, from Ontology and Linked Data to quality in Web Archives and Topic Detection. We first provide a brief overview of both TPDL editions, and we introduce the selected papers.
Plant parasitic nematodes (PPN) are known to survive periods of desiccation, an ability that increases the risk of them surviving unintentional transport between countries. To investigate nematode survival in soil subject to prolonged storage, soil collected from a native forest and an organic orchard was stored separately in cupboards at ambient temperature for 36 months. Subsamples were taken at 0, 3, 6, 12, 13, 24 and 36 months to determine the presence of plant parasitic and total nematodes using a standard misting technique. Pratylenchus was used as a model to determine if PPNs that had been under prolonged storage were able to infect plant hosts at 13, 24 and 36 months. Overall, the total number of nematodes recovered from stored soil declined over time, with differences in species diversity determined by molecular methods, related to soil origin. No PPN were recovered in soil stored beyond 13 months using the three-day misting technique. By comparison, Pratylenchus nematodes, using a baiting method, were found to successfully invade host plant roots (ryegrass and white clover) even after 36 months storage and were observed to produce offspring at 13 months. Baiting was not effective for Pratylenchus found in soil originally collected from the forest but was for orchard soil, a result attributed to the lack of suitable host plants for the Pratylenchus species found in forest soil. This study demonstrated, that in protected environments, nematodes could survive for at least 36 months and were observed to produce offspring at 13 months. Baiting with a host plant was more sensitive in detecting nematodes than using the misting extraction technique, although this approach only works where the host plant is known. Without a priori knowledge of the nematode-plant host association, plant baiting may also produce false negatives. In the context of plant biosecurity and providing an accurate risk assessment in soil contaminants, the development of a generic test for PPN that induces nematodes in a resting stage to emerge and respond to a cue would enhance the probability of detection. However, as assessments at the border are often time limited, a molecular based bioassay that can be used to indicate the presence of multiple species of live PPN species may be a more feasible option for risk assessments.
The inclusive charged particle transverse momentum distribution is measured in proton–proton collisions at s=900 GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region (|η|<0.8) over the transverse momentum range 0.15<pT<10 GeV/c. The correlation between transverse momentum and particle multiplicity is also studied. Results are presented for inelastic (INEL) and non-single-diffractive (NSD) events. The average transverse momentum for |η|<0.8 is 〈pT〉INEL=0.483±0.001 (stat.)±0.007 (syst.) GeV/c and 〈pT〉NSD=0.489±0.001 (stat.)±0.007 (syst.) GeV/c, respectively. The data exhibit a slightly larger 〈pT〉 than measurements in wider pseudorapidity intervals. The results are compared to simulations with the Monte Carlo event generators PYTHIA and PHOJET.
Harmonic decomposition of two particle angular correlations in Pb–Pb collisions at √sNN=2.76 TeV
(2012)
Angular correlations between unidentified charged trigger (t) and associated (a) particles are measured by the ALICE experiment in Pb–Pb collisions at √sNN=2.76 TeV for transverse momenta 0.25<pTt,a<15 GeV/c, where pTt>pTa. The shapes of the pair correlation distributions are studied in a variety of collision centrality classes between 0 and 50% of the total hadronic cross section for particles in the pseudorapidity interval |η|<1.0. Distributions in relative azimuth Δϕ≡ϕt−ϕa are analyzed for |Δη|≡|ηt−ηa|>0.8, and are referred to as “long-range correlations”. Fourier components VnΔ≡〈cos(nΔϕ)〉 are extracted from the long-range azimuthal correlation functions. If particle pairs are correlated to one another through their individual correlation to a common symmetry plane, then the pair anisotropy VnΔ(pTt,pTa) is fully described in terms of single-particle anisotropies vn(pT) as VnΔ(pTt,pTa)=vn(pTt)vn(pTa). This expectation is tested for 1⩽n⩽5 by applying a global fit of all VnΔ(pTt,pTa) to obtain the best values vn{GF}(pT). It is found that for 2⩽n⩽5, the fit agrees well with data up to pTa∼3–4 GeV/c, with a trend of increasing deviation as pTt and pTa are increased or as collisions become more peripheral. This suggests that no pair correlation harmonic can be described over the full 0.25<pT<15 GeV/c range using a single vn(pT) curve; such a description is however approximately possible for 2⩽n⩽5 when pTa<4 GeV/c. For the n=1 harmonic, however, a single v1(pT) curve is not obtained even within the reduced range pTa<4 GeV/c.
Rapidity and transverse momentum dependence of inclusive J/ψ production in pp collisions at √s=7 TeV
(2011)
The ALICE experiment at the LHC has studied inclusive J/ψ production at central and forward rapidities in pp collisions at √s=7 TeV. In this Letter, we report on the first results obtained detecting the J/ψ through the dilepton decay into e+e− and μ+μ− pairs in the rapidity ranges |y|<0.9 and 2.5<y<4, respectively, and with acceptance down to zero pT. In the dielectron channel the analysis was carried out on a data sample corresponding to an integrated luminosity Lint=5.6 nb−1 and the number of signal events is NJ/ψ=352±32(stat.)±28(syst.); the corresponding figures in the dimuon channel are Lint=15.6 nb−1 and NJ/ψ=1924±77(stat.)±144(syst.). The measured production cross sections are σJ/ψ(|y|<0.9)=10.7±1.0(stat.)±1.6(syst.)−2.3+1.6(syst.pol.)μb and σJ/ψ(2.5<y<4)=6.31±0.25(stat.)±0.76(syst.)−1.96+0.95(syst.pol.)μb. The differential cross sections, in transverse momentum and rapidity, of the J/ψ were also measured.
The first measurement of two-pion Bose–Einstein correlations in central Pb–Pb collisions at √sNN=2.76 TeV at the Large Hadron Collider is presented. We observe a growing trend with energy now not only for the longitudinal and the outward but also for the sideward pion source radius. The pion homogeneity volume and the decoupling time are significantly larger than those measured at RHIC.
Inclusive transverse momentum spectra of primary charged particles in Pb–Pb collisions at √sNN=2.76 TeV have been measured by the ALICE Collaboration at the LHC. The data are presented for central and peripheral collisions, corresponding to 0–5% and 70–80% of the hadronic Pb–Pb cross section. The measured charged particle spectra in |η|<0.8 and 0.3<pT<20 GeV/c are compared to the expectation in pp collisions at the same sNN, scaled by the number of underlying nucleon–nucleon collisions. The comparison is expressed in terms of the nuclear modification factor RAA. The result indicates only weak medium effects (RAA≈0.7) in peripheral collisions. In central collisions, RAA reaches a minimum of about 0.14 at pT=6–7 GeV/c and increases significantly at larger pT. The measured suppression of high-pT particles is stronger than that observed at lower collision energies, indicating that a very dense medium is formed in central Pb–Pb collisions at the LHC.
Das humane Immundefizienz-Virus (HIV) benötigt für die Virus-Zellbindung spezifische Oberflächenrezeptoren auf den Wirtszellen (z. B. CD4, CXCR4, CCR5). Zurzeit basiert die Behandlung der chronisch persistierenden HIV-Erkrankung auf einer lebenslangen Chemotherapie (Highly Active Antiretroviral Therapy, ART) bestehend beispielsweise aus einer Kombination von 2 Nukleosidanaloga und einem Protease-Inhibitor, die das Virus nicht eradiziert, sondern nur in seiner Vermehrung hemmt. Dies birgt jedoch die Gefahr der Entwicklung von Resistenzen gegenüber der medikamentösen Therapie. Zusätzlich wird eine Veränderung der HIV-Rezeptorspezifität unter der Behandlung mit Antagonisten des HIV-Rezeptors CCR5 befürchtet. Cytarabin (Ara-C) ist ein Zytostatikum, das in der Therapie von Leukämien eingesetzt wird. Als Nukleosidanalogon gehört es strukturell zur selben Wirkstoffklasse wie die in der HIV-Therapie eingesetzten Nukleosidanaloga, jedoch sind bisher keine antiretroviralen Eigenschaften für Ara-C beschrieben worden. Die T-lymphoide Zelllinie C8166 ist permissiv für HIV. Die Adaptation von C8166-Zellen an das Wachstum in Gegenwart von Ara-C (Zellinie C8166rAra-C5μM) resultierte in einer signifikanten Verringerung der Oberflächenexpression der HIV-Rezeptoren CD4 und CXCR4 und zu einer verringerten Permissivität gegenüber HIV. In der vorliegenden Arbeit sollte untersucht werden, ob die Adaptation an Ara-C bei anderen T-lymphoiden Zelllinien ebenfalls zur Verringerung der Expression von CD4, und CXCR4 führt. Zusätzlich sollte untersucht werden, wie sich die Expression von CCR5 verhält. Es wurden die folgenden parentalen und an Ara-C adaptieten T-lymphoiden Zelllinien verwendet: H9, H9rAra-C600μM, MOLT4/8, MOLT4/8rAra-C100μM und MOLT4/8rAra-C200μM. Bei allen Ara-C resistenten Zelllinien kam es zu einer signifikant verringerten Expression von CD4 und CXCR4 auf mRNA und Proteinebene sowie zu einer signifikanten Erhöhung der CCR5-Expression. Im Gegensatz hierzu zeigten an AZT adaptierte H9-Zellen (H9rAZT3000μM) keine signifikante Veränderung in der Expression von CD4, CXCR4 oder CCR5 im Vergleich zu parentalen H9-Zellen. Die akute Behandlung der parentalen H9-Zellen mit niedrigen, untoxischen Ara-C Konzentrationen führte ebenfalls zu einem Anstieg der CCR5-Expression und zu einer Verminderung der CD4- und CXCR4-Expression. Zellzyklusmessungen ergaben, dass der Zellzyklus in mit untoxischen Ara-C-Konzentrationen behandelten H9-Zellen (Anstieg der Zellteilungsrate auf das 2-fache) und in allen an Ara-C adaptierten Zelllinien im Vergleich zu den unbehandelten bzw. parentalen Zellen stärker stimuliert war. Epigenetische Einflüsse könnten bei der veränderten Expression von CD4, CXCR4 und/oder CCR5 in Ara-C resistenten Zellen eine Rolle spielen. Dies erscheint jedoch unwahrscheinlich, da weder der DNA-Methylierungsinhibitor Aza-C noch der Histondeacetylase-Inhibitor SAHA die Expression von CD4, CXCR4 oder CCR5 beeinflussten. Weitere Untersuchungen müssen zeigen, ob eine Kombination von Ara-C, das zu einer Verringerung der CXCR4- und CD4-Expression und zu einer Erhöhung der CCR5-Expression führt, mit CCR5-Inhibitoren eine therapeutische Option darstellt. Möglicherweise wirkt die Verwendung von Ara-C auch einem CCR5/CXCR4-Shift entgegen.
Den gegenstand unserer untersuchung bildet das märchen von dem sich deckenden tischtuch, dem goldesel und dem von selbst schlagenden Knüppel, das zu den häufigsten und weitverbreitetsten aller volksmärchen gehört. Das tischtuch und der esel werden dem helden des märchens mit anderen, gleich aussehenden, wiewohl in ihrer art gewöhnlichen gegenständen vertauscht, aber er befiehlt dem Knüppel den betrüger durchzuprügeln und zwingt diesen so ihm die zaubergegenstände zurückzugeben. Neben dieser märchenform hat sich eine andere verbreitet, in der zwei zaubergegenstände: ein essenspendender und ein schlagender auftreten, doch ist die haupfabel der geschichte sohst ähnlich. Das erstgenannte zauberding wird einer anderen person überlassen und mit hilfe des letztgenannten zurückgewonnen. Es existiert auch noch eine dritte form von unserem märchen. Darin erscheint als zaubergegenstand nur eine essen u. a. mahöende mühle, die dadurch auch die aufgabe des Knüppels erfüllen muss, dass ihr neuer besitzer sie nicht einzuhalten weiss und infolge der ungeheuren menge des essens in not gerät.
Phase transitions in a non-perturbative regime can be studied by ab initio Lattice Field Theory methods. The status and future research directions for LFT investigations of Quantum Chromo-Dynamics under extreme conditions are reviewed, including properties of hadrons and of the hypothesized QCD axion as inferred from QCD topology in different phases. We discuss phase transitions in strong interactions in an extended parameter space, and the possibility of model building for Dark Matter and Electro-Weak Symmetry Breaking. Methodological challenges are addressed as well, including new developments in Artificial Intelligence geared towards the identification of different phases and transitions.
Sorbus cordigastensis N. Mey. (Kordigast-Mehlbeere) ist eine Rote-Liste-Art aus dem Komplex hybridogener Sippen von Sorbus aria und S. torminalis, die endemisch am Kordigast, einem Zeugenberg des Oberen Jura in der Weismainalb (Naturraum „Nördliche Fränkische Alb“) vorkommt. Ziel der Untersuchung war es, die Verbreitung und Größe der Population sowie den Zustand ihrer Verjüngung zu erfassen. Zu diesem Zweck wurden sämtliche im Gebiet vorkommenden Individuen mit einer Wuchshöhe über 1,3 m punktgenau kartiert. In drei etwa 0,35–0,4 ha großen Waldbeständen wurden mittels Stichprobenverfahren die Anzahl und Wuchshöhe der Jungpflanzen sowie das Ausmaß der Wildschäden ermittelt. Sorbus cordigastensis ist mit etwa einem größeren (> 1,3 m hoch) Individuum pro Hektar im untersuchten Gebiet selten, kommt aber lokal und insbesondere an Waldrändern gehäuft vor. In Beständen mit fruktifizierenden Altbäumen verjüngt sich die Art gut. In den drei untersuchten Waldbeständen konnten, bezogen auf einen Hektar Fläche, im Durchschnitt etwa 1500 Jungpflanzen mit einer Wuchshöhe < 1,3 m nachgewiesen werden. Der Großteil davon ist weniger als 30 cm hoch, Jungpflanzen über 90 cm Höhe fehlen jedoch. Eine der Ursachen dafür sind starke Wildschäden. Bei zwei Drittel aller Jungpflanzen ist der Leittrieb ein- oder mehrmals verbissen. Verschiedene Beobachtungen weisen darauf hin, dass darüber hinaus Lichtmangel in den relativ dichten Beständen die dauerhafte Etablierung der Verjüngung beeinträchtigt. Die Population der Kordigast-Mehlbeere ist derzeit an ihrem Naturstandort noch relativ groß und gut zur Reproduktion fähig. Da sich ihre Verjüngung aber nicht ausreichend etablieren kann, ist der Bestand auf längere Sicht vom Aussterben bedroht. Schutzmaßnahmen müssen darauf abzielen, die Bedingungen für das Aufwachsen der Verjüngung durch Verringerung der Wildschäden und Auflichtung der Bestände zu verbessern.
This paper focuses on an ongoing project that began in 2012, entitled "The Collection of Jane Ryan & William Saunders". This project is an attempt to reconstitute the Marcos Collection. Sourced from auction catalogues, museum archives, and scant government records, their lavish inventory of commissioned portraits, jewellery, Regency silverware, and old master paintings is reproduced as photographic installations, postcards, and three-dimensional prints. Reconstruction, in this instance, becomes a sustained democratic gesture, allowing an increasingly forgetful public to access a collection that has remained unavailable through a systemic failure by successive post-dictatorial governments to institutionalize collective acts of remembering.
Depuis bientôt trois (3) ans, le Docteur Heméry-Hervais SIMA-EYI enseignant et directeur en outre, du Centre d’études pour la littérature gabonaise(CELIG) anime à la faculté des lettres et des sciences humaines, notamment au sein du département des Littératures Africaines de l’Université Omar Bongo, un séminaire intitulé « Littérature et société au Gabon » . Ce séminaire vise à étudier, analyser la littérature gabonaise dans ses rapports apparents avec la société dans laquelle cette littérature est produite. Pour ce faire, le Docteur SIMA-EYI a demandé à ses étudiants de voir, dans l’optique d’un colloque sur la littérature gabonaise , quelle place les institutions littéraires(maisons d’éditions, universités, centres de recherche, ministères, etc.)accordent à la littérature produite dans notre pays . Ainsi, scindée en deux(2) groupes,l’un dirigé par Guy Wilfried IDIATHA et l’autre par Désiré Clitandre DZONTEU, la classe de licence des Littératures Africaines s’est donc penchée sur cet épineux problème. Notre équipe s’est intéressée au groupe bancaire BICIG et son concours littéraire et artistique ; au Théâtre national ; aux maisons d’éditions entre autres, La Maison Gabonaise du Livre, Ndzé, Hilaire Makaya et les éditions du silence ; l’Union des écrivains gabonais(UDEG), l’Ecole Normale supérieure(ENS) et l’organisation des Nations unies pour l’éducation , la science et la culture(UNESCO). Il est sans rappelé que ce travail ne fut pas une sinécure, plutôt parfois un parcours du combattant. -------------------------------------------------------------------------------------------- CRELAF (Cercle de Reflexion des Etudiants en Littératures Africaines), Département de Littératures Africaines, Université Omar Bongo, Gabon
Die vorliegende Dissertationsschrift befasst sich mit der molekulargenetischen Analyse zweier Basalganglienerkrankungen. Zum einen wurden Patienten mit M. Parkinson genetisch untersucht, zum anderen Patienten mit autosomal dominanter zervikaler Torsionsdystonie. Die Aufgabe bestand in der passenden Wahl der Methode zur jeweiligen humangenetischen Fragestellung. Der erste Teil handelte von der Suche der krankheitsverursachenden Mutation für die autosomal dominante zervikale Torsionsdystonie mit Spätmanifestation auf Chromosom 18p (Kandidatenlokus DYT7). Die erkrankte Familie deutscher Herkunft zeigt dystone Symptome mit Betonung auf kraniozervikale und brachiale Körperabschnitte und ist somit die weltweit einzige bekannte Familie mit Vererbung dieser ansonsten sporadisch auftretenden Erkrankung. Die PCR-Sequenzierung der Kandidatengene ZFP161, LOC390828, NDUFV2 und PTPRM auf dem DYT7 Lokus erbrachte bei den sieben erkrankten Familienmitgliedern im Vergleich zu nicht verwandten Kontrollen (Ehepartner und 96 Kontrollen der Blutbank) keinen Aminosäureaustausch, der ausschließlich bei den erkrankten Probanden zu finden war. Technisch konzentrierte sich diese Untersuchung auf die Amplifizierung und anschließende Sequenzierung jedes einzelnen Exons in den zu untersuchenden Proben, und die Bestätigung einer putativen Mutation mittels Verdau der PCR-Produkte durch Restriktionsendonukleasen. Die Auswahl der Kandidatengene erfolgte aufgrund der Annahme pathobiochemischer Mechanismen, die durch andere Formen der vererbten Torsionsdystonie oder zellbiologische Experimente als krankheitsverursachend gelten. Auch wenn keine Mutation gefunden wurde, so konnten bereits bekannte und neue single nucleotide polymorphisms (SNP) etabliert werden. Die zweite Thematik befasste sich mit der Frage, ob das bereits bekannte Parkinson-Gen UCH-L1 auf dem PARK5 Lokus krankheitsverursachend für den autosomal dominanten M. Parkinson in einer spanischen Familie ist. Diese parametrische Kopplungsanalyse wurde mithilfe der heißen Polyacrylamid-Gelelektrophorese (PAGE) durchgeführt. Dabei konnte in allen Patienten und den Verwandten ersten Grades über Analyse der Mikrosatelliten nördlich und südlich der Kandidatenregion (UCH-L1) in einem Bereich sehr niedriger Rekombinationswahrscheinlichkeit eine Haplotypisierung erfolgen. Die Haplotypisierung zeigte nicht die erforderliche Identifizierung eines Krankheitsallels bei allen betroffenen Probanden. Somit ist hier neben der einzig bekannten deutschen PARK5 Familie keine weitere Familie mit UCH-L1 Mutation bestätigt worden. Dementsprechend ist die Ätiologie dieser Erkrankung in dieser Familie noch unklar, was aber der Bedeutung des Ubiquitin-Proteasom Systems in der Parkinson-Entität keinen Abbruch getan hat. Da alle anderen autosomal dominanten Parkinson-Loci ausgeschlossen sind, muss sich die Ursache für den M. Parkinson in dieser Familie in einem heute noch unbekannten Gen befinden. Weitere Untersuchungen im Rahmen eines Genomscans sind aufgrund der geringen Fallzahl nicht möglich. Die letzte Aufgabe dieser Arbeit bestand in der Durchführung einer Assoziationsstudie mit den putativen PINK1 (PARK6) Interaktoren NME4 und MTIF3 für den mehrheitlich sporadisch auftretenden M. Parkinson. Dabei wurden in zwei unabhängigen Studiengruppen mit insgesamt 453 sporadischen Parkinsonpatienten und 370 Kontrollen jeweils zwei SNPs auf gekoppelte Vererbung mit der Erkrankung untersucht. Der Unterschied zwischen den Testgruppen bestand im Studiendesign, da zum einen mit den Patienten nicht verwandte Kontrollen und zum anderen verwandte Kontrollen verwendet wurden. Die mit beiden Studientypen normalerweise auftretenden Probleme durch Stratifikation bzw. erniedrigte statistische Power konnten durch Kombination der Studien ausgeglichen werden. Das Methodenspektrum umfasste PCR und Restriktionsverdau, was zum Auffinden eines Kopplungsungleichgewichts für das Gen MTIF3 führte. Ein heterozygoter Basenaustausch für den Polymorphismus rs7669 erhöht signifikant das Relative Risiko an M. Parkinson zu erkranken, wohingegen der homozygote Basenaustausch das Krankheitsrisiko des Trägers signifikant erniedrigt. Bezüglich des Relativen Risikos wurde der Effekt der molekularen Heterosis nachgewiesen. Bei diesem mitochondrial lokalisierten Gen handelt es sich um einen Initiator der mitochondrialen Translation. Demzufolge besteht hier Einfluss auf die Homöostase und somit Funktionalität der Atmungskettenkomplexe, die als bedeutend für die Pathogenese des M. Parkinson angesehen werden. Die Verbindung zum mitochondrial lokalisierten PINK1 besteht aufgrund seiner Kinase-Aktivität in der An- und Abschaltung des mitochondrialen Translations - Initiationsfaktors. Aber auch die Wichtigkeit von NME4 konnte in dieser Studie trotz fehlender Assoziation nicht ausgeschlossen werden, da vorangehende experimentelle Ergebnisse dieses Protein bereits in den PINK1 Signalweg zuordnen konnten. MTIF3 könnte wohlmöglich ein wichtiger genetische Risikofaktor für den idiopathischen M. Parkinson sein. Es bleibt abzuwarten, ob zukünftige genetische und zellbiologische Experimente die Wichtigkeit, die in diesem Protein zu liegen scheint, bestätigen können.
A Fallen Citadel and Other Poems is a powerful collection of over forty prose poems. The poems cover an array of issues ranging from the crisis that ensued after the 2007-2008 elections in Kenya to other social issues: loss of identity, poverty, hopelessness, and AIDs. These poems are powerful, vivid, full of imagery, and delightful. Some begin tragically, but end with hope; they begin with an everyday event, but end with a philosophical question about the meaning of life; and others are not only disturbing, but also thought provoking. Abala's poetic maneuvers in this collection are bound to delight and fascinate any reader.
We show the existence of additive kinematic formulas for general flag area measures, which generalizes a recent result by Wannerer. Building on previous work by the second named author, we introduce an algebraic framework to compute these formulas explicitly. This is carried out in detail in the case of the incomplete flag manifold consisting of all (p+1)-planes containing a unit vector.
We show how nonlocal boundary conditions of Robin type can be encoded in the pointwise expression of the fractional operator. Notably, the fractional Laplacian of functions satisfying homogeneous nonlocal Neumann conditions can be expressed as a regional operator with a kernel having logarithmic behaviour at the boundary.
We provide a Hopf boundary lemma for the regional fractional Laplacian (−Δ)sΩ, with Ω ⊂ RN a bounded open set. More precisely, given u a pointwise or weak super-solution of the equation (−Δ)s u = c(x)u in Ω, we show that the ratio u(x)∕(dist(x, 𝜕Ω))2s−1 is strictly Ω positive as x approaches the boundary 𝜕Ω of Ω. We also prove a strong maximum principle for distributional super-solutions.
We show explicit formulas for the evaluation of (possibly higher-order) fractional Laplacians (-△)ˢ of some functions supported on ellipsoids. In particular, we derive the explicit expression of the torsion function and give examples of s-harmonic functions. As an application, we infer that the weak maximum principle fails in eccentric ellipsoids for s ∈ (1; √3 + 3/2) in any dimension n ≥ 2. We build a counterexample in terms of the torsion function times a polynomial of degree 2. Using point inversion transformations, it follows that a variety of bounded and unbounded domains do not satisfy positivity preserving properties either and we give some examples.
Augmented Reality ist eine Technologie, mit der die Wahrnehmung der realen Umgebung durch computergenerierte Sinnesreize verändert bzw. erweitert wird. Zur Erweiterung dieser „angereicherten Realität“ werden virtuelle Informationen wie z.B. 3D-Objekte, Grafiken und Videos in Echtzeit in Abbildern der realen Umgebung dargestellt. Die Erweiterungen helfen dem Anwender Aufgaben in der Realität auszuführen, da sie ihm Informationen bereitstellen, die er – ohne AR – nicht unmittelbar wahrnehmen könnte. Die Zielsetzung ist, dem Benutzer den Eindruck zu vermitteln, dass die reale Umgebung und die virtuellen Objekte koexistent miteinander verschmelzen. Für AR-Anwendungen existieren zahlreiche potenzielle Einsatzgebiete, doch verhindern bisher einige Probleme die Verbreitung dieser Technologie. Einer breiten Nutzung von AR-Anwendungen steht beispielsweise die Problematik gegenüber, dass deren Erstellung hohe programmiertechnische Anforderungen an die Entwickler stellt. Zur Verminderung dieser Probleme ist es wünschenswert Benutzern ohne Programmierkenntnisse (Autoren) die Entwicklung von AR-Anwendungen zu ermöglichen. Zum anderen bestehen technologische Probleme bei den für die Registrierung der virtuellen Objekte essenziellen Trackingverfahren. Weiterhin weisen die bisherigen AR-Anwendungen im Allgemeinen und die mittels autorenorientierter Systeme erstellten AR-Applikationen im Besonderen Defizite bezüglich der Authentizität der Darstellungen auf. Dabei sind hauptsächlich inkorrekte Verdeckungen und unrealistische Schatten bei den virtuellen Objekten verantwortlich für den Verlust des Koexistenzeindrucks. In dieser Arbeit wird unter Berücksichtigung der Trackingprobleme und auf Basis von Analysen, die die wichtigsten Authentizitätskriterien bestimmen, ein Konzept zur authentischen Integration von virtuellen Objekten in AR-Anwendungen erarbeitet und dargelegt. Auf diesem Integrationsprozess basierend werden Konzepte für Werkzeuge mit grafischen Benutzungsschnittstellen abgeleitet, mit denen Autoren die Erstellung von AR-Anwendungen mit hoher Darstellungsauthentizität ermöglicht wird. Einerseits verfügen die mit diesen Werkzeugen erstellten AR-Anwendungen über eine verbesserte Registrierung der virtuellen Objekte. Andererseits stellen die Werkzeuge Lösungen bereit, damit die virtuellen Objekte der AR-Anwendungen korrekte Verdeckungen aufweisen und über Schatten und Schattierungseffekte verfügen, die mit der tatsächlichen Beleuchtungssituation der realen Umgebung übereinstimmen. Sämtliche dieser Autorenwerkzeuge basieren auf einem in dieser Arbeit dargelegten Prinzip, bei dem die authentische Integration mittels leicht verständlicher bzw. wenig komplexer Arbeitsschritte und auf Basis der Verwendung einer Bildsequenz der realen Zielumgebung stattfindet. Die Konzepte dieser Arbeit werden durch die Implementierung der Autorenwerkzeuge validiert. Dabei zeigt sich, dass die Konzepte technisch umsetzbar sind. Die Evaluierung basiert auf der Gegenüberstellung eines in dieser Arbeit entwickelten Anforderungskatalogs und verdeutlicht die Eignung des Integrationsprozesses und der davon abgeleiteten Konzepte der Autorenwerkzeuge. Die Autorenwerkzeuge werden in eine bestehende, frei verfügbare AR-Autorenumgebung integriert.
The paper introduces the socio-anthropological concept of international representations to examine the relationship between a civilizational rhetoric, the West European and the international politics of otherization and containment of Southeast Europe, and an essentialist and timeless bias in international relations theory, including both radical and constructivist trends...
Clean water is fundamental to human health and ecosystem integrity. However, water quality deteriorates due to novel anthropogenic pollutants present at microgram per liter concentrations in urban water cycles (termed micropollutants). Wastewater treatment plants (WWTP) have been identified as major point sources for aquatic (micro-)pollutants. Chemical and ecotoxicological analyses have shown that conventional biological WWTPs do not fully remove micropollutants and associated toxicities, which is often because of mobile, polar and/or recalcitrant compounds and transformation products (TPs). To minimize possible environmental risks, advanced wastewater treatment (AWWT) technologies could be a promising mitigation measure. Multiple processes are therefore being developed and evaluated such as ozonation and ozonation followed by granulated activated carbon (GAC) or biological filtration. Assessing the performance of these combined AWWTs was the focus the TransRisk project. Within this project, this thesis accomplished four major goals.
Firstly, the preparation of (waste)water samples was optimised for in vitro bioassays. Acidification, filtration and solid phase extraction (SPE) were tested for their impact on environmentally relevant in vitro endocrine activities, mutagenicity, genotoxicity and cytotoxicity. Significantly different outcomes of these assays were detected comparing neutral and acidified samples. Sample filtration had a lesser impact, but in some cases retention of particle-bound compounds could have caused significant toxicity losses. Out of three SPE sorbents the Telos C18/ENV at sample pH 2.5 extracted highest toxicity, some undetected in aqueous samples. These results indicate that sample preparation needs to be optimised for specific sample matrices and bioassays to avoid false-positive or -negative detects in effect-based analyses.
Secondly, the above listed in vitro toxicities were monitored in a protected region for drinking water production in South-West Germany (2012-2015). Out of 30 sampling sites surface water and groundwater were the least polluted. Nonetheless, a few groundwater samples induced high anti-estrogenic activity that prompted further monitoring. The latter included a waterworks in which no toxicity was detected. Hospital wastewater also had elevated in vitro toxicities and hospitals are, thus, relevant intervention points for source control. The biological WWTPs were effective in removing most of the detected toxicity, and the selected bioassays proved to be pertinent tools for water quality assessment and prioritisation of pollution hotspots.
Thirdly, the in vivo bioassay ISO10872 based on Caenorhabditis elegans (C. elegans) was adapted for this thesis. Using this model, a median effect concentration (EC50) for reproductive toxicity of the polycyclic aromatic hydrocarbon β-naphthoflavone (β- NF) of 114 µg/L was computed which is slightly lower than reported in the scientific literature. β-NF induced cyp-35A3::GFP (a biomarker in transgenic animals) in a time and concentration dependent manner (≤ 21.3–24 fold above controls). β-NF spiked wastewater samples supported earlier hypotheses on particle-bound pollutants. Reproductive toxicity (96 h) and cyp-35A3 induction (24 h) of biologically treated and/or ozonated wastewater extracts and growth promoting effects of GAC/biologically filtered ozonated wastewater extracts were observed. This suggested the presence of residual bioactive/toxic chemicals not included in the targeted chemical analysis. It also highlighted the importance of integrating multiple (apical and molecular) endpoints in wastewater assessments.
Fourthly, five in vitro and the adapted C. elegans bioassay were integrated into a wastewater quality evaluation (developed within TransRisk). Out of the five AWWT options, ozonation (at 1 g O3,applied/g DOC, HRT ~ 18 min) combined with nonaerated GAC filtration was rated most effective for toxicity removal. All five AWWTs largely removed estrogenic and (anti-)androgenic activities, but not anti-estrogenic activity and mutagenicity, which even increased during ozonation. This has been observed in related studies and points towards toxic TPs. These results also emphasized the need for implementing an effective post-treatment for ozonation. The results from a parallel in vivo study with Lumbriculus variegatus and Potamopyrgus antipodarum conducted on site at the WWTP (using flow through systems) were in accordance with the C. elegans results. In this context, it is suggested to further implement C. elegans as sensitive, feasible and ecologically relevant model.
In conclusion, this thesis shows how optimised sample preparation, long-term (in vitro) environmental monitoring, sensitive and ecologically relevant (in vivo) bioassays as well as innovative evaluation concepts, are pivotal in improving the removal of micropollutants and their toxicities with AWWTs. Future research should further develop and evaluate measures at sewer systems, conventional biological, tertiary and other advanced treatment technologies, as well as sociopolitical strategies (e.g., source control or natural conservation) and restoration projects. The effect-based tools optimised in this thesis will support assessing their success.
Wrack burial reduces germination and establishment of the invasive cordgrass Spartina densiflora
(2014)
Germination and emergence of halophytes may decrease significantly by seed burial in dead plant material, or wrack, which is common and abundant in tidal marshes. The effects of plant debris (wrack) burial on seed germination and seedling establishment of Spartina densiflora, an invasive cordgrass, were studied under greenhouse conditions and compared with field observations. Five wrack burial depths were applied: control without wrack, 1 cm (1235 ± 92 g DW wrack m-2), 2 cm (3266 ± 13 g DW m-2), 4 cm (4213 ± 277 g DW m-2), and 8 cm (6138 ± 227 g DW m-2). Sediment pH, electrical conductivity, redox potential and temperature were recorded. Quiescence increased with wrack load up to ~20% at 8 cm deep. Germination decreased with wrack load from 96% to 14%, which could be related with anoxic conditions under the debris since sediment redox potential was as low as -83 ± 7 mV at 8 cm. Germination percentage increased and quiescent and dormant percentages decreased at higher daily sediment temperatures and with higher daily temperature fluctuations, conditions that were recorded without or under low loads of wrack. Spartina densiflora did not show primary dormancy, but its seeds entered into a non-deep physiological dormancy below 1 cm deep in plant debris. The establishment of S. densiflora seedlings was also greatly reduced by wrack burial since only 6 seedlings (11 ± 5 % of germinated seeds) emerged above plant debris from 1 cm and all seedlings died from deeper than 1 cm. S. densiflora seedling development was also reduced by wrack burial. The inverse relationship between germination and emergence of S. densiflora with wrack burial recorded in our study is useful to predict its invasion dynamics and to plan the management of invaded marshes.
The title compound, C20H22O2, crystallizes with two independent molecules in the asymmetric unit. In each molecule, all the non-H atoms lie in a common plane (r.m.s. deviations of 0.098 and 0.079 Å). There is a [pi]-[pi] stacking interaction in the crystal structure. The central aromatic rings of the two molecules, which are stacked head-to-tail one above the other, are separated by centroid-to-centroid distances of 3.872 (13) and 3.999 (10) Å. Key indicators: single-crystal X-ray study; T = 173 K; mean σ(C–C) = 0.003 A° ; R factor = 0.044; wR factor = 0.101; data-to-parameter ratio = 14.6.
The title compound, C14H20O3, is a synthetic analogue with a long aliphatic side chain of the important food additive and flavoring agent, vanillin. There are two independent molecules in the asymmetric unit, each having an essentially planar conformation (r.m.s. deviations of 0.023 and 0.051Å for all non-H atoms of the two molecules in the asymmetric unit). Key indicators: single-crystal X-ray study; T = 173 K; mean σ(C–C) = 0.002 A°; R factor = 0.049; wR factor = 0.144; data-to-parameter ratio = 15.9.
We present the first wide-range measurement of the charged-particle pseudorapidity density distribution, for different centralities (the 0-5%, 5-10%, 10-20%, and 20-30% most central events) in Pb-Pb collisions at sNN−−−√=2.76 TeV at the LHC. The measurement is performed using the full coverage of the ALICE detectors, −5.0<η<5.5, and employing a special analysis technique based on collisions arising from LHC "satellite" bunches. We present the pseudorapidity density as a function of the number of participating nucleons as well as an extrapolation to the total number of produced charged particles (Nch=17165±772 for the 0-5% most central collisions). From the measured dNch/dη distribution we derive the rapidity density distribution, dNch/dy, under simple assumptions. The rapidity density distribution is found to be significantly wider than the predictions of the Landau model. We assess the validity of longitudinal scaling by comparing to lower energy results from RHIC. Finally the mechanisms of the underlying particle production are discussed based on a comparison with various theoretical models.
Endokrin inaktives Hypophysenadenom und sekundäre Nebennierenrindeninsuffizienz : ein Fallbericht
(2021)
Das Hypophysenadenom als Ursache einer sekundären Nebennierenrindeninsuffizienz, nur mit isoliertem ACTH-Defizit, ist außergewöhnlich. Ein ACTH-Mangel tritt in der Regel nicht isoliert, sondern zusammen mit dem Ausfall anderer Hypophysenfunktionen auf. Besonders bei Patienten mit Kinderwunsch sollte den Erkrankungen der Hypophyse und der Nebennieren große Aufmerksamkeit geschenkt werden.
Bacterial biosynthetic assembly lines, such as non-ribosomal peptide synthetases (NRPS) and polyketide synthases, are often subject of synthetic biology – because they produce a variety of natural products invaluable for modern pharmacotherapy. Acquiring the ability to engineer these biosynthetic assembly lines allows the production of artificial non-ribosomal peptides (NRP), polyketides, and hybrids thereof with new or improved properties. However, traditional bioengineering approaches have suffered for decades from their very limited applicability and, unlike combinatorial chemistry, are stigmatized as inefficient because they cannot be linked to the high-throughput screening platforms of the pharmaceutical industry. Although combinatorial chemistry can generate new molecules cheaper, faster, and in greater numbers than traditional natural product discovery and bioengineering approaches, it does not meet current medical needs because it covers only a limited biologically relevant chemical space. Hence, methods for high-throughput generation of new natural product-like compound libraries could provide a new avenue towards the identification of new lead compounds. To this end, prior to this work, we introduced an artificial synthetic NRPS type, referred to as type S NRPS, to provide a first-of-its-kind bicombinatorial approach to parallelized high-throughput NRP library generation. However, a bottleneck of these first two generations of type S NRPS was a significant drop in production yields. To address this issue, we applied an iterative optimization process that enabled titer increases of up to 55-fold compared to the non-optimized equivalents, restoring them to wild-type levels and beyond.
»Read Better!«
(2018)
This essay is an excerpt from Jumana Emil Abboud's ongoing journal, which she started keeping in 2010. With the help of photographer Issa Freij, the artist identified spirited water spots in the topography of Palestine, based on her childhood memories and a 1922 study on "Haunted Springs and Water Demons in Palestine". The text was written as part of a performance by Abboud at the Khalil Sakakini Cultural Center in 2016.
A new species of Liolaemus is described from southwest of the town of Añelo, Neuquén Province, Argentina. Integrative evidence methodology of external morphological characters and molecular phylogenetic analyses of mitochondrial DNA (cyt-b) is used to place the new species to the species group of Liolaemus boulengeri. The new species is phenotypically close to L. mapuche. The new Liolaemus is medium to large in size (males 77.64–83.98 mm, females 72.88–78.58 mm), with evident sexual dichromatism. Genetic distances of the mtDNA (cyt-b) between the new species and its closest relative species are greater than 3% (L. cuyanus 7.48–12.02%; L. josei 7.56–9.60%; L. puelche 8.23–9.93%; L. mapuche 8.51–9.79%). Molecular and morphological phylogenetic results show L. mapuche as the sister species of the new one. The new species is larger than L. mapuche. Dorsal and ventral scales are more numerous in the new species than in L. mapuche, precloacal pores in females are present in L. mapuche and absent in the new species. It has strict psammophilic habits, using sand mounds and sheltering, under Alpataco (Neltuma alpataco) bushes. The L. boulengeri group now contains 75 species distributed in Argentina, Bolivia, Brazil, Chile, Paraguay, Peru and Uruguay.
Neste artigo, proponho a aproximação do poema "Engführung" (1958), do poeta Paul Celan, com o ensaio "Cascas" (2011 [2017]), do historiador de arte francês Georges Didi-Huberman, tomando como ponto de partida a ideia de percurso que atravessa ambas as obras. Para tanto, baseio-me nas leituras que Joachim Seng faz do poema de Celan (1992; 1998), nas quais lê "Engführung" como um trajeto do eu-poético pelo campo de concentração (Auschwitz) que é, ao mesmo tempo, campo da memória e linguagem. Em "Cascas", Didi-Huberman relata o percurso da sua visita a Auschwitz, enfocando o papel do olhar na realização do trabalho da memória. Nesse sentido, ao posicionar lado a lado o poema e o ensaio, estes parecem apontar para modos de olhar e dizer Auschwitz que colocam para o leitor as tensões inerentes a este movimento, não se omitem desta tarefa ética e refletem criticamente a postura individual e coletiva diante da lacuna do testemunho e do que resta do campo de concentração.
The STAR Collaboration reports measurements of back-to-back azimuthal correlations of di-π0s produced at forward pseudorapidities (2.6<η<4.0) in p+p, p+Al, and p+Au collisions at a center-of-mass energy of 200 GeV. We observe a clear suppression of the correlated yields of back-to-back π0 pairs in p+Al and p+Au collisions compared to the p+p data. The observed suppression of back-to-back pairs as a function of event activity and transverse momentum suggests nonlinear gluon dynamics arising at high parton densities. The larger suppression found in p+Au relative to p+Al collisions exhibits a dependence of the saturation scale, Q2s, on the mass number, A. The suppression in high-activity p+Au collisions is consistent with theoretical predictions including gluon saturation effects.
The STAR Collaboration reports measurements of back-to-back azimuthal correlations of di-π0s produced at forward pseudorapidities (2.6<η<4.0) in p+p, p+Al, and p+Au collisions at a center-of-mass energy of 200 GeV. We observe a clear suppression of the correlated yields of back-to-back π0 pairs in p+Al and p+Au collisions compared to the p+p data. The observed suppression of back-to-back pairs as a function of transverse momentum suggests nonlinear gluon dynamics arising at high parton densities. The larger suppression found in p+Au relative to p+Al collisions exhibits a dependence of the saturation scale, Q2s, on the mass number, A. A linear scaling of the suppression with A1/3 is observed with a slope of −0.09 ± 0.01.
We report measurements of the longitudinal double-spin asymmetry, ALL, for inclusive jet and dijet production in polarized proton-proton collisions at midrapidity and center-of-mass energy s√ = 510 GeV, using the high luminosity data sample collected by the STAR experiment in 2013. These measurements complement and improve the precision of previous STAR measurements at the same center-of-mass energy that probe the polarized gluon distribution function at partonic momentum fraction 0.015 ≲x≲ 0.25. The dijet asymmetries are separated into four jet-pair topologies, which provide further constraints on the x dependence of the polarized gluon distribution function. These measurements are in agreement with previous STAR measurements and with predictions from current next-to-leading order global analyses. They provide more precise data at low dijet invariant mass that will better constraint the shape of the polarized gluon distribution function of the proton.
We report measurements of the longitudinal double-spin asymmetry, ALL, for inclusive jet and dijet production in polarized proton-proton collisions at midrapidity and center-of-mass energy s√ = 510 GeV, using the high luminosity data sample collected by the STAR experiment in 2013. These measurements complement and improve the precision of previous STAR measurements at the same center-of-mass energy that probe the polarized gluon distribution function at partonic momentum fraction 0.015 ≲x≲ 0.25. The dijet asymmetries are separated into four jet-pair topologies, which provide further constraints on the x dependence of the polarized gluon distribution function. These measurements are in agreement with previous STAR measurements and with predictions from current next-to-leading order global analyses. They provide more precise data at low dijet invariant mass that will better constraint the shape of the polarized gluon distribution function of the proton.
We report the first multi-differential measurements of strange hadrons of K−, ϕ and Ξ− yields as well as the ratios of ϕ/K− and ϕ/Ξ− in Au+Au collisions at sNN−−−√=3GeV with the STAR experiment fixed target configuration at RHIC. The ϕ mesons and Ξ− hyperons are measured through hadronic decay channels, ϕ→K+K− and Ξ−→Λπ−. Collision centrality and rapidity dependence of the transverse momentum spectra for these strange hadrons are presented. The 4π yields and ratios are compared to thermal model and hadronic transport model predictions. At this collision energy, thermal model with grand canonical ensemble (GCE) under-predicts the ϕ/K− and ϕ/Ξ− ratios while the result of canonical ensemble (CE) calculations reproduce ϕ/K−, with the correlation length rc∼2.7\,fm, and ϕ/Ξ−, rc∼4.2\,fm, for the 0-10\% central collisions. Hadronic transport models including high mass resonance decays could also describe the ratios. While thermal calculations with GCE work well for strangeness production in high energy collisions, the change to CE at 3GeV implies a rather different medium property at high baryon density.
We report the first multi-differential measurements of strange hadrons of K−, ϕ and Ξ− yields as well as the ratios of ϕ/K− and ϕ/Ξ− in Au+Au collisions at sNN−−−√=3GeV with the STAR experiment fixed target configuration at RHIC. The ϕ mesons and Ξ− hyperons are measured through hadronic decay channels, ϕ→K+K− and Ξ−→Λπ−. Collision centrality and rapidity dependence of the transverse momentum spectra for these strange hadrons are presented. The 4π yields and ratios are compared to thermal model and hadronic transport model predictions. At this collision energy, thermal model with grand canonical ensemble (GCE) under-predicts the ϕ/K− and ϕ/Ξ− ratios while the result of canonical ensemble (CE) calculations reproduce ϕ/K−, with the correlation length rc∼2.7\,fm, and ϕ/Ξ−, rc∼4.2\,fm, for the 0-10\% central collisions. Hadronic transport models including high mass resonance decays could also describe the ratios. While thermal calculations with GCE work well for strangeness production in high energy collisions, the change to CE at 3GeV implies a rather different medium property at high baryon density.
We report the first multi-differential measurements of strange hadrons of K−, ϕ and Ξ− yields as well as the ratios of ϕ/K− and ϕ/Ξ− in Au+Au collisions at sNN−−−√=3GeV with the STAR experiment fixed target configuration at RHIC. The ϕ mesons and Ξ− hyperons are measured through hadronic decay channels, ϕ→K+K− and Ξ−→Λπ−. Collision centrality and rapidity dependence of the transverse spectra for these strange hadrons are presented. The 4π yields and ratios are compared to thermal model and hadronic transport model predictions. At the collision energy, thermal model with grand canonical ensemble (GCE) under-predicts the ϕ/K− ratio while the result of canonical ensemble (CE) calculations reproduce well the ratios of ϕ/K−, with the correlation length rc∼2.7\,fm, and ϕ/Ξ−, rc∼4.2\,fm, for the 0-10\% central collisions. Hadronic transport models including high mass resonance decays could also describe the ratios. While thermal calculations with GCE work well for strangeness production in high energy collisions, the change to CE at 3GeV implies a rather different medium property at high baryon density.
We report the first multi-differential measurements of strange hadrons of K−, ϕ and Ξ− yields as well as the ratios of ϕ/K− and ϕ/Ξ− in Au+Au collisions at sNN−−−√=3GeV with the STAR experiment fixed target configuration at RHIC. The ϕ mesons and Ξ− hyperons are measured through hadronic decay channels, ϕ→K+K− and Ξ−→Λπ−. Collision centrality and rapidity dependence of the transverse momentum spectra for these strange hadrons are presented. The 4π yields and ratios are compared to thermal model and hadronic transport model predictions. At this collision energy, thermal model with grand canonical ensemble (GCE) under-predicts the ϕ/K− ratio while the result of canonical ensemble (CE) calculations reproduce well the ratios of ϕ/K−, with the correlation length rc∼2.7\,fm, and ϕ/Ξ−, rc∼4.2\,fm, for the 0-10\% central collisions. Hadronic transport models including high mass resonance decays could also describe the ratios. While thermal calculations with GCE work well for strangeness production in high energy collisions, the change to CE at 3GeV implies a rather different medium property at high baryon density.
We report on the first multi-differential measurement of ϕ meson and Ξ− hyperon production as well as the ϕ/K− and ϕ/Ξ− ratio in Au+Au collisions at sNN−−−√=3GeV with the STAR experiment under its fixed targ et configuration at RHIC. ϕ mesons and Ξ− hyperons are measured through their hadronic decay channels, ϕ→K+K− and Ξ−→Λπ−. The transverse kinetic energy spectra of K−, ϕ and Ξ− are presented in different centrality and rapidity intervals. The total production yields and the ratios within a 4π coverage are calculated and compared to thermal model predictions. A calculation within the grand canonical ensemble framework shows a clear discrepancy from our measurement. Our data favor the canonical ensemble approach employing local strangeness conservation with a small strangeness correlation length (rc≤4.2 fm) in 0--10\% central Au+Au collisions at sNN−−−√=3GeV.
We report precision measurements of hypernuclei 3ΛH and 4ΛH lifetimes obtained from Au+Au collisions at \snn = 3.0\,GeV and 7.2\,GeV collected by the STAR experiment at RHIC, and the first measurement of 3ΛH and 4ΛH mid-rapidity yields in Au+Au collisions at \snn = 3.0\,GeV. The lifetimes are measured to be 221±15(stat.)±19(syst.)\,ps for 3ΛH and 218±6(stat.)±13(syst.)\,ps for 4ΛH. The pT-integrated yields of 3ΛH and 4ΛH are presented in different centrality and rapidity intervals. It is observed that the shape of the rapidity distribution of 4ΛH is different for 0--10\% and 10--50\% centrality collisions. Thermal model calculations, using the canonical ensemble for strangeness, describes the 3ΛH yield well, while underestimating the 4ΛH yield. Transport models, combining baryonic mean-field and coalescence (JAM) or utilizing dynamical cluster formation via baryonic interactions (PHQMD) for light nuclei and hypernuclei production, approximately describe the measured 3ΛH and 4ΛH yields.
We report precision measurements of hypernuclei 3ΛH and 4ΛH lifetimes obtained from Au+Au collisions at \snn = 3.0\,GeV and 7.2\,GeV collected by the STAR experiment at RHIC, and the first measurement of 3ΛH and 4ΛH mid-rapidity yields in Au+Au collisions at \snn = 3.0\,GeV. 3ΛH and 4ΛH, being the two simplest bound states composed of hyperons and nucleons, are cornerstones in the field of hypernuclear physics. Their lifetimes are measured to be 221±15(stat.)±19(syst.)\,ps for 3ΛH and 218±6(stat.)±13(syst.)\,ps for 4ΛH. The pT-integrated yields of 3ΛH and 4ΛH are presented in different centrality and rapidity intervals. It is observed that the shape of the rapidity distribution of 4ΛH is different for 0--10\% and 10--50\% centrality collisions. Thermal model calculations, using the canonical ensemble for strangeness, describes the 3ΛH yield well, while underestimating the 4ΛH yield. Transport models, combining baryonic mean-field and coalescence (JAM) or utilizing dynamical cluster formation via baryonic interactions (PHQMD) for light nuclei and hypernuclei production, approximately describe the measured 3ΛH and 4ΛH yields. Our measurements provide means to precisely assess our understanding of the fundamental baryonic interactions with strange quarks, which can impact our understanding of more complicated systems involving hyperons, such as the interior of neutron stars or exotic hypernuclei.
We report precision measurements of hypernuclei 3ΛH and 4ΛH lifetimes obtained from Au+Au collisions at \snn = 3.0\,GeV and 7.2\,GeV collected by the STAR experiment at RHIC, and the first measurement of 3ΛH and 4ΛH mid-rapidity yields in Au+Au collisions at \snn = 3.0\,GeV. 3ΛH and 4ΛH, being the two simplest bound states composed of hyperons and nucleons, are cornerstones in the field of hypernuclear physics. Their lifetimes are measured to be 221±15(stat.)±19(syst.)\,ps for 3ΛH and 218±6(stat.)±13(syst.)\,ps for 4ΛH. The pT-integrated yields of 3ΛH and 4ΛH are presented in different centrality and rapidity intervals. It is observed that the shape of the rapidity distribution of 4ΛH is different for 0--10\% and 10--50\% centrality collisions. Thermal model calculations, using the canonical ensemble for strangeness, describes the 3ΛH yield well, while underestimating the 4ΛH yield. Transport models, combining baryonic mean-field and coalescence (JAM) or utilizing dynamical cluster formation via baryonic interactions (PHQMD) for light nuclei and hypernuclei production, approximately describe the measured 3ΛH and 4ΛH yields. Our measurements provide means to precisely assess our understanding of the fundamental baryonic interactions with strange quarks, which can impact our understanding of more complicated systems involving hyperons, such as the interior of neutron stars or exotic hypernuclei.
Understanding gluon density distributions and how they are modified in nuclei are among the most important goals in nuclear physics. In recent years, diffractive vector meson production measured in ultra-peripheral collisions (UPCs) at heavy-ion colliders has provided a new tool for probing the gluon density. In this Letter, we report the first measurement of J/ψ photoproduction off the deuteron in UPCs at the center-of-mass energy sNN−−−√=200 GeV in d+Au collisions. The differential cross section as a function of momentum transfer −t is measured. In addition, data with a neutron tagged in the deuteron-going Zero-Degree Calorimeter is investigated for the first time, which is found to be consistent with the expectation of incoherent diffractive scattering at low momentum transfer. Theoretical predictions based on the Color Glass Condensate saturation model and the gluon shadowing model are compared with the data quantitatively. A better agreement with the saturation model has been observed. With the current measurement, the results are found to be directly sensitive to the gluon density distribution of the deuteron and the deuteron breakup, which provides insights into the nuclear gluonic structure.
Understanding gluon density distributions and how they are modified in nuclei are among the most important goals in nuclear physics. In recent years, diffractive vector meson production measured in ultra-peripheral collisions (UPCs) at heavy-ion colliders has provided a new tool for probing the gluon density. In this Letter, we report the first measurement of J/ψ photoproduction off the deuteron in UPCs at the center-of-mass energy sNN−−−√=200 GeV in d+Au collisions. The differential cross section as a function of momentum transfer −t is measured. In addition, data with a neutron tagged in the deuteron-going Zero-Degree Calorimeter is investigated for the first time, which is found to be consistent with the expectation of incoherent diffractive scattering at low momentum transfer. Theoretical predictions based on the Color Glass Condensate saturation model and the gluon shadowing model are compared with the data quantitatively. A better agreement with the saturation model has been observed. With the current measurement, the results are found to be directly sensitive to the gluon density distribution of the deuteron and the deuteron breakup, which provides insights into the nuclear gluonic structure.
The chiral magnetic effect (CME) is predicted to occur as a consequence of a local violation of P and CP symmetries of the strong interaction amidst a strong electro-magnetic field generated in relativistic heavy-ion collisions. Experimental manifestation of the CME involves a separation of positively and negatively charged hadrons along the direction of the magnetic field. Previous measurements of the CME-sensitive charge-separation observables remain inconclusive because of large background contributions. In order to better control the influence of signal and backgrounds, the STAR Collaboration performed a blind analysis of a large data sample of approximately 3.8 billion isobar collisions of 9644Ru+9644Ru and 9640Zr+9640Zr at sNN−−−√=200 GeV. Prior to the blind analysis, the CME signatures are predefined as a significant excess of the CME-sensitive observables in Ru+Ru collisions over those in Zr+Zr collisions, owing to a larger magnetic field in the former. A precision down to 0.4% is achieved, as anticipated, in the relative magnitudes of the pertinent observables between the two isobar systems. Observed differences in the multiplicity and flow harmonics at the matching centrality indicate that the magnitude of the CME background is different between the two species. No CME signature that satisfies the predefined criteria has been observed in isobar collisions in this blind analysis.
The STAR collaboration presents jet substructure measurements related to both the momentum fraction and the opening angle within jets in p+p and Au+Au collisions at sNN−−−√=200 GeV. The substructure observables include SoftDrop groomed momentum fraction (zg), groomed jet radius (Rg), and subjet momentum fraction ((zSJ)) and opening angle ((θSJ)). The latter observable is introduced for the first time. Fully corrected subjet measurements are presented for p+p collisions and are compared to leading order Monte Carlo models. The subjet θSJ distributions reflect the jets leading opening angle and are utilized as a proxy for the resolution scale of the medium in Au+Au collisions. We compare data from Au+Au collisions to those from p+p which are embedded in minimum-bias Au+Au events in order to include the effects of detector smearing and the heavy-ion collision underlying event. The subjet observables are shown to be more robust to the background than zg and (Rg).
We observe no significant modifications of the subjet observables within the two highest-energy, back-to-back jets, resulting in a distribution of opening angles and the splittings that are vacuum-like. We also report measurements of the differential di-jet momentum imbalance (AJ) for jets of varying θg. We find no qualitative differences in energy loss signatures for varying angular scales in the range 0.1<θSJ<0.3, leading to the possible interpretation that energy loss in this population of high momentum di-jet pairs, is due to soft medium-induced gluon radiation from a single color-charge as it traverses the medium.
The STAR collaboration presents jet substructure measurements related to both the momentum fraction and the opening angle within jets in \pp and \AuAu collisions at \sqrtsn =200 GeV. The substructure observables include SoftDrop groomed momentum fraction (\zg), groomed jet radius (\rg), and subjet momentum fraction (\zsj) and opening angle (\tsj). The latter observable is introduced for the first time. Fully corrected subjet measurements are presented for \pp collisions and are compared to leading order Monte Carlo models. The subjet \tsj~distributions reflect the jets leading opening angle and are utilized as a proxy for the resolution scale of the medium in \AuAu collisions. We compare data from \AuAu collisions to those from \pp which are embedded in minimum-bias \AuAu events in order to include the effects of detector smearing and the heavy-ion collision underlying event. The subjet observables are shown to be more robust to the background than \zg~and \rg.
We observe no significant modifications of the subjet observables within the two highest-energy, back-to-back jets, resulting in a distribution of opening angles and the splittings that are vacuum-like. We also report measurements of the differential di-jet momentum imbalance (AJ) for jets of varying \tsj. We find no qualitative differences in energy loss signatures for varying angular scales in the range 0.1< \tsj <0.3, leading to the possible interpretation that energy loss in this population of high momentum di-jet pairs, is due to soft medium-induced gluon radiation from a single color-charge as it traverses the medium.
Measurement of cold nuclear matter effects for inclusive J/ψ in p+Au collisions at √sNN = 200 GeV
(2021)
Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive J/ψ at mid-rapidity in p+Au collisions at sNN−−−√ = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, RpAu, obtained by taking a ratio of J/ψ yield in p+Au collisions to that in p+p collisions scaled by the number of binary nucleon-nucleon collisions. The differential J/ψ yield in both p+p and p+Au collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the J/ψ RpAu is derived within the transverse momentum (pT) range of 0 to 10 GeV/c. A suppression of approximately 30% is observed for pT<2 GeV/c, while J/ψ RpAu becomes compatible with unity for pT greater than 3 GeV/c, indicating the J/ψ yield is minimally affected by the CNM effects at high pT. Comparison to a similar measurement from 0-20% central Au+Au collisions reveals that the observed strong J/ψ suppression above 3 Gev/c is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured J/ψ RpAu, while their agreement with the J/ψ yield in p+p and p+Au collisions is worse.
Measurement of cold nuclear matter effects for inclusive J/ψ in p+Au collisions at √sNN = 200 GeV
(2022)
Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive J/ψ at mid-rapidity in 0-100\% p+Au collisions at sNN−−−√ = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, RpAu, obtained by taking a ratio of J/ψ yield in p+Au collisions to that in p+p collisions scaled by the number of binary nucleon-nucleon collisions. The differential J/ψ yield in both p+p and p+Au collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the J/ψ RpAu is derived within the transverse momentum (pT) range of 0 to 10 GeV/c. A suppression of approximately 30% is observed for pT<2 GeV/c, while J/ψ RpAu becomes compatible with unity for pT greater than 3 GeV/c, indicating the J/ψ yield is minimally affected by the CNM effects at high pT. Comparison to a similar measurement from 0-20% central Au+Au collisions reveals that the observed strong J/ψ suppression above 3 Gev/c is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured J/ψ RpAu, while their agreement with the J/ψ yields in p+p and p+Au collisions is worse.
We report a new measurement of the production cross section for inclusive electrons from open heavy-flavor hadron decays as a function of transverse momentum (pT) at mid-rapidity (|y|< 0.7) in p+p collisions at s√=200 GeV. The result is presented for 2.5 <pT< 10 GeV/c with an improved precision at high pT with respect to the previous measurements, and thus provides a better constraint on perturbative QCD calculations. Moreover, this measurement also provides a high-precision reference for measurements of nuclear modification factors for inclusive electrons from open-charm and -bottom hadron decays in heavy-ion collisions.
We report a new measurement of the production cross section for inclusive electrons from open heavy-flavor hadron decays as a function of transverse momentum (pT) at mid-rapidity (|y|< 0.7) in p+p collisions at s√=200 GeV. The result is presented for 2.5 <pT< 10 GeV/c with an improved precision above 6 GeV/c with respect to the previous measurements, providing more constraints on perturbative QCD calculations. Moreover, this measurement also provides a high-precision reference for measurements of nuclear modification factors for inclusive electrons from open-charm and -bottom hadron decays in heavy-ion collisions.
Partons traversing the strongly interacting medium produced in heavy-ion collisions are expected to lose energy depending on their color charge and mass. We measure the nuclear modification factors for charm- and bottom-decay electrons, defined as the ratio of yields, scaled by the number of binary nucleon-nucleon collisions, in sNN−−−√ = 200 GeV Au+Au collisions to p+p collisions (RAA), or in central to peripheral Au+Au collisions (RCP). We find the bottom-decay electron RAA and RCP to be significantly higher than that of charm-decay electrons. Model calculations including mass-dependent parton energy loss in a strongly coupled medium are consistent with the measured data. These observations provide clear evidence of mass ordering of charm and bottom quark energy loss when traversing through the strongly coupled medium created in heavy-ion collisions.
Partons traversing the strongly interacting medium produced in heavy-ion collisions are expected to lose energy depending on their color charge and mass. We measure the nuclear modification factors for charm- and bottom-decay electrons, defined as the ratio of yields, scaled by the number of binary nucleon-nucleon collisions, in sNN−−−√ = 200 GeV Au+Au collisions to p+p collisions (RAA), or in central to peripheral Au+Au collisions (RCP). We find the bottom-decay electron RAA and RCP to be significantly higher than that of charm-decay electrons. Model calculations including mass-dependent parton energy loss in a strongly coupled medium are consistent with the measured data. These observations provide clear evidence of mass ordering of charm and bottom quark energy loss when traversing through the strongly coupled medium created in heavy-ion collisions.
Partons traversing the strongly interacting medium produced in heavy-ion collisions are expected to lose energy depending on their color charge and mass. We measure the nuclear modification factors for charm- and bottom-decay electrons, defined as the ratio of yields, scaled by the number of binary nucleon-nucleon collisions, in sNN−−−√ = 200 GeV Au+Au collisions to p+p collisions (RAA), or in central to peripheral Au+Au collisions (RCP). We find the bottom-decay electron RAA and RCP to be significantly higher than that of charm-decay electrons. Model calculations including mass-dependent parton energy loss in a strongly coupled medium are consistent with the measured data. These observations provide clear evidence of mass ordering of charm and bottom quark energy loss when traversing through the strongly coupled medium created in heavy-ion collisions.
Partons traversing the strongly interacting medium produced in heavy-ion collisions are expected to lose energy depending on their color charge and mass. We measure the nuclear modification factors for charm- and bottom-decay electrons, defined as the ratio of yields, scaled by the number of binary nucleon-nucleon collisions, in sNN−−−√ = 200 GeV Au+Au collisions to p+p collisions (RAA), or in central to peripheral Au+Au collisions (RCP). We find the bottom-decay electron RAA and RCP to be significantly higher than that of charm-decay electrons. Model calculations including mass-dependent parton energy loss in a strongly coupled medium are consistent with the measured data. These observations provide clear evidence of mass ordering of charm and bottom quark energy loss when traversing through the strongly coupled medium created in heavy-ion collisions.
Partons traversing the strongly interacting medium produced in heavy-ion collisions are expected to lose energy depending on their color charge and mass. We measure the nuclear modification factors for charm- and bottom-decay electrons, defined as the ratio of yields, scaled by the number of binary nucleon-nucleon collisions, in sNN−−−√ = 200 GeV Au+Au collisions to p+p collisions (RAA), or in central to peripheral Au+Au collisions (RCP). We find the bottom-decay electron RAA and RCP to be significantly higher than that of charm-decay electrons. Model calculations including mass-dependent parton energy loss in a strongly coupled medium are consistent with the measured data. These observations provide clear evidence of mass ordering of charm and bottom quark energy loss when traversing through the strongly coupled medium created in heavy-ion collisions.
In high-energy heavy-ion collisions, partonic collectivity is evidenced by the constituent quark number scaling of elliptic flow anisotropy for identified hadrons. A breaking of this scaling and dominance of baryonic interactions is found for identified hadron collective flow measurements in sNN−−−√ = 3 GeV Au+Au collisions. In this paper, we report measurements of the first- and second-order azimuthal anisotropic parameters, v1 and v2, of light nuclei (d, t, 3He, 4He) produced in sNN−−−√ = 3 GeV Au+Au collisions at the STAR experiment. An atomic mass number scaling is found in the measured v1 slopes of light nuclei at mid-rapidity. For the measured v2 magnitude, a strong rapidity dependence is observed. Unlike v2 at higher collision energies, the v2 values at mid-rapidity for all light nuclei are negative and no scaling is observed with the atomic mass number. Calculations by the Jet AA Microscopic Transport Model (JAM), with baryonic mean-field plus nucleon coalescence, are in good agreement with our observations, implying baryonic interactions dominate the collective dynamics in 3 GeV Au+Au collisions at RHIC.
In high-energy heavy-ion collisions, partonic collectivity is evidenced by the constituent quark number scaling of elliptic flow anisotropy for identified hadrons. A breaking of this scaling and dominance of baryonic interactions is found for identified hadron collective flow measurements in sNN−−−√ = 3 GeV Au+Au collisions. In this paper, we report measurements of the first-order and second-order azimuthal anisotropic parameters, v1 and v2, of light nuclei (d, t, 3He, 4He) produced in sNN−−−√ = 3 GeV Au+Au collisions at the STAR experiment. An atomic mass number scaling is found in the measured v1 slopes of light nuclei at mid-rapidity. For the measured v2 magnitude, a strong rapidity dependence is observed. Unlike v2 at higher collision energies, the v2 values at mid-rapidity for all light nuclei are negative and no scaling is observed with the atomic mass number. Calculations by the Jet AA Microscopic Transport Model (JAM), with baryonic mean-field plus nucleon coalescence, are in good agreement with our observations, implying baryonic interactions dominate the collective dynamics in 3 GeV Au+Au collisions at RHIC.
A linearly polarized photon can be quantized from the Lorentz-boosted electromagnetic field of a nucleus traveling at ultrarelativistic speed. When two relativistic heavy nuclei pass one another at a distance of a few nuclear radii, the photon from one nucleus may interact through a virtual quark-antiquark pair with gluons from the other nucleus, forming a short-lived vector meson (e.g., ρ0). In this experiment, the polarization was used in diffractive photoproduction to observe a unique spin interference pattern in the angular distribution of ρ0 → π+π− decays. The observed interference is a result of an overlap of two wave functions at a distance an order of magnitude larger than the ρ0 travel distance within its lifetime. The strong-interaction nuclear radii were extracted from these diffractive interactions and found to be 6.53 ± 0.06 fm (197Au) and 7.29 ± 0.08 fm (238U), larger than the nuclear charge radii. The observable is demonstrated to be sensitive to the nuclear geometry and quantum interference of nonidentical particles. Polarized photon-gluon fusion reveals quantum wave interference of non-identical particles and shape of high-energy nuclei.
We report cumulants of the proton multiplicity distribution from dedicated fixed-target Au+Au collisions at 3.0 GeV, measured by the STAR experiment in the kinematic acceptance of rapidity (y) and transverse momentum (pT) within −0.5<y<0 and 0.4<pT<2.0 GeV/c. In the most central 0--5\% collisions, a proton cumulant ratio is measured to be C4/C2=−0.85±0.09 (stat.)±0.82 (syst.), which is less than unity, the Poisson baseline. The hadronic transport UrQMD model reproduces our C4/C2 in the measured acceptance. Compared to higher energy results and the transport model calculations, the suppression in C4/C2 is consistent with fluctuations driven by baryon number conservation and indicates an energy regime dominated by hadronic interactions. These data imply that the QCD critical region, if created in heavy-ion collisions, could only exist at energies higher than 3\,GeV.
We report cumulants of the proton multiplicity distribution from dedicated fixed-target Au+Au collisions at 3.0 GeV, measured by the STAR experiment in the kinematic acceptance of rapidity (y) and transverse momentum (pT) within −0.5<y<0 and 0.4<pT<2.0 GeV/c. In the most central 0--5\% collisions, a proton cumulant ratio is measured to be C4/C2=−0.85±0.09 (stat.)±0.82 (syst.), which is less than unity, the Poisson baseline. The hadronic transport UrQMD model reproduces our C4/C2 in the measured acceptance. Compared to higher energy results and the transport model calculations, the suppression in C4/C2 is consistent with fluctuations driven by baryon number conservation and indicates an energy regime dominated by hadronic interactions. These data imply that the QCD critical region, if created in heavy-ion collisions, could only exist at energies higher than 3\,GeV.
We report cumulants of the proton multiplicity distribution from dedicated fixed-target Au+Au collisions at sNN−−−√ = 3.0 GeV, measured by the STAR experiment in the kinematic acceptance of rapidity (y) and transverse momentum (pT) within −0.5<y<0 and 0.4<pT<2.0 GeV/c. In the most central 0--5\% collisions, a proton cumulant ratio is measured to be C4/C2=−0.85±0.09 (stat.)±0.82 (syst.), which is less than unity, the Poisson baseline. The hadronic transport UrQMD model reproduces our C4/C2 in the measured acceptance. Compared to higher energy results and the transport model calculations, the suppression in C4/C2 is consistent with fluctuations driven by baryon number conservation and indicates an energy regime dominated by hadronic interactions. These data imply that the QCD critical region, if created in heavy-ion collisions, could only exist at energies higher than 3\,GeV.
Two-particle correlations on transverse rapidity in Au+Au collisions at √sNN = 200 GeV at STAR
(2022)
Two-particle correlation measurements projected onto two-dimensional, transverse rapidity coordinates (yT1,yT2), allow access to dynamical properties of the QCD medium produced in relativistic heavy-ion collisions that angular correlation measurements are not sensitive to. We report non-identified charged-particle correlations for Au + Au minimum-bias collisions at sNN−−−√ = 200 GeV taken by the STAR experiment at the Relativistic Heavy-Ion Collider (RHIC). Correlations are presented as 2D functions of transverse rapidity for like-sign, unlike-sign and all charged-particle pairs, as well as for particle pairs whose relative azimuthal angles lie on the near-side, the away-side, or at all relative azimuth. The correlations are constructed using charged particles with transverse momentum pT≥0.15 GeV/c, pseudorapidity from −1 to 1, and azimuthal angles from −π to π. The significant correlation structures that are observed evolve smoothly with collision centrality. The major correlation features include a saddle shape plus a broad peak with maximum near yT≈3, corresponding to pT≈ 1.5 GeV/c. The broad peak is observed in both like- and unlike-sign charge combinations and in near- and away-side relative azimuthal angles. The all-charge, all-azimuth correlation measurements are compared with the theoretical predictions of {\sc hijing} and {\sc epos}. The results indicate that the correlations for peripheral to mid-central collisions can be approximately described as a superposition of nucleon + nucleon collisions with minimal effects from the QCD medium. Strong medium effects are indicated in mid- to most-central collisions.
A linearly polarized photon can be quantized from the Lorentz-boosted electromagnetic field of a nucleus traveling at ultra-relativistic speed. When two relativistic heavy nuclei pass one another at a distance of a few nuclear radii, the photon from one nucleus may interact through a virtual quark-antiquark pair with gluons from the other nucleus forming a short-lived vector meson (e.g. ρ0). In this experiment, the polarization was utilized in diffractive photoproduction to observe a unique spin interference pattern in the angular distribution of ρ0→π+π− decays. The observed interference is a result of an overlap of two wave functions at a distance an order of magnitude larger than the ρ0 travel distance within its lifetime. The strong-interaction nuclear radii were extracted from these diffractive interactions, and found to be 6.53±0.06 fm (197Au) and 7.29±0.08 fm (238U), larger than the nuclear charge radii. The observable is demonstrated to be sensitive to the nuclear geometry and quantum interference of non-identical particles.
Notwithstanding decades of progress since Yukawa first developed a description of the force between nucleons in terms of meson exchange, a full understanding of the strong interaction remains a major challenge in modern science. One remaining difficulty arises from the non-perturbative nature of the strong force, which leads to the phenomenon of quark confinement at distances on the order of the size of the proton. Here we show that in relativistic heavy-ion collisions, where quarks and gluons are set free over an extended volume, two species of produced vector (spin-1) mesons, namely ϕ and K∗0, emerge with a surprising pattern of global spin alignment. In particular, the global spin alignment for ϕ is unexpectedly large, while that for K∗0 is consistent with zero. The observed spin-alignment pattern and magnitude for the ϕ cannot be explained by conventional mechanisms, while a model with a connection to strong force fields, i.e. an effective proxy description within the Standard Model and Quantum Chromodynamics, accommodates the current data. This connection, if fully established, will open a potential new avenue for studying the behaviour of strong force fields.
The strong force, as one of the four fundamental forces at work in the universe, governs interactions of quarks and gluons, and binds together the atomic nucleus. Notwithstanding decades of progress since Yukawa first developed a description of the force between nucleons in terms of meson exchange, a full understanding of the strong interaction remains a major challenge in modern science. One remaining difficulty arises from the non-perturbative nature of the strong force, which leads to the phenomenon of quark confinement at distance scales on the order of the size of the proton. Here we show that in relativistic heavy-ion collisions, where quarks and gluons are set free over an extended volume, two species of produced vector (spin-1) mesons, namely ϕ and K∗0, emerge with a surprising pattern of global spin alignment. In particular, the global spin alignment for ϕ is unexpectedly large, while that for K∗0 is consistent with zero. The observed spin-alignment pattern and magnitude for the ϕ cannot be explained by conventional mechanisms, while a model with strong force fields accommodates the current data. This is the first time that the strong force field is experimentally supported as a key mechanism that leads to global spin alignment. We extract a quantity proportional to the intensity of the field of the strong force. Within the framework of the Standard Model, where the strong force is typically described in the quark and gluon language of Quantum Chromodynamics, the field being considered here is an effective proxy description. This is a qualitatively new class of measurement, which opens a new avenue for studying the behaviour of strong force fields via their imprint on spin alignment.
The strong force, as one of the four fundamental forces at work in the universe, governs interactions of quarks and gluons, and binds together the atomic nucleus. Notwithstanding decades of progress since Yukawa first developed a description of the force between nucleons in terms of meson exchange, a full understanding of the strong interaction remains a major challenge in modern science. One remaining difficulty arises from the non-perturbative nature of the strong force, which leads to the phenomenon of quark confinement at distance scales on the order of the size of the proton. Here we show that in relativistic heavy-ion collisions, where quarks and gluons are set free over an extended volume, two species of produced vector (spin-1) mesons, namely ϕ and K∗0, emerge with a surprising pattern of global spin alignment. In particular, the global spin alignment for ϕ is unexpectedly large, while that for K∗0 is consistent with zero. The observed spin-alignment pattern and magnitude for the ϕ cannot be explained by conventional mechanisms, while a model with strong force fields accommodates the current data. This is the first time that the strong force field is experimentally supported as a key mechanism that leads to global spin alignment. We extract a quantity proportional to the intensity of the field of the strong force. Within the framework of the Standard Model, where the strong force is typically described in the quark and gluon language of Quantum Chromodynamics, the field being considered here is an effective proxy description. This is a qualitatively new class of measurement, which opens a new avenue for studying the behaviour of strong force fields via their imprint on spin alignment.
In high-energy heavy-ion collisions, partonic collectivity is evidenced by the constituent quark number scaling of elliptic flow anisotropy for identified hadrons. A breaking of this scaling and dominance of baryonic interactions is found for identified hadron collective flow measurements in √sNN = 3 GeV Au+Au collisions. In this paper, we report measurements of the first- and second-order azimuthal anisotropic parameters, v1 and v2, of light nuclei (d, t, 3He, 4He) produced in √sNN = 3 GeV Au+Au collisions at the STAR experiment. An atomic mass number scaling is found in the measured v1 slopes of light nuclei at mid-rapidity. For the measured v2 magnitude, a strong rapidity dependence is observed. Unlike v2 at higher collision energies, the v2 values at mid-rapidity for all light nuclei are negative and no scaling is observed with the atomic mass number. Calculations by the Jet AA Microscopic Transport Model (JAM), with baryonic mean-field plus nucleon coalescence, are in good agreement with our observations, implying baryonic interactions dominate the collective dynamics in 3 GeV Au+Au collisions at RHIC.
We report on the measurements of directed flow v1 and elliptic flow v2 for hadrons (π±, K ±, K0 S , p, φ, Λ and ) from Au+Au collisions at √sN N = 3 GeV and v2 for (π±, K ±, p and p) at 27 and 54.4 GeV with the STAR experiment. While at the two higher energy midcentral collisions the numberof-constituent-quark (NCQ) scaling holds, at 3 GeV the v2 at midrapidity is negative for all hadrons and the NCQ scaling is absent. In addition, the v1 slopes at midrapidity for almost all observed hadrons are found to be positive, implying dominant repulsive baryonic interactions. The features of negative v2 and positive v1 slope at 3 GeV can be reproduced with a baryonic mean-field in transport model calculations. These results imply that the medium in such collisions is likely characterized by baryonic interactions.
Measurement of cold nuclear matter effects for inclusive J/ψ in p+Au collisions at √sNN = 200 GeV
(2022)
Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive J/ψ at mid-rapidity in 0-100% p+Au collisions at √sNN = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, RpAu, obtained by taking a ratio of J/ψ yield in p+Au collisions to that in p+p collisions scaled by the number of binary nucleon-nucleon collisions. The differential J/ψ yield in both p+p and p+Au collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the J/ψ RpAu is derived within the transverse momentum (pT) range of 0 to 10 GeV/c. A suppression of approximately 30% is observed for pT < 2 GeV/c, while J/ψ RpAu becomes compatible with unity for pT greater than 3 GeV/c, indicating the J/ψ yield is minimally affected by the CNM effects at high pT. Comparison to a similar measurement from 0-20% central Au+Au collisions reveals that the observed strong J/ψ suppression above 3 GeV/c is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured J/ψ RpAu, while their agreement with the J/ψ yields in p+p and p+Au collisions is worse.
We report the first multi-differential measurements of strange hadrons of K −, φ and − yields as well as the ratios of φ/K − and φ/− in Au+Au collisions at √sNN = 3 GeV with the STAR experiment fixed target configuration at RHIC. The φ mesons and − hyperons are measured through hadronic decay channels, φ → K + K − and Ξ− → Λπ−. Collision centrality and rapidity dependence of the transverse momentum spectra for these strange hadrons are presented. The 4π yields and ratios are compared to thermal model and hadronic transport model predictions. At this collision energy, thermal model with grand canonical ensemble (GCE) under-predicts the φ/K − and φ/− ratios while the result of canonical ensemble (CE) calculations reproduce φ/K −, with the correlation length rc ∼ 2.7 fm, and φ/−, rc ∼ 4.2 fm, for the 0-10% central collisions. Hadronic transport models including high mass resonance decays could also describe the ratios. While thermal calculations with GCE work well for strangeness production in high energy collisions, the change to CE at 3 GeV implies a rather different medium property at high baryon density.
Measurements of mass and Λ binding energy of 4ΛH and 4ΛHe in Au+Au collisions at sNN−−−√=3 GeV are presented, with an aim to address the charge symmetry breaking (CSB) problem in hypernuclei systems with atomic number A = 4. The Λ binding energies are measured to be 2.22±0.06(stat.)±0.14(syst.) MeV and 2.38±0.13(stat.)±0.12(syst.) MeV for 4ΛH and 4ΛHe, respectively. The measured Λ binding-energy difference is 0.16±0.14(stat.)±0.10(syst.) MeV for ground states. Combined with the γ-ray transition energies, the binding-energy difference for excited states is −0.16±0.14(stat.)±0.10(syst.) MeV, which is negative and comparable to the value of the ground states within uncertainties. These new measurements on the Λ binding-energy difference in A = 4 hypernuclei systems are consistent with the theoretical calculations that result in ΔB4Λ(1+exc)≈−ΔB4Λ(0+g.s.)<0 and present a new method for the study of CSB effect using relativistic heavy-ion collisions.
Measurements of mass and Λ binding energy of 4ΛH and 4ΛHe in Au+Au collisions at sNN−−−√=3 GeV are presented, with an aim to address the charge symmetry breaking (CSB) problem in hypernuclei systems with atomic number A = 4. The Λ binding energies are measured to be 2.22±0.06(stat.)±0.14(syst.) MeV and 2.38±0.13(stat.)±0.12(syst.) MeV for 4ΛH and 4ΛHe, respectively. The measured Λ binding-energy difference is 0.16±0.14(stat.)±0.10(syst.) MeV for ground states. Combined with the γ-ray transition energies, the binding-energy difference for excited states is −0.16±0.14(stat.)±0.10(syst.) MeV, which is negative and comparable to the value of the ground states within uncertainties. These new measurements on the Λ binding-energy difference in A = 4 hypernuclei systems are consistent with the theoretical calculations that result in ΔB4Λ(1+exc)≈−ΔB4Λ(0+g.s.)<0 and present a new method for the study of CSB effect using relativistic heavy-ion collisions.
Measurements of mass and Λ binding energy of 4ΛH and 4ΛHe in Au+Au collisions at sNN−−−√=3 GeV are presented, with an aim to address the charge symmetry breaking (CSB) problem in hypernuclei systems with atomic number A = 4. The Λ binding energies are measured to be 2.22±0.06(stat.)±0.14(syst.) MeV and 2.38±0.13(stat.)±0.12(syst.) MeV for 4ΛH and 4ΛHe, respectively. The measured Λ binding-energy difference is 0.16±0.14(stat.)±0.10(syst.) MeV for ground states. Combined with the γ-ray transition energies, the binding-energy difference for excited states is −0.16±0.14(stat.)±0.10(syst.) MeV, which is negative and comparable to the value of the ground states within uncertainties. These new measurements on the Λ binding-energy difference in A = 4 hypernuclei systems are consistent with the theoretical calculations that result in ΔB4Λ(1+exc)≈−ΔB4Λ(0+g.s.)<0 and present a new method for the study of CSB effect using relativistic heavy-ion collisions.
Azimuthal anisotropy measurement of (multi-)strange hadrons in Au+Au collisions at √sNN = 54.4 GeV
(2023)
Azimuthal anisotropy of produced particles is one of the most important observables used to access the collective properties of the expanding medium created in relativistic heavy-ion collisions. In this paper, we present second (v2) and third (v3) order azimuthal anisotropies of K0S, ϕ, Λ, Ξ and Ω at mid-rapidity (|y|<1) in Au+Au collisions at sNN−−−√ = 54.4 GeV measured by the STAR detector. The v2 and v3 are measured as a function of transverse momentum and centrality. Their energy dependence is also studied. v3 is found to be more sensitive to the change in the center-of-mass energy than v2. Scaling by constituent quark number is found to hold for v2 within 10%. This observation could be evidence for the development of partonic collectivity in 54.4 GeV Au+Au collisions. Differences in v2 and v3 between baryons and anti-baryons are presented, and ratios of v3/v3/22 are studied and motivated by hydrodynamical calculations. The ratio of v2 of ϕ mesons to that of anti-protons (v2(ϕ)/v2(p¯)) shows centrality dependence at low transverse momentum, presumably resulting from the larger effects from hadronic interactions on anti-proton v2.
We report the measurement of K∗0 meson at midrapidity (|y|< 1.0) in Au+Au collisions at sNN−−−√~=~7.7, 11.5, 14.5, 19.6, 27 and 39 GeV collected by the STAR experiment during the RHIC beam energy scan (BES) program. The transverse momentum spectra, yield, and average transverse momentum of K∗0 are presented as functions of collision centrality and beam energy. The K∗0/K yield ratios are presented for different collision centrality intervals and beam energies. The K∗0/K ratio in heavy-ion collisions are observed to be smaller than that in small system collisions (e+e and p+p). The K∗0/K ratio follows a similar centrality dependence to that observed in previous RHIC and LHC measurements. The data favor the scenario of the dominance of hadronic re-scattering over regeneration for K∗0 production in the hadronic phase of the medium.
We report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at sNN−−−√ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum (pT) region −0.9<y<0 and 0.4<pT<2.0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, pT, and y are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5\% collisions, the value of proton cumulant ratio C4/C2 is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of C4/C2 at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions.
We present the first measurements of transverse momentum spectra of π±, K±, p(p¯) at midrapidity (|y|<0.1) in U+U collisions at √sNN = 193 GeV with the STAR detector at the Relativistic Heavy Ion Collider (RHIC). The centrality dependence of particle yields, average transverse momenta, particle ratios and kinetic freeze-out parameters are discussed. The results are compared with the published results from Au+Au collisions at sNN−−−−√= 200 GeV in STAR. The results are also compared to those from A Multi Phase Transport (AMPT) model.
Elliptic flow measurements from two-, four- and six-particle correlations are used to investigate flow fluctuations in collisions of U+U at sNN−−−√ = 193 GeV, Cu+Au at sNN−−−√ = 200 GeV and Au+Au spanning the range sNN−−−√ = 11.5 - 200 GeV. The measurements show a strong dependence of the flow fluctuations on collision centrality, a modest dependence on system size, and very little if any, dependence on particle species and beam energy. The results, when compared to similar LHC measurements, viscous hydrodynamic calculations, and Glauber model eccentricities, indicate that initial-state-driven fluctuations predominate the flow fluctuations generated in the collisions studied.
Elliptic flow measurements from two-, four- and six-particle correlations are used to investigate flow fluctuations in collisions of U+U at sNN−−−√= 193 GeV, Cu+Au at sNN−−−√= 200 GeV and Au+Au spanning the range sNN−−−√= 11.5 - 200 GeV. The measurements show a strong dependence of the flow fluctuations on collision centrality, a modest dependence on system size, and very little if any, dependence on particle species and beam energy. The results, when compared to similar LHC measurements, viscous hydrodynamic calculations, and T$\mathrel{\protect\raisebox{-2.1pt}{R}}$ENTo model eccentricities, indicate that initial-state-driven fluctuations predominate the flow fluctuations generated in the collisions studied.
We report high-precision measurements of the longitudinal double-spin asymmetry, 𝐴𝐿𝐿, for midrapidity inclusive jet and dijet production in polarized 𝑝𝑝 collisions at a center-of-mass energy of √𝑠=200 GeV. The new inclusive jet data are sensitive to the gluon helicity distribution, Δ𝑔(𝑥,𝑄2), for gluon momentum fractions in the range from 𝑥≃0.05 to 𝑥≃0.5, while the new dijet data provide further constraints on the 𝑥 dependence of Δ𝑔(𝑥,𝑄2). The results are in good agreement with previous measurements at √𝑠=200 GeV and with recent theoretical evaluations of prior world data. Our new results have better precision and thus strengthen the evidence that Δ𝑔(𝑥,𝑄2) is positive for 𝑥>0.05.
We present the first inclusive measurements of the invariant and SoftDrop jet mass in proton-proton collisions at s√=200 GeV at STAR. The measurements are fully corrected for detector effects, and reported differentially in both the jet transverse momentum and jet radius parameter. We compare the measurements to established leading-order Monte Carlo event generators and find that STAR-tuned PYTHIA-6 reproduces the data, while LHC tunes of PYTHIA-8 and HERWIG-7 do not agree with the data, providing further constraints on parameter tuning. Finally, we observe that SoftDrop grooming, for which the contribution of wide-angle non-perturbative radiation is suppressed, shifts the jet mass distributions into closer agreement with the partonic jet mass as determined by both PYTHIA-8 and a next-to-leading-logarithmic accuracy perturbative QCD calculation. These measurements complement recent LHC measurements in a different kinematic region, as well as establish a baseline for future jet mass measurements in heavy-ion collisions at RHIC.
We report a systematic measurement of cumulants, Cn, for net-proton, proton and antiproton, and correlation functions, κn, for proton and antiproton multiplicity distributions up to the fourth order in Au+Au collisions at sNN−−−√ = 7.7, 11.5, 14.5, 19.6, 27, 39, 54.4, 62.4 and 200 GeV. The Cn and κn are presented as a function of collision energy, centrality and kinematic acceptance in rapidity, y, and transverse momentum, pT. The data were taken during the first phase of the Beam Energy Scan (BES) program (2010 -- 2017) at the Relativistic Heavy Ion Collider (RHIC) facility. The measurements are carried out at midrapidity (|y|< 0.5) and transverse momentum 0.4 < pT < 2.0 GeV/c, using the STAR detector at RHIC. We observe a non-monotonic energy dependence (sNN−−−√ = 7.7 -- 62.4 GeV) of the net-proton C4/C2 with the significance of 3.1σ for the 0-5\% central Au+Au collisions. This is consistent with the expectations of critical fluctuations in a QCD-inspired model. Thermal and transport model calculations show a monotonic variation with sNN−−−√. For the multiparticle correlation functions, we observe significant negative values for a two-particle correlation function, κ2, of protons and antiprotons, which are mainly due to the effects of baryon number conservation. Furthermore, it is found that the four-particle correlation function, κ4, of protons plays a role in determining the energy dependence of proton C4/C1 below 19.6 GeV, which cannot be solely understood by the negative values of κ2 for protons.
We report a systematic measurement of cumulants, Cn, for net-proton, proton and antiproton multiplicity distributions, and correlation functions, κn, for proton and antiproton multiplicity distributions up to the fourth order in Au+Au collisions at sNN−−−√ = 7.7, 11.5, 14.5, 19.6, 27, 39, 54.4, 62.4 and 200 GeV. The Cn and κn are presented as a function of collision energy, centrality and kinematic acceptance in rapidity, y, and transverse momentum, pT. The data were taken during the first phase of the Beam Energy Scan (BES) program (2010 -- 2017) at the BNL Relativistic Heavy Ion Collider (RHIC) facility. The measurements are carried out at midrapidity (|y|< 0.5) and transverse momentum 0.4 < pT < 2.0 GeV/c, using the STAR detector at RHIC. We observe a non-monotonic energy dependence (sNN−−−√ = 7.7 -- 62.4 GeV) of the net-proton C4/C2 with the significance of 3.1σ for the 0-5\% central Au+Au collisions. This is consistent with the expectations of critical fluctuations in a QCD-inspired model. Thermal and transport model calculations show a monotonic variation with sNN−−−√. For the multiparticle correlation functions, we observe significant negative values for a two-particle correlation function, κ2, of protons and antiprotons, which are mainly due to the effects of baryon number conservation. Furthermore, it is found that the four-particle correlation function, κ4, of protons plays a role in determining the energy dependence of proton C4/C1 below 19.6 GeV, which cannot be understood by the effect of baryon number conservation.
Rationale: The AMP-activated protein kinase (AMPK) is stimulated by hypoxia, and although the AMPKα1 catalytic subunit has been implicated in angiogenesis, little is known about the role played by the AMPKα2 subunit in vascular repair.
Objective: To determine the role of the AMPKα2 subunit in vascular repair.
Methods and Results: Recovery of blood flow after femoral artery ligation was impaired (>80%) in AMPKα2-/- versus wild-type mice, a phenotype reproduced in mice lacking AMPKα2 in myeloid cells (AMPKα2ΔMC). Three days after ligation, neutrophil infiltration into ischemic limbs of AMPKα2ΔMC mice was lower than that in wild-type mice despite being higher after 24 hours. Neutrophil survival in ischemic tissue is required to attract monocytes that contribute to the angiogenic response. Indeed, apoptosis was increased in hypoxic neutrophils from AMPKα2ΔMC mice, fewer monocytes were recruited, and gene array analysis revealed attenuated expression of proangiogenic proteins in ischemic AMPKα2ΔMC hindlimbs. Many angiogenic growth factors are regulated by hypoxia-inducible factor, and hypoxia-inducible factor-1α induction was attenuated in AMPKα2-deficient cells and accompanied by its enhanced hydroxylation. Also, fewer proteins were regulated by hypoxia in neutrophils from AMPKα2ΔMC mice. Mechanistically, isocitrate dehydrogenase expression and the production of α-ketoglutarate, which negatively regulate hypoxia-inducible factor-1α stability, were attenuated in neutrophils from wild-type mice but remained elevated in cells from AMPKα2ΔMC mice.
Conclusions: AMPKα2 regulates α-ketoglutarate generation, hypoxia-inducible factor-1α stability, and neutrophil survival, which in turn determine further myeloid cell recruitment and repair potential. The activation of AMPKα2 in neutrophils is a decisive event in the initiation of vascular repair after ischemia.
Medicinal plants represent a big reservoir for discovering new drugs against all kinds of diseases including inflammation. In spite the large number of promising anti-inflammatory plant extracts and isolated components, research on medicinal plants proves to be very difficult. Based on that background this review aims to provide a summarized insight into the hitherto known pharmacologically active concentrations, bioavailability, and clinical efficacy of boswellic acids, curcumin, quercetin and resveratrol. These examples have in common that the achieved plasma concentrations were found to be often far below the determined IC50 values in vitro. On the other hand demonstrated therapeutic effects suggest a necessity of rethinking our pharmacokinetic understanding. In this light this review discusses the value of plasma levels as pharmacokinetic surrogates in comparison to the more informative value of tissue concentrations. Furthermore the need for new methodological approaches is addressed like the application of combinatorial approaches for identifying and pharmacokinetic investigations of active multi-components. Also the physiological relevance of exemplary in vitro assays and absorption studies in cell-line based models is discussed. All these topics should be ideally considered to avoid inaccurate predictions for the efficacy of herbal components in vivo and to unlock the “black box” of herbal mixtures.
Heute gewinnen pflanzliche Arzneimittel im Zeichen einer verstärkten Hinwendung zu natürlichen, relativ nebenwirkungsarmen Medikamenten zunehmend an Bedeutung, so auch die über Jahrtausende hinweg traditionell angewandte Ginsengwurzel (Panax ginseng) und der Indische Weihrauch (Boswellia serrata). Neben der Struktur- und Extraktanalytik konzentriert sich die Forschung in zunehmenden Maße darauf, die zahlreichen pharmakologisch untersuchten und klinisch beobachteten Wirkungen dieser beiden Arzneipflanzen einzelnen Inhaltsstoffen zuzuordnen. Bei der Ginsengwurzel gestaltet sich dies jedoch besonders schwierig. Dies ist begründet durch die große Anzahl strukturell ähnlicher Ginsenoside sowie durch deren unterschiedlicher Metabolismus. Zwar ist aus In-vitro-Experimenten bekannt, daß die Degradation über die stufenweise Deglukosylierung stattfindet, allerdings ist bislang nicht geklärt, ob intakte Ginsenoside überhaupt resorbiert werden und welche der vielen in vitro ermittelten Degradationsprodukte tatsächlich den systemischen Kreislauf erreichen. Anders als bei Ginseng, kann die therapeutische Wirkung des Indischen Weihrauches wohl definierten Inhaltsstoffen, AKBA und KBA, zugeschrieben werden. Dennoch mangelt es hier an verlässlichen pharmakokinetischen Daten, da bislang keine validierte bioanalytische Methode zur Verfügung stand. Im Rahmen der Bioanalytik von Ginsenosiden und Boswellliasäuren kamen in der vorliegenden Arbeit die Nano-ESI-MS(n)-Technik sowie die HPLC-Analytik zur Anwendung. Bereits bei der Strukturanalyse von Ginsenosiden erwies sich die Kombination der Nano-ESI-Technik mit MS(n)-Experimenten in einer Quadrupol-Ionenfalle als besonders vorteilhaft. Im Vergleich zu konventionellem ESI bietet Nano-ESI nicht nur den Vorzug, mit kleinsten Substanzmengen lange Messungen durchführen zu können, sondern auch den Vorteil einer effektiveren, weniger diskreminierenden Ionisation. Sowohl die hohe Sensitivität der Nano-Elektrosprayionisierung bei der Analyse von glykosidischen Verbindungen als auch die umfangreichen Strukturinformationen infolge mehrerer aufeinanderfolgender stoßinduzierter Fragmentierungen machen diese Technik zu einer attraktiven und effizienten Methode zur Analyse von Ginsenosiden. In MS(n)-Experimenten äußert sich das charakteristische Fragmentierungsverhalten der Ginsenoside in der sequentiellen Abspaltung der Zuckereinheiten in sukkzessiven Fragmentierungsschritten. Mit dieser Methode konnten die Zuckerketten an verschiedenen Positionen des Protopanaxadiol- bzw. Protopanaxatriolaglykons der Ginsenoside identifiziert, die glykosidischen Verknüpfungen innerhalb der einzelnen Zuckereinheiten durch spezifische Ringfragmente bestimmt und die genaue(n) Verknüpfungsposition(en) enzymatisch eingeführter Galaktose(n) lokalisiert werden. Bisher wurden allerdings Nano-ESI-MS/MS bzw. MS(n)-Untersuchungen primär an wässrigen oder organischen Lösungen von isolierten / aufgereinigten Stoffen oder Stoffgemischen durchgeführt. In dieser Arbeit wurde erstmals diese Technik in der Bioanalytik zur Identifizierung von Ginsenosiden und deren Degradationsprodukte in Humanplasma und -urin angewandt. Obwohl die optimale Analytkonzentration für die Nano-Elektrosprayionisierung im allgemeinen bei 10-5M liegt, ist es gelungen, die Ginsenoside anhand ihrer spezifischen Fragmentionen im MS/MS Modus bis zu einer Konzentration von 2 ng/mL (10-8M) in biologischen Matrices nachzuweisen. Auch wenn die Molekülionenpeaks bei diesen geringen Konzentrationen im Rauschen untergehen, können die Ginsenoside durch selektive Isolierung der gewünschten Vorläuferionen und deren anschließende Fragmentierung in der Quadrupol-Ionenfalle auf der Basis der Detektion spezifischer Fragmente identifiziert werden. Da bei der Fragmentierung der gleichen Vorläuferionenmasse in Leerplasma bzw. Urin keine charakteristischen Fragmentionen gebildet werden, handelt es sich somit um einen spezifischen Nachweis der Ginsenoside in biologischen Matrices. Vor dem Hintergrund dieser vielversprechenden Vorversuche wurde eine Pilotstudie zum qualitativen Screening von Ginsenosiden und deren Metaboliten in Humanplasma und –urin durchgeführt. Es konnte gezeigt werden, daß Protopanaxatriol-Ginsenoside sowohl im Magen hydrolysiert als auch intestinal degradiert werden. Schon in den ersten Stunden nach der einmaligen oralen Einnahme von Ginsana G115 Kapseln wurden die Hydrolyseprodukte G-Rh1 und hydratisiertes G-Rh1 in Humanplasma detektiert. Die schnelle Resorption dieser beiden Verbindungen aus dem oberen Gastrointestinaltrakt deutet auf die Hydrolyse des Ginsenosides Rg1 im Magen hin. Das spätere Auftreten eines weiteren monoglukosylierten Protopanaxatriols, des Degradationsproduktes G-F1, liefert den ersten In-Vivo-Hinweis auf einen intestinalen Metabolismus von Protopanaxatriol-Ginsenoside. Im Gegensatz zu den Protopanaxatriolginsenosiden passieren die Protopanaxadiol-Ginsenoside den Magen unverändert, wie aus der Abwesenheit jeglicher Protopanaxadiol-Degradationsprodukte im Plasma und Urin in den ersten Stunden nach der Applikation geschlossen werden kann. Erst im unteren Gastrointestinaltrakt werden Protopanaxadiol-Ginsenoside durch intestinale Bakterien zu „Compound-K“ abgebaut und anschließend resorbiert. Der Nachweis von Ginsenosid Rb1 im Plasma, sowie weiterer Ginsenoside im Urin eines Probanden zeigt, daß auch Ginsenoside in ihrer intakten Form resorbiert werden können. Dennoch sind weitere Studien hierzu notwendig, um zu klären, ob die Resorption intakter Ginsenoside die Regel oder eher eine Ausnahme darstellt. Mit der Identifizierung des Hydrolyseproduktes G-Rh1, der Degradationsprodukte G-F1 sowie „Compound-K“ in Humanplasma und -urin konnte schließlich die Frage geklärt werden, welche der zahlreichen in vitro bestimmten Degradationsprodukte tatsächlich den systemischen Kreislauf erreichen. Damit ist die Basis für eine spätere Quantifizierung dieser Verbindungen nach ihrer Isolierung bzw. Herstellung und Charakterisierung als Referenzsubstanzen geschaffen. Außerdem können diese neuen Erkenntnisse helfen, pharmakologische Ergebnisse aus In-vitro-Versuchen mit In-vivo-Daten besser zu korrelieren, da sie erste Hinweise geben, welche der in vitro getesteten Substanzen für die in vivo beobachteten Effekte verantwortlich sein könnten. Bisher wurde Nano-ESI-MS(n) in der Bioanalytik pflanzlicher Arzneistoffe nicht eingesetzt. In dieser Arbeit wurde diese Technik erstmals zum Screening von Ginsenosiden und deren Degradationsprodukte in Humanplasma und –urin benutzt. Darüber hinaus konnte gezeigt werden, daß Nano-ESI-MS(n) auch eine empfindliche und sensitive Methode zur Identifizierung und zum Nachweis anderer medizinisch relevanter glykosidischer Verbindungen in biologischen Matrices darstellt, woraus sich neue Perspektiven für den Einsatz dieser Technik in der Metabolitenforschung sowie in der Bioanalytik pflanzlicher Xenobiotika ergeben. In den letzten Jahren rückte auch der Indische Weihrauch immer mehr in den Mittelpunkt des wissenschaftlichen sowie therapeutischen Interesses. Aufgrund der selektiven Hemmung der 5-Lipoxygenase gewinnen AKBA und KBA, als neue entzündungshemmende Verbindungen, zunehmend an Bedeutung. Während die quantitative Analytik der Boswelliasäuren in Extrakten und in verschiedenen Fertigarzneimitteln erhebliche Fortschritte erzielen konnte, fehlten auf dem Gebiet der Bioanalytik bislang validierte analytische Methoden zur Durchführung pharmakokinetischer Studien. Vor diesem Hintergrund wurde eine HPLC-Methode zur Bestimmung von KBA in Humanplasma entwickelt und validiert. Die Methode ist durch eine einfache Probenvorbereitung gekennzeichnet, die sich auf eine Festphasenextraktion der KBA aus der komplex zusammengesetzten biologischen Matrix beschränkt. Im Anschluß an die chromatographische Trennung auf einer RP-C18 Säule erfolgt die Quantifizierung der KBA mittels UV-Detektion bei 250 nm. Um eine adäquate Bestimmung der KBA in Humanplasma zu gewährleisten, wurde eine umfassende Validierung durchgeführt. Alle ermittelten Validierungsparameter, wie Spezifität, Linearität, Präzision, Richtigkeit, Reproduzierbarkeit, untere Quantifizierungsgrenze und Stabilität lagen innerhalb der vorgegebenen Grenzen. Damit erfüllt die entwickelte HPLC-Methode die allgemein gültigen Anforderungen an die Validierung bioanalytischer Methoden. Mit der Erstellung einer Plasmakonzentrations-Zeit-Kurve im Rahmen einer ersten Pilotstudie konnte diese Methode zudem ihre praktische Anwendbarkeit unter Beweis stellen. Somit steht für zukünftige pharmakokinetische Studien eine validierte HPLC-Analytik zur Bestimmung von KBA, einer der Hauptwirkstoffe des Indischen Weihrauches, zur Verfügung, die sich durch hohe Spezifität, Reproduzierbarkeit und Präzision auszeichnet. Verlässliche Daten zur Pharmakokinetik am Menschen sind heute von besonderer Bedeutung, da sie helfen, die Dosierung zu optimieren, die biopharmazeutischen Eigenschaften von Präparaten zu verbessern und die Sicherheit bei der Anwendung zu erhöhen. Insbesondere im Hinblick auf bereits festgestellte Interaktionen von pflanzlichen Arzneimitteln mit Medikamenten reicht es nicht mehr aus, wenn sich pflanzliche Arzneimittel, wie beispielsweise Ginseng und Indischer Weihrauch, nur auf ihre langjährigen tradierten Anwendungserfahrungen berufen. So wird auch bei Phytopharmaka in verstärktem Maße eine wissenschaftliche Absicherung durch bioanalytische Forschung erwartet. Mit der Identifizierung der Ginsenoside und deren Degradationsprodukte im Menschen, der erstmaligen Anwendung von Nano-ESI-MS(n) in der Metabolitenforschung und der Entwicklung einer validierten bioanalytischen Methode zur Bestimmung der 11-Keto-Beta-Boswelliasäure in Humanplasma wurde diesen Erfordernissen Rechnung getragen.
Dosing accuracy of two disposable insulin pens according to new ISO 11608-1: 2012 requirements.
(2015)
OBJECTIVE: The aim was to compare 2 disposable insulin pens, FlexTouch® (Novo Nordisk, insulin aspart) and SoloSTAR® (Sanofi, insulin glulisine), according to new ISO 11608-1:2012 requirements for dosing accuracy.
METHODS: Sixty pens of each type were tested at 1, 40, and 80 U doses. Following the new ISO requirements, each dose was delivered from the front, middle, and rear one-third of the pen. Statistical analysis was performed using Student's t test.
RESULTS: Both pens delivered all doses within ISO limits. The difference between the average measured dose and the target dose was significantly smaller for SoloSTAR than FlexTouch at 40 U (P = .009) and 80 U (P = .008), but not at 1 U (P = .417).
CONCLUSION: Both insulin pens fulfilled the dosing accuracy requirements defined by ISO 11608-1:2012 at all 3 dosage levels.