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In “Fern von Aleppo”, the Syrian author Faisal Hamdo, who left his home in 2014 and sought refuge in Germany, tells of his very personal integration experiences. The book represents a kind of intercultural communication. In his book, Faisal Hamdo, who sees himself as a “mediator between the worlds”, tries to give the German reader answers to many questions regarding Syrian culture. From a text linguistic point of view, this book identifies the narrative development that seems to be tailored to the in-tercultural context. Accordingly, the present article raises the following questions: Does the structure of classic narration differ from the structure of narration in an intercultural context? Which intercultural information units are presented in the text? How are they embedded in the narrative text? Which constituents of the narrative structure are suitable for realizing intercultural communication? Which communicative functions do the constituents of the narrative structure fulfill in an intercultural context? The contribution sets itself the goal of analyzing the narrative structure to investigate how intercultural communication comes about through narration, how the intercultural information units are integrated into the constituents of the classic narrative structure so that they fulfill their communicative function, and to developa suitable analysis model.
Objective: The aim of this study was to report the basic cerebrospinal fluid (CSF) profile in patients with primary progressive multiple sclerosis (PPMS).
Methods: The results of CSF analysis from 254 patients with PPMS were collected at four university hospitals in Germany. Routine CSF parameters and different indices of intrathecal immunoglobulin synthesis were evaluated. We assessed possible correlations between the various CSF parameters and the expanded disability status scale (EDSS) both at the time of lumbar puncture and during the course of the disease.
Results: The median cell count and albumin concentration in the CSF did not deviate from normal values. The CSF-serum albumin-quotient (QALB) was elevated in 29.6% of the patients, while intrathecal immunoglobulin G (IgG) oligoclonal bands (OCBs) were detected in 91.1% of the patients. CSF-lactate levels as well as local IgM- and IgA-synthesis were correlated with the yearly disease progression rate, as assessed by EDSS.
Conclusion: We present the results of the hitherto largest and most detailed CSF biomarker profile in a cohort of 254 patients with PPMS. As reported previously, OCBs are the most sensitive marker for intrathecal IgG synthesis. CSF-lactate concentrations are positively correlated with the progression rate, which might suggest that mitochondrial dysfunction plays a relevant role in PPMS. The negative correlation between intrathecally produced IgM and IgA and disease progression may indicate their hitherto unexplored protective role.
18-OH-Corticosteron (18 ) wird als die unmittelbare Vorstufe der Aldosteron-Synthese angesehen. In-vitro-Untersuchungen sowie vereinzelten klinischen Beobachtungen zufolge sollen Nebennierenrinden-Adenome, im Gegensatz zu Nebennierenrinden-Hyperplasie, vermehrt 8- bilden. In der vorliegenden Studie wurde an 1.272 Patienten einer Hochdruckambulanz, wobei bei 84 Patienten mit primärem Aldosteronismus infolge eines Adenoms sowie bei 110 Patienten infolge einer Nebennierenrinden-Hyperplasie die Diagnose gesichert werden konnte, der diagnostische Stellenwert von 8- im Vergleich zu den Aldosteron-Metaboliten Aldosteron-18-Glucuronid (ALD-18-G) und Tetrahydroaldosteron (TH-ALD) untersucht. Dies im Hin blick auf: 1. die Erkennung eines primären Aldosteronismus, und 2. der differentialdiagnostischen Unterscheidung zwischen einem Adenom und einer Hyperpläsie.
Bezüglich der ersten Fragestellung wurde für 18-OHB - hinsichtlich der Unterscheidung zwischen dem primären Aldosteronismus infolge eines Adenoms und einer essentiellen Hypertonie-eine diagnostische Sensitivität von 99,2% bei einer diagnostischen Spezifität von 95,2% berechnet. Deutlich geringer war mit einer diagnostischen Sensitivität von 79,7% bei einer diagnostischen Spezifität von 60,9% die Abgrenzung zwischen dem primären Aldosteronismus infolge einer Hyperpläsie und einer essentiellen Hypertonie.
18-OHB war bei 11 der 84 Adenom- und 5 der 110 Hyperplasie-Patienten zunächst das einzig erhöhte Steroid im 24 h-Urin. Bei ihnen konnte erst innerhalb einer bis zu 2jährigen Beobachtungszeit ein langsamer Anstieg der Aldosteron-Metabolite beobachtet werden. Somit stellt das 18-OHB einen „Frühmarker" der Erkrankung dar.
In der Unterscheidung zwischen einem Nebennierenrinden-Adenom und einer -Hyperplasie besitzt 18-OHB mit einer diagnostischen Sensitivität von 84,5% bei einer diagnostischen Spezifität von 96,4% ein höheres Abgrenzungsvermögen als Tetrahydro-Aldosteron und Aldosteron-18-Glucuronid dar.
Für die Unterscheidung des Adenoms von der Hyperpläsie ließ sich für 18-OH-Corticosteron im 24 h-Urin ein Wert von 7,9 [ig/die als eine optimale Diskriminanzschwelle berechnen. Bei einer höheren Ausscheidung ist in 84,5% der Fälle mit einem Nebennierenrinden-Adenom zu rechnen. Hinsichtlich der diagnostischen Wertung von 18-OHB sind weder geschlechts- noch altersspezifische Abhängigkeiten zu berücksichtigen.
Die Bestimmung von Tetrahydro-Aldosteron (oder Aldosteron-18-Glucuronid) in Kombination mit 18-OH-Corticosteron stellt die optimale Methode zur Diagnostik des primären Hyperaldosteronismus, insbesondere infolge eines Adenoms, dar.
Tibnīn was an important small Crusader fief and a fortified castle. It was vital for the Kingdom of Jerusalem, because it included fertile agricultural lands, was a tax collection centre, and because it controlled the Damascus-to-Tyre commercial route. Additionally, its castle played defensive and offensive role in the north of the Kingdom of Jerusalem and upper Galilee, and its rulers of Tibnīn played a major role in forming the history of the Latin East. When the Crusaders invaded the Levant at the end of the eleventh century, it was given rise to new demographic, cultural, socio-economic, and architectural features. The present Paper aims at removing some of the mystery concerning the fief of Tibnīn and its castle in the Latin East. This paper thus is a study of the demographic structure of Tibnīn and discusses the socio-economic role of Tibnīn in the Latin east. Moreover, the role of Tibnīn in influencing the relations between Muslims and the Crusaders in the Levant and the architecture of the castle of Tibnīn and its importance in the age of the Crusade will be examined.
The Crusade movement is one of the most important occurrences of medieval history. It took place throughout two centuries in the Levant and affected both Muslims and Crusaders and in turn changed the way in which West and East related to one another.1 When the Crusaders took control of the Holy Land and many Islamic cities in the Levant, they transferred their feudal European system there. They established four main fiefdoms or lordships, Jerusalem, Edessa, Antioch and Tripoli. In addition, there were another twelve secondary fiefdoms,2 of which Tibnīn was one. Tibnīn was called “Toron” by the Crusaders. Once the Crusaders had captured Tibnīn, they began building its fortified castle, from which the fief of Tibnīn gained its importance throughout the period of the Crusades.
This paper traces the military role of Tibnīn and its rulers in the Latin East against the Muslims until 1187/ 583. Tibnīn played a key role in overcoming the Muslims in Tyre and controlled it in 1124. It also played a vital role in the conflict between Damascus and the Kingdom of Jerusalem. Tibnīn participated in defending Antioch, Banyas, Hebron and Transjordan several times. Furthermore, its soldiers and Knights joined the army of the Kingdom of Jerusalem to capture Ascalon in 1153, and joined the campaigns of Amaury I, King of Jerusalem, against Egypt from 1164 to1169. The military situation of Tibnīn under the rule of the royal house until its fall to the Muslims in 1187/ 583 will be studied as well.
Die Verwendung von photolabilen Schutzgruppen zur nicht-invasiven Kontrolle von Systemen birgt ein großes Potential für verschiedenste Anwendungsgebiete, die von der Erforschung und Regulation biologischer Prozesse, über den Einsatz in medizinischer Therapie bis hin zur Verwendung als molekulare Datenspeicher reichen. Für diese Umsetzung benötigt es allerdings eine breite Auswahl an entsprechenden PPGs und das Wissen über ihre Reaktionsmechanismen. Im Allgemeinen lässt sich die Konzeptionierung von PPGs in drei Prozesse einteilen, beginnend bei dem Design und der Synthese einer neuen PPG. Bei diesem Schritt liegt der Fokus auf ein oder zwei besonderen Eigenschaften, wie beispielsweise einer Absorptionswellenlänge in einem bestimmten Spektralbereich oder einer hohen Uncaging-Quantenausbeute. Im zweiten Schritt folgt die Untersuchung der PPG bezüglich spektroskopischer und mechanistischer Eigenschaften und ggf. anschließender Optimierung auf synthetischer Ebene. Die so gewonnenen Informationen sind dann hilfreich bei dem letzten Schritt, bei dem es um den Einsatz der PPG in einem entsprechenden System geht. Hierbei müssen die verwendeten PPGs genau auf das Zielsystem abgestimmt sein, dazu zählen verschiedenste Parameter wie Anregungswellenlänge, Extinktionskoeffizient, Art und Struktur der Photoprodukte sowie Uncaging-Effizienz und Geschwindigkeit.
In der vorliegenden Arbeit wurde über die drei vorgestellten Projekte mittels spektroskopischer Methoden zu allen drei genannten Stadien zur Konzeptionierung von PPGs ein Beitrag geleistet. Dazu zählt die Entwicklung der CBT-basierten PPGs, die Untersuchung der Struktur-Wirkungsbeziehung von (DMA)(2)F-PPGs und die Etablierung einer wellenlängenselektiven An-/Aus-Funktionalität eines Antibiotikums. In enger interdisziplinärer Zusammenarbeit zwischen theoretischen, synthetischen und biologischen Teilgebieten konnte jedes Projekt innerhalb der jeweiligen Entwicklungsstufe erfolgreich abgeschlossen werden.
Mithilfe des relativ neuen Ansatzes, bei dem durch quantenmechanische Berechnungen der vertikalen Anregungsenergie von der kationischen Spezies einer PPG-Grundstruktur eine Aussage über ihre Qualität postuliert werden kann, konnte ausgehend von der Fluoren-Grundstruktur eine neue Klasse von PPGs gefunden werden. Dabei erwies sich die CBT-Struktur mit den Schwefelatomen an der para-Position als besonders geeignet. Insbesondere konnte die Grundstruktur durch die (OMePh)2-Substitution, welche in einer signifikanten bathochromen Verschiebung des Absorptionsmaximums resultierte, optimiert werden. Die Untersuchung der Ultrakurzzeit-Dynamik beider p-CBT Strukturen gab Aufschluss über die unterschiedlichen photochemischen Eigenschaften als PPG.
Für die Stoffklasse der Dimethylamino-Fluorene wurde ein wichtiger Unterschied zwischen den einfach- und zweifach-substituierten Derivaten aufgedeckt, der entscheidend für einen signifikanten Uncaging-Effizienzunterschied ist. Dabei stellt sich die Stabilität des symmetrisch-substituierten Fluorenyl-Kations als der wichtigste Faktor bezüglich der Uncaging-Quantenausbeuten heraus. Beide Schutzgruppen sind in der Lage photoinduziert eine AG freizusetzen, wobei der Reaktionsmechanismus über die kationische Spezies (DMA)(2)F + abläuft. Der Unterschied hierbei liegt in der Lebensdauer der beiden Kationen, die im Falle der symmetrischen PPG stark lösungsmittelabhängig ist und bis zu mehreren Stunden betragen kann, was bis dato das langlebigste Kation dieser Molekülklasse darstellt. Für die zukünftige Optimierung dieser PPG-Klasse ist die Erkenntnis über die Gründe für die Stabilität des Kations von großem Vorteil. Der stabilisierende Faktor ist zum einen die zweite Dimethylamino-Gruppe der symmetrischen Verbindung, welche durch die Erweiterung der Mesomerie zur besseren Verteilung der positiven Ladung im Molekül führt. Zum anderen spielt das Lösungsmittel eine entscheidende Rolle. Dabei bieten protische, polare Medien eine zusätzliche Stabilisierung, die notwendig für die Langlebigkeit des Kations ist. Die Lebensdauer des Kations war zudem durch eine zweite Bestrahlungswellenlänge kontrollierbar. Ausgehend vom Kation konnte eine reversible Nebenreaktion in protischen Lösungsmitteln identifiziert werden, die einen Austausch der AG durch das Lösungsmittel darstellt.
Zusätzlich konnte die kleine Stoffklasse der bisher bekannten Photobasen durch die Verbindung (DMA)2F-OH erweitert werden. Genauer betrachtet handelt es sich dabei um eine photoinduzierte Hydroxidfreisetzung, wodurch je nach eingesetzter Konzentration ein pH-Sprung von bis zu drei Einheiten erreicht werden konnte. Dabei stellt sich die Lebensdauer des pH-Sprungs als ein entscheidender Parameter für Photobasen dar, welcher sich für die hier untersuchte Verbindung aufgrund der besonderen Stabilität des entsprechenden Kations, im Vergleich zu einigen der bereits bekannten Verbindungen, als besonders langlebig herausgestellt hat. Ein weiterer Vorteil des Einsatzes von (DMA)2F-OH als Photobase ist die Möglichkeit den pH-Sprung durch zwei verschiedene Wellenlängen sowohl zeitlich als auch örtlich zu kontrollieren, indem die Verbindung zwischen den zwei Spezies (DMA)2F-OH und (DMA)2F + geschaltet werden kann.
Im Hinblick auf die Anwendungen von PPGs zur verbesserten zeitlichen und örtlichen Kontrolle biologischer Zielsysteme ist im Rahmen dieser Arbeit das Prinzip vom wellenlängenselektiven Uncaging zweier PPGs an einem Molekül (two-PPG-one-molecule, TPOM) etabliert worden. Das Zielmolekül war hier das Antibiotikum Puromycin, welches durch seine Fähigkeit an das Ribosom zu binden, die Proteinbiosynthese inhibieren kann. Dabei wurden zwei verschiedene PPGs gefunden, die sowohl aufeinander als auch auf das Biomolekül selbst abgestimmt sind. Im Ausgangszustand sind beide PPGs am Puromycin angebracht, wodurch es in seiner biologischen Wirkung inaktiv ist. Befindet sich das doppelt geschützte Puromycin in der ROI, so kann es durch die Bestrahlung mit einer bestimmten Wellenlänge infolge des ersten Uncaging-Schritts aktiviert werden. Da biologische Systeme nicht statisch sind, können aktivierte Moleküle stets von der gewünschten ROI nach außen gelangen, wodurch der Anspruch der räumlichen Kontrolle nicht erfüllt wird. In diesem Fall kann durch die TPOM-Umsetzung die zweite Bestrahlungswellenlänge auf den entsprechenden Bereich angewendet werden, wodurch das Uncaging der zweiten PPG initiiert und folglich das Puromycin deaktiviert wird. Des Weiteren konnte gezeigt werden, dass die Deaktivierungswellenlänge auch in der Lage ist beide PPGs zu entfernen, wodurch eine vollständige Inaktivierung des Puromycins außerhalb der ROI garantiert werden kann.
Ist die Proteinbiosynthese längerfristig blockiert, führt das schließlich zum Zelltod. Ein großes Anwendungsgebiet dieses Antibiotikums sind die Neurowissenschaften. Aufgrund der Tatsache, dass Puromycin keine Unterscheidung zwischen eukaryotischen und prokaryotischen Zellen macht, findet es keine Anwendung in der Medizin. Eine zeitliche und örtliche Kontrolle seiner Wirkung könnte den Anwendungsbereich dieses Antibiotikums evtl. ausweiten. Das wohl naheliegendste wäre der Einsatz bei Tumorzellen, deren Behandlung durch Zytostatika auf den gesamten Körper wirken und dadurch viele schwere Nebenwirkungen verursachen.
Wie bereits weiter oben beschrieben muss für jedes Biomolekül und das entsprechende Wirkzentrum die Auswahl des passenden PPG-Paares einzeln abgestimmt werden. Dennoch lässt sich anhand des hier etablierten Systems ein Konzept für die erfolgreiche Umsetzung zukünftiger TPOM-Systeme an anderen biomolekularen Wirkstoffen zusammenfassend formulieren.
* Der erste Schritt sollte die Betrachtung des Wirkzentrums des zu modifizierenden Biomoleküls sein: Welche funktionelle Gruppe bzw. Gruppen sind entscheidend für die Bindetasche oder –stelle? Dieser Bereich des Biomoleküls soll im Zuge des Uncagings entweder blockiert oder abgespalten werden. In der unmittelbaren Nähe muss die PPG1 angebracht werden.
* Bei der Wahl von PPG1 ist das wichtigste Kriterium, dass das Biomolekül mit enthaltener Schutzgruppe in seiner Wirkung unbeeinträchtigt bleibt. Dies schränkt die Auswahl beträchtlich ein. Eine mögliche Umsetzung wäre die Anbringung einer Nitro-Gruppe falls vorhanden an einen Benzolring, welcher sich im Fall eines großen Biomoleküls in der Nähe der wichtigen funktionellen Stelle befindet.
* Die zweite PPG (PPG2), deren photoinduzierte Abspaltung zur Aktivierung des Wirkstoffs führen soll, kann strukturell frei gewählt werden. Das Auswahlkriterium hierbei ist das Absorptionsspektrum. Hierbei sollte das Absorptionsmaximum rotverschoben zur PPG1 sein, um eine unerwünschte Abspaltung zu vermeiden. Außerdem darf keine signifikante Absorption von PPG2 bei der Uncaging-Wellenlänge von PPG1 vorhanden sein.
* Beide PPGs sollten eine ähnliche Uncaging-Quantenausbeute vorweisen, um im Deaktivierungsschritt der doppelt geschützten Verbindung durch das höher energetische Licht keine Bevorzugung einer einzelnen Schutzgruppe zu riskieren.
Anhand der erarbeiteten Herangehensweise können weitere Wirkstoffe oder Biomoleküle hin zu einer An- / Aus-Funktionalität modifiziert werden. Mit der Umsetzung des TPOM-Konzepts kann eine Verbesserung der örtlichen und zeitlichen Kontrolle der Aktivität eines Antibiotikums erreicht werden. Für die Anwendung in biologischer Umgebung ist diese präzische Kontrolle essentiell, um unerwünschte Nebenwirkungen angesundem Gewebe zu verhindern.
This article discusses the counterpart of interactive machine learning, i.e., human learning while being in the loop in a human-machine collaboration. For such cases we propose the use of a Contradiction Matrix to assess the overlap and the contradictions of human and machine predictions. We show in a small-scaled user study with experts in the area of pneumology (1) that machine-learning based systems can classify X-rays with respect to diseases with a meaningful accuracy, (2) humans partly use contradictions to reconsider their initial diagnosis, and (3) that this leads to a higher overlap between human and machine diagnoses at the end of the collaboration situation. We argue that disclosure of information on diagnosis uncertainty can be beneficial to make the human expert reconsider her or his initial assessment which may ultimately result in a deliberate agreement. In the light of the observations from our project, it becomes apparent that collaborative learning in such a human-in-the-loop scenario could lead to mutual benefits for both human learning and interactive machine learning. Bearing the differences in reasoning and learning processes of humans and intelligent systems in mind, we argue that interdisciplinary research teams have the best chances at tackling this undertaking and generating valuable insights.
We focus on the role of social media as a high-frequency, unfiltered mass information transmission channel and how its use for government communication affects the aggregate stock markets. To measure this effect, we concentrate on one of the most prominent Twitter users, the 45th President of the United States, Donald J. Trump. We analyze around 1,400 of his tweets related to the US economy and classify them by topic and textual sentiment using machine learning algorithms. We investigate whether the tweets contain relevant information for financial markets, i.e. whether they affect market returns, volatility, and trading volumes. Using high-frequency data, we find that Trump’s tweets are most often a reaction to pre-existing market trends and therefore do not provide material new information that would influence prices or trading. We show that past market information can help predict Trump’s decision to tweet about the economy.
Mitochondial NADH:ubiquinone oxidoreductase (complex I) the largest multiprotein enzyme of the respiratory chain, catalyses the transfer of two electrons from NADH to ubiquinone, coupled to the translocation of four protons across the membrane. In addition to the 14 strictly conserved central subunits it contains a variable number of accessory subunits. At present, the best characterized enzyme is complex I from bovine heart with a molecular mass of about 980 kDa and 32 accessory proteins. In this study, the subunit composition of mitochondrial complex I from the aerobic yeast Y. lipolytica has been analysed by a combination of proteomic and genomic approaches. The sequences of 37 complex I subunits were identified. The sum of their individual molecular masses (about 930 kDa) was consistent with the native molecular weight of approximately 900 kDa for Y. lipolytica complex I obtained by BN-PAGE. A genomic analysis with Y. lipolytica and other eukaryotic databases to search for homologues of complex I subunits revealed 31 conserved proteins among the examined species. A novel protein named “X” was found in purified Y. lipolytica complex I by MALDI-MS. This protein exhibits homology to the thiosulfate sulfurtransferase enzyme referred to as rhodanese. The finding of a rhodanese-like protein in isolated complex I of Y. lipolytica allows to assume a special regulatory mechanism of complex I activity through control of the status of its iron-sulfur clusters. The second part of this study was aimed at investigating the possible role of one of these extra subunits, 39 kDa (NUEM) subunit which is related to the SDRs-enzyme family. The members of this family function in different redox and isomerization reactions and contain a conserved NAD(P)H-binding site. It was proposed that the 39 kDa subunit may be involved in a biosynthetic pathway, but the role of this subunit in complex I is unknown. In contrast to the situation in N. crassa, deletion of the 39 kDa encoding gene in Y. lipolytica led to the absence of fully assembled complex I. This result might indicate a different pathway of complex I assembly in both organisms. Several site-directed mutations were generated in the nucleotide binding motif. These had either no effect on enzyme activity and NADPH binding, or prevented complex I assembly. Mutations of arginine-65 that is located at the end of the second b-strand and responsible for selective interaction with the 2’-phosphate group of NADPH retained complex I activity in mitochondrial membranes but the affinity for the cofactor was markedly decreased. Purification of complex I from mutants resulted in decrease or loss of ubiquinone reductase activity. It is very likely that replacement of R65 not only led to a decrease in affinity for NADPH but also caused instability of the enzyme due to steric changes in the 39 kDa subunit. These data indicate that NADPH bound to the 39 kDa subunit (NUEM) is not essential for complex I activity, but probably involved in complex I assembly in Y. lipolytica.
Índice Gramática Lição Adjectivos 4.1 Demonstrativos 12.1 Interrogativos 13.1 Números cardinais 4.2 Possessivo nominal 11.1 Possessivo pronominal 9.2 Pronomes pessoais 1.2 Substantivo: classes 1-10 2.1 Substantivos: classes 1-18 6.1 Verbo: infinitivo 1.1 Verbo: infinitivo negativo 3.1 Verbo: optativo 8.2 Verbo: passado recente e remoto 14.1 Verbo: prefixo do objecto 8.1 Verbo: prefixo do sujeito 1.3 Verbo: prefixo do sujeito (classes 3-14) 7.1 Verbo: presente contínuo 2.2 Verbo: presente contínuo negativo 3.3 Verbo: presente do indicativo 1.4 Verbo: presente negativo 3.2
Übermäßige Gewaltanwendungen durch Polizist:innen in Deutschland sind bislang nur in Ansätzen untersucht. Das Buch liefert umfassende wissenschaftliche Befunde zu einschlägigen Situationen und ihrer strafrechtlichen Aufarbeitung. Auf Basis einer Betroffenenbefragung mit über 3.300 Teilnehmenden und über 60 qualitativen Interviews stellen sich die Fälle als komplexe Interaktionsgeschehen dar, bei deren Aufarbeitung eine besondere Definitionsmacht der Polizei sichtbar wird.
Das Forschungsprojekt KviAPol (Körperverletzung im Amt durch Polizeibeamte und -beamtinnen) untersucht polizeiliche Gewaltanwendungen, die aus Sicht der Betroffenen rechtswidrig waren, mittels quantitativer Online-Befragung sowie die polizeiliche, justizielle und zivilgesellschaftliche Perspektive auf rechtswidrige Polizeigewalt und deren Aufarbeitung in Deutschland mittels qualitativer Interviews. Zum Team gehören die Wissenschaftlichen Mitarbeiterinnen Laila Abdul-Rahman, Hannah Espín Grau und Luise Klaus sowie Prof. Dr. Tobias Singelnstein, der die Projektleitung innehat.
In relativistic heavy-ion collisions, a global spin polarization, PH, of Λ and Λ¯ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing PH with decreasing sNN−−−√. A splitting between Λ and Λ¯ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of sNN−−−√=19.6 and 27 GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of PΛ¯−PΛ<0.24% and PΛ¯−PΛ<0.35%, respectively, at a 95% confidence level. We derive an upper limit on the naïve extraction of the late-stage magnetic field of B<9.4⋅1012 T and B<1.4⋅1013 T at sNN−−−√=19.6 and 27 GeV, respectively, although more thorough derivations are needed. Differential measurements of PH were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of |y|<1 and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.
In relativistic heavy-ion collisions, a global spin polarization, PH, of Λ and Λ¯ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing PH with decreasing sNN−−−√. A splitting between Λ and Λ¯ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of sNN−−−√=19.6 and 27 GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of PΛ¯−PΛ<0.24% and PΛ¯−PΛ<0.35%, respectively, at a 95% confidence level. We derive an upper limit on the naïve extraction of the late-stage magnetic field of B<9.4⋅1012 T and B<1.4⋅1013 T at sNN−−−√=19.6 and 27 GeV, respectively, although more thorough derivations are needed. Differential measurements of PH were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of |y|<1 and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.
In relativistic heavy-ion collisions, a global spin polarization, PH, of Λ and Λ¯ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing PH with decreasing sNN−−−√. A splitting between Λ and Λ¯ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of sNN−−−√=19.6 and 27 GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of PΛ¯−PΛ<0.24% and PΛ¯−PΛ<0.35%, respectively, at a 95% confidence level. We derive an upper limit on the naïve extraction of the late-stage magnetic field of B<9.4⋅1012 T and B<1.4⋅1013 T at sNN−−−√=19.6 and 27 GeV, respectively, although more thorough derivations are needed. Differential measurements of PH were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of |y|<1 and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.
Elliptic flow of heavy-flavor decay electrons in Au+Au collisions at √sNN = 27 and 54.4 GeV at RHIC
(2023)
We report on new measurements of elliptic flow (v2) of electrons from heavy-flavor hadron decays at mid-rapidity (|y|<0.8) in Au+Au collisions at sNN−−−√ = 27 and 54.4 GeV from the STAR experiment. Heavy-flavor decay electrons (eHF) in Au+Au collisions at sNN−−−√ = 54.4 GeV exhibit a non-zero v2 in the transverse momentum (pT) region of pT< 2 GeV/c with the magnitude comparable to that at sNN−−−√=200 GeV. The measured eHF v2 at 54.4 GeV is also consistent with the expectation of their parent charm hadron v2 following number-of-constituent-quark scaling as other light and strange flavor hadrons at this energy. These suggest that charm quarks gain significant collectivity through the evolution of the QCD medium and may reach local thermal equilibrium in Au+Au collisions at sNN−−−√=54.4 GeV. The measured eHF v2 in Au+Au collisions at sNN−−−√= 27 GeV is consistent with zero within large uncertainties. The energy dependence of v2 for different flavor particles (π,ϕ,D0/eHF) shows an indication of quark mass hierarchy in reaching thermalization in high-energy nuclear collisions.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at √sNN = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40%) collisions. Moreover, the ν in the 0-5% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a minimum around √sNN = 27 GeV. The physics implications on the QCD phase structure are discussed.
Elliptic flow of heavy-flavor decay electrons in Au+Au collisions at √sNN = 27 and 54.4 GeV at RHIC
(2023)
We report on new measurements of elliptic flow (v2) of electrons from heavy-flavor hadron decays at mid-rapidity (|y|<0.8) in Au+Au collisions at sNN−−−√ = 27 and 54.4 GeV from the STAR experiment. Heavy-flavor decay electrons (eHF) in Au+Au collisions at sNN−−−√ = 54.4 GeV exhibit a non-zero v2 in the transverse momentum (pT) region of pT< 2 GeV/c with the magnitude comparable to that at sNN−−−√=200 GeV. The measured eHF v2 at 54.4 GeV is also consistent with the expectation of their parent charm hadron v2 following number-of-constituent-quark scaling as other light and strange flavor hadrons at this energy. These suggest that charm quarks gain significant collectivity through the evolution of the QCD medium and may reach local thermal equilibrium in Au+Au collisions at sNN−−−√=54.4 GeV. The measured eHF v2 in Au+Au collisions at sNN−−−√= 27 GeV is consistent with zero within large uncertainties. The energy dependence of v2 for different flavor particles (π,ϕ,D0/eHF) shows an indication of quark mass hierarchy in reaching thermalization in high-energy nuclear collisions.
We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity (|y|< 0.7) in Au+Au collisions at sNN−−−√=200 GeV. Invariant yields of HFEs are measured for the transverse momentum range of 3.5<pT<9 GeV/c in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in p+p collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.
We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity (|y|< 0.7) in Au+Au collisions at sNN−−−√=200 GeV. Invariant yields of HFEs are measured for the transverse momentum range of 3.5<pT<9 GeV/c in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in p+p collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.
We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity (|y| < 0.7) in Au+Au collisions at √sNN = 200 GeV. Invariant yields of HFEs are measured for the transverse momentum range of 3.5 < pT < 9 GeV/c in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in p + p collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at sNN−−−√ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the ν in the 0-5\% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a possible minimum around sNN−−−√ = 27 GeV. The physics implications on the QCD phase structure are discussed.
The longitudinal and transverse spin transfers to Λ (Λ¯¯¯¯) hyperons in polarized proton-proton collisions are expected to be sensitive to the helicity and transversity distributions, respectively, of (anti-)strange quarks in the proton, and to the corresponding polarized fragmentation functions. We report improved measurements of the longitudinal spin transfer coefficient, DLL, and the transverse spin transfer coefficient, DTT, to Λ and Λ¯¯¯¯ in polarized proton-proton collisions at s√ = 200 GeV by the STAR experiment at RHIC. The data set includes longitudinally polarized proton-proton collisions with an integrated luminosity of 52 pb−1, and transversely polarized proton-proton collisions with a similar integrated luminosity. Both data sets have about twice the statistics of previous results and cover a kinematic range of |ηΛ(Λ¯¯¯¯)| < 1.2 and transverse momentum pT,Λ(Λ¯¯¯¯) up to 8 GeV/c. We also report the first measurements of the hyperon spin transfer coefficients DLL and DTT as a function of the fractional jet momentum z carried by the hyperon, which can provide more direct constraints on the
The longitudinal and transverse spin transfers to Λ (Λ¯¯¯¯) hyperons in polarized proton-proton collisions are expected to be sensitive to the helicity and transversity distributions, respectively, of (anti-)strange quarks in the proton, and to the corresponding polarized fragmentation functions. We report improved measurements of the longitudinal spin transfer coefficient, DLL, and the transverse spin transfer coefficient, DTT, to Λ and Λ¯¯¯¯ in polarized proton-proton collisions at s√ = 200 GeV by the STAR experiment at RHIC. The data set includes longitudinally polarized proton-proton collisions with an integrated luminosity of 52 pb−1, and transversely polarized proton-proton collisions with a similar integrated luminosity. Both data sets have about twice the statistics of previous results and cover a kinematic range of |ηΛ(Λ¯¯¯¯)| < 1.2 and transverse momentum pT,Λ(Λ¯¯¯¯) up to 8 GeV/c. We also report the first measurements of the hyperon spin transfer coefficients DLL and DTT as a function of the fractional jet momentum z carried by the hyperon, which can provide more direct constraints on the polarized fragmentation functions.
The differential cross section for 𝑍0 production, measured as a function of the boson’s transverse momentum (𝑝T), provides important constraints on the evolution of the transverse momentum dependent parton distribution functions (TMDs). The transverse single spin asymmetry (TSSA) of the 𝑍0 is sensitive to one of the polarized TMDs, the Sivers function, which is predicted to have the opposite sign in 𝑝 + 𝑝 → 𝑊 ∕𝑍 + 𝑋 from that which enters in semi-inclusive deep inelastic scattering. In this Letter, the STAR Collaboration reports the first measurement of the 𝑍0∕𝛾∗ differential cross section as a function of its 𝑝T in 𝑝+𝑝 collisions at a center-of-mass energy of 510 GeV, together with the 𝑍0∕𝛾∗ total cross section. We also report the measurement of 𝑍0∕𝛾∗ TSSA in transversely polarized 𝑝+𝑝 collisions at 510 GeV.
We report results on an elastic cross section measurement in proton–proton collisions at a center-of-mass energy √𝑠 = 510 GeV, obtained with the Roman Pot setup of the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The elastic differential cross section is measured in the four-momentum transfer squared range 0.23 ≤ −𝑡 ≤ 0.67 GeV2. This is the only measurement of the proton-proton elastic cross section in this 𝑡 range for collision energies above the Intersecting Storage Rings (ISR) and below the Large Hadron Collider (LHC) colliders. We find that a constant slope 𝐵 does not fit the data in the aforementioned 𝑡 range, and we obtain a much better fit using a second-order polynomial for 𝐵(𝑡). This is the first measurement below the LHC energies for which the non-constant behavior 𝐵(𝑡) is observed. The 𝑡 dependence of 𝐵 is also determined using six subintervals of 𝑡 in the STAR measured 𝑡 range, and is in good agreement with the phenomenological models. The measured elastic differential cross section d𝜎∕dt agrees well with the results obtained at √𝑠 = 540 GeV for proton–antiproton collisions by the UA4 experiment. We also determine that the integrated elastic cross section within the STAR 𝑡-range is 𝜎f id el = 462.1 ± 0.9(stat.) ± 1.1(syst.) ± 11.6(scale) 𝜇b.
We report the first measurements of cumulants, up to 4𝑡ℎ order, of deuteron number distributions and protondeuteron correlations in Au+Au collisions recorded by the STAR experiment in phase-I of Beam Energy Scan (BES) program at the Relativistic Heavy Ion Collider. Deuteron cumulants, their ratios, and proton-deuteron mixed cumulants are presented for different collision centralities covering a range of center-of-mass energy per nucleon pair √𝑠NN = 7.7 to 200 GeV. It is found that the cumulant ratios at lower collision energies favor a canonical ensemble over a grand canonical ensemble in thermal models. An anti-correlation between proton and deuteron multiplicity is observed across all collision energies and centralities, consistent with the expectation from global baryon number conservation. The UrQMD model coupled with a phase-space coalescence mechanism qualitatively reproduces the collision-energy dependence of cumulant ratios and proton-deuteron correlations.
We report results on an elastic cross section measurement in proton-proton collisions at a center-of-mass energy s√=510 GeV, obtained with the Roman Pot setup of the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The elastic differential cross section is measured in the four-momentum transfer squared range 0.23≤−t≤0.67 GeV2. We find that a constant slope B does not fit the data in the aforementioned t range, and we obtain a much better fit using a second-order polynomial for B(t). The t dependence of B is determined using six subintervals of t in the STAR measured t range, and is in good agreement with the phenomenological models. The measured elastic differential cross section dσ/dt agrees well with the results obtained at s√=546 GeV for proton--antiproton collisions by the UA4 experiment. We also determine that the integrated elastic cross section within the STAR t-range is σfidel=462.1±0.9(stat.)±1.1(syst.)±11.6(scale) μb.
We report the first measurements of cumulants, up to 4th order, of deuteron number distributions and proton-deuteron correlations in Au+Au collisions recorded by the STAR experiment in phase-I of Beam Energy Scan (BES) program at the Relativistic Heavy Ion Collider. Deuteron cumulants, their ratios, and proton-deuteron mixed cumulants are presented for different collision centralities covering a range of center-of-mass energy per nucleon pair sNN−−−−√~=~7.7 to 200~GeV. It is found that the cumulant ratios at lower collision energies favor a canonical ensemble over a grand canonical ensemble in thermal models. An anti-correlation between proton and deuteron multiplicity is observed across all collision energies and centralities, consistent with the expectation from global baryon number conservation. The UrQMD model coupled with a phase-space coalescence mechanism qualitatively reproduces the collision-energy dependence of cumulant ratios and proton-deuteron correlations.
We measure triangular flow relative to the reaction plane at 3 GeV center-of-mass energy in Au+Au collisions at the BNL Relativistic Heavy Ion Collider. A significant v3 signal for protons is observed, which increases for higher rapidity, higher transverse momentum, and more peripheral collisions. The triangular flow is essentially rapidity-odd with a slope at mid-rapidity, dv3/dy|(y=0), opposite in sign compared to the slope for directed flow. No significant v3 signal is observed for charged pions and kaons. Comparisons with models suggest that a mean field potential is required to describe these results, and that the triangular shape of the participant nucleons is the result of stopping and nuclear geometry.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2024)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane. This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions. A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of (R=0.4) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb+Pb collision data.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2024)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane. This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions. A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of (R=0.4) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb+Pb collision data.
The polarization of Λ and Λ¯ hyperons along the beam direction has been measured relative to the second and third harmonic event planes in isobar Ru+Ru and Zr+Zr collisions at √sNN = 200 GeV. This is the first experimental evidence of the hyperon polarization by the triangular flow originating from the initial density fluctuations. The amplitudes of the sine modulation for the second and third harmonic results are comparable in magnitude, increase from central to peripheral collisions, and show a mild pT dependence. The azimuthal angle dependence of the polarization follows the vorticity pattern expected due to elliptic and triangular anisotropic flow, and qualitatively disagree with most hydrodynamic model calculations based on thermal vorticity and shear induced contributions. The model results based on one of existing implementations of the shear contribution lead to a correct azimuthal angle dependence, but predict centrality and pT dependence that still disagree with experimental measurements. Thus, our results provide stringent constraints on the thermal vorticity and shear-induced contributions to hyperon polarization. Comparison to previous measurements at RHIC and the LHC for the second-order harmonic results shows little dependence on the collision system size and collision energy.
The elliptic (v2) and triangular (v3) azimuthal anisotropy coefficients in central 3He+Au, d+Au, and p+Au collisions at sNN−−−√ = 200 GeV are measured as a function of transverse momentum (pT) at mid-rapidity (|η|<0.9), via the azimuthal angular correlation between two particles both at |η|<0.9. While the v2(pT) values depend on the colliding systems, the v3(pT) values are system-independent within the uncertainties, suggesting an influence on eccentricity from sub-nucleonic fluctuations in these small-sized systems. These results also provide stringent constraints for the hydrodynamic modeling of these systems.
The relevance of the work and the influence of Franz Rosenzweig, a German Jewish philosopher of the beginning of the last century; are still to get the appreciation they deserve. Rosenzweig was the author of one of the greatest – and less read – books of the 20th century, "The Star of Redemption", where he develops his philosophical system mainly on basis of theological categories. To the "monologue of the I" of mainstream philosophy, Rosenzweig opposes a "new thinking", of existential character, which values orality and the "other", and where language substitutes reason as a tool for thought. In it one can find some correspondences with the thought of Walter Benjamin. This "new thinking", also, strongly influenced Emmanuel Levinas and nowadays bears its fruits within "linguistic turn" philosophy and theology, and post-modern Jewish thought. This philosophy found in Rosenzweig's work in translation one of its main practical applications. To translate was for Rosenzweig a necessity, emanating from an ethics constituted as "first philosophy". This article examines some aspects of Rosenzweig's writings from where his "philosophy of translation" is made explicit.
Death and the King's Grey Hair and Other Plays is a collection of three plays, 'Death and the King's Grey Hair, ' 'Truce with the Devil, ' and 'Fringe Benefits, ' which are all experimental plays from the early period of the writing career of Denja Abdullahi, who is presently renowned as a poet of populist expressions. 'Death and the King's Grey Hair' examines the use and misuse of absolute power based on an ancient Jukun myth of young kings and short reigns. 'Truce with the Devil' is a satire on the later abandonment of the creed of Marxism by its adherents, a kind of mockery of turncoat revolutionaries in the grip of practical social realities. 'Fringe Benefits', a radio play, is an expose of the happening in Nigeria's ivory towers, seen from the eyes of a participant-observer.
Background and Aims: Fecal biomarkers are important non-invasive markers monitoring disease activity in inflammatory bowel disease (IBD). We compared the significance of fecal eosinophil cationic protein (fECP) and fecal calprotectin (fCal).
Methods: fECP and fCal were measured in patients with Crohn's disease (CD, n = 97), ulcerative colitis (UC, n = 53), Clostridioides difficile infection (CDI, n = 9), primary food allergy (PFA, n = 11), pollen-associated food allergy (n = 25) and non-inflammatory controls (n = 78). Results were correlated with clinical and endoscopic IBD activity scores.
Results: fECP was significantly elevated in CD, UC, CDI and PFA compared to controls. fCal was significantly increased in CD, UC and CDI. fECP had lower diagnostic accuracy than fCal (area under the curve (AUC) = 0.88) in differentiating between endoscopically active and inactive patients with IBD (AUC = 0.77, ROC analysis). In contrast to fCal, fECP correlated negatively with age and levels were also elevated in clinically and endoscopically inactive patients with IBD <45 years (endoscopically inactive IBD vs controls; AUC for fECP = 0.86; AUC for fCal = 0.62). However, in those patients with low inflammatory activity (fCal <250 mg/kg), high fECP indicated the need for treatment modification or surgery (fECP <200 µg/kg = 22%; 200–600 µg/kg = 44%; >600 µg/kg = 82%) at month 48 of follow-up.
Conclusions: fECP is a diagnostic and prognostic marker in young patients with IBD in remission.
Leaving aside elliptical coordinations, it is striking that no agreement has been reached on the structure of basic coordinate constructions. We propose that:
- coordinate constructions are structurally asymmetric: the conjunction makes a subconstituent with one of the conjuncts.
- such constituents can have several functions: coordinate daughter, adjunct daughter or main clause.
In order to show that some conjuncts should be analysed as adjuncts, we focus on asymmetric cases of coordination, in which the order of the conjuncts cannot be reversed, taking examples from French, Welsh and Korean. We present an HPSG analysis which treats the coordinating conjunctions as weak heads, with lexical subtypes, and coordinate phrases as multi-headed constructions, with different subtypes.
Of all French functional elements, the form de has without question the widest variety of uses, and presents the greatest challenge for linguistic description and analysis. Historically a preposition, it still has a number of prepositional uses in modern French, but in many contexts it calls for an altogether different treatment. We begin by outlining a general distinction between oblique and non-oblique uses of de. We then develop a detailed account of constructions where de combines with an N'. We provide a unitary analysis of de in three constructions (quantifier extraction, "quantification at a distance", and negative contexts) which have been not been considered to be related in previous accounts.
In French, Italian, and Romanian, forms inherited from the Latin paradigm 'esse' are used for the copula, the passive auxiliary and tense or perfective auxiliaries. We show that the copula and the passive auxiliary should be identified, while the tense or perfective auxiliaries are different lexemes. Moreover, the copula has the same description across all the Romance languages. While they all are argument inheritance verbs, the copula and the tense or perfective auxiliaries differ with respect to their complement structure: (i) the second only have one complement structure (the complement participle is complement unsaturated), the copula has two complement structures (the predicate is either complement saturated or unsaturated); (ii) French and Italian tense auxiliaries are the head of a flat VP, where the participle is sister to its subcategorized complements, the Romanian perfective auxiliary is the head of a verbal complex; (iii) when the complement predicate is unsaturated, the Romance copula is the head of a flat VP.
Two consequences of the analysis are worth mentioning. First, the copula (and the passive auxiliary) should not be taken into account when stating the environments for auxiliary selection in French and Italian. Second, argument inheritance and complement structure are different phenomena, and argue in favor of theories which systematically distinguish between valence features and constituent structures.
While French degree words in French have been assigned several syntactic categories, we show that they are rather highy polymorphic adverbs (they occur in all syntactic domains), which select the expression they modify on a purely semantic basis. Like French adverbs in general, they occur both to the left and to the right of the head they modify. Following previous work (a.o. van Noord and Bouma 1994, Abeillé and Godard 1997, Bouma et al. 2000), we assign them two different grammatical functions, adjuncts and complements. Semantically, they differ from quantifiers. We follow Kennedy (2000) who analyzes them as scalar predicate modifiers. Finally, the specific syntactic constraints that characterize a subset of them can be shown to follow from, or be related to, their weight properties (Abeillé and Godard 2000). We conclude that their apparently idiosyncratic properties fit into a more general theory of grammar.
Neuronale Repräsentation intrinsischer cochleärer Signale im Colliculus inferior der Wüstenrennmaus
(2008)
Die vorliegende Arbeit untersucht die neuronale Repräsentation von cochleären Verzerrungsprodukten im auditorischen Mittelhirn der Wüstenrennmaus. Die hohe Sensitivität und die gute Frequenzauflösung des Hörorgans der Säugetiere basiert auf einer aktiven mechanischen Verstärkung der schallinduzierten Basilarmembranschwingung im Innenohr. Die äußeren Haarsinneszellen, die während des Transduktionsprozesses zyklisch ihre Länge ändern und dabei zusätzliche Schwingungsenergie in das System zurückführen, sind der zugrunde liegende Motor des aktiven cochleären Verstärkers. Die stark nichtlinearen Eigenschaften dieses Verstärkers führen allerdings bei gleichzeitiger Verstärkung mehrerer Frequenzkomponenten zur Generierung von Kombinationsschwingungen, welche im Ursprungssignal nicht vorhanden sind. Wird das Ohr beispielsweise durch zwei Töne mit den Frequenzen f1 und f2 stimuliert (f1<f2), so entstehen verschiedene Kombinationsschwingungen, deren prominenteste das quadratische (f2-f1) und das cubische (2 f1-f2) Verzerrungsprodukt sind. Diese Verzerrungen des Ursprungssignals breiten sich von ihrem Entstehungsort im Innenohr, dem Überlappungsbereich der Stimuluswanderwellen, im Flüssigkeitsraum der Cochlea aus und werden über das Mittelohr in den Gehörgang übertragen. Im Gehörgang sind sie mit Hilfe eines sensitiven Mikrophons als otoakustische Emissionen (DPOAE - distortion product otoacoustic emissions) messbar. Zusätzlich bilden sie an ihrem Resonanzort auf der Basilarmembran, vergleichbar mit einem externen Stimuluston gleicher Frequenz, eine eigene Wanderwelle aus und aktivieren den Transduktionsprozess. Die neuronalen Korrelate der cochleären Verzerrungsprodukte sind auf verschiedenen Stationen der Hörbahn messbar und cochleäre Verzerrungsprodukte können als separate Töne wahrgenommen werden. In der vorliegenden Arbeit wurden die neuronalen Korrelate und otoakustischen Emissionen von cochleären Verzerrungsprodukten erstmals simultan bestimmt. Durch den direkten Vergleich der neuronalen Aktivität mit der peripheren Emissionsmessung sollen eventuelle zentralnervöse Veränderungen der Repräsentation der cochleären Verzerrungsprodukte untersucht werden. Dazu wurde die elektrische Aktivität von 91 Neuronen des Colliculus inferior der Wüstenrennmaus während der Stimulation durch zwei hochfrequente Stimulustöne gemessen. Die Frequenzen der Stimulustöne waren so gewählt, dass die Frequenz eines, durch sie evozierten Verzerrungsproduktes, mit der charakteristischen Frequenz des jeweiligen Neurons übereinstimmte. In 95 % aller Messungen konnte eine robuste neuronale Aktivität während Zweitonstimulation gemessen werden, die sich auf die Stimulation durch ein spezifisches cochleäres Verzerrungsprodukt zurückführen lässt. Bei einem Teil der Versuche wurden die Verzerrungsprodukte durch direkte intracochleäre Auslöschung mit einem dritten Tonstimulus eindeutig als Quelle der neuronalen Aktivität bestätigt. Für Verzerrungsproduktfrequenzen oberhalb 1,3 kHz lassen sich die Antworten der Neurone im schwellennahen Bereich gut mit den simultan im Gehörgang bestimmten DPOAE-Pegeln erklären, was einen engen Zusammenhang zwischen intracochleärem Verzerrungsproduktpegel und DPOAE-Pegel nahe legt. Bei höheren Stimuluspegeln konnten die maximalen neuronalen Antworten auf den intracochleären Verzerrungsproduktstimulus signifikant von der Einzeltonantwort abweichen, wobei sowohl eine Erhöhung als auch eine Reduktion der Maximalantwort möglich war. Ein inhibitorischer bzw. verstärkender Einfluss der Stimulustöne auf die neuronale Verzerrungsproduktantwort wird als mögliche Ursache der Unterschiede diskutiert. Für Verzerrungsproduktfrequenzen unterhalb 1,3 kHz wurde ein deutlicher Unterschied zwischen dem intracochleären Verzerrungsproduktpegel und dem im Gehörgang gemessenen Emissionspegel deutlich. Ein Teil der getesteten tieffrequenten Neurone antwortete während Zweitonstimulation bereits für Stimuluspegel, die unterhalb der Reintonschwelle des Neurons lagen. Eine frequenzspezifische Verschlechterung der Mittelohrübertragungsleistung bei tiefen Frequenzen wird als mögliche Ursache für die unterschwelligen Antworten der Neurone diskutiert. Die Ergebnisse der vorliegenden Arbeit zeigen, dass cochleäre Verzerrungsprodukte einen substanziellen Anteil an der neuronalen Repräsentation von komplexen Stimuli haben können. Im Besonderen machen die vorgestellten Daten deutlich, dass die neuronalen Repräsentation der Grundfrequenz eines komplexen Klangs wesentlich von cochleären Verzerrungsprodukten beeinflusst sein kann. Dies bedeutet, dass bereits im Innenohr Tonhöheninformation extrahiert werden kann und damit die Relevanz in der Literatur diskutierter neuronaler Mechanismen zur Berechnung von Tonhöhe relativiert wird.
"Calderón als religiöser Dichter" ist einer von Krauss' interessantesten Aufsätzen der frühen Jahre, von denen "einige zur Zeit ihres Erscheinens wissenschaftlich bahnbrechend waren", wie Hans Ulrich Gumbrecht in seinem Porträt von Werner Krauss in "Das Leben und Sterben der großen Romanisten" konstatiert. [...] Erwartbar wäre gewesen, in Calderón das Ende des mittelalterlich geprägten Kosmos zu sehen, des imperialen 'Goldenen Zeitalters' Spaniens (ca. 1550 bis 1680), in dem es im barocken Schauspiel zu Exzessen der illusionistischen Überwältigung und Massenspektakeln des Glaubens kam. Doch für Krauss ist Calderón vielmehr ein Weg, der direkt in die Dialektik der Aufklärung führt. Das Rettbare, das auf die Praxis des konkreten Handelns Beziehbare muss bei Calderón das Widerständige sein, das auch Carlo Barck an Krauss' Studie faszinierte. [...] Zwei Gedanken lassen sich aus seinem Artikel filtern, die sich an aktuell stark diskutierte Probleme anschließen lassen. Zum einen geht es um Materialität, zum anderen um humanistische Anliegen, die sich in den Kulturtechniken einer Religionskultur wie der des spanischen Katholizismus des 17. Jahrhunderts auffinden und aktualisieren lassen, etwa im Bilderhandeln oder im Umgang mit Schuldempfinden. Es spricht für Krauss' weitreichendes Verständnis religiöser Phänomene, dass er an ihnen Dinge wie Präsenz, Immersion und Liminalität auf den Punkt bringen konnte.
Was macht eine höfisch kultivierte Dame oder einen höfischen Ritter aus? Die mittelalterliche, von Frankreich ausgehende Artusepik antwortet auf diese Frage unter Bezug auf drei Komponenten, nämlich eine edle Abkunft (Geburtsadel), eine edle Gesinnung (Tugendadel) und einen gewissen höfischen Lebensstil, zu dem, ganz zentral, auch höfische Luxus- und Repräsentationsobjekte gehören, so etwa ritterliche Bewaffnung und kostbare Kleidung. Was passiert, wenn es an einer Harmonie von innen und außen öffentlich sichtbar mangelt und die Wirkungseinheit von Mensch und Repräsentationsobjekt zu Bruch geht, zeigt uns die mittelalterliche Erzählung vom schlecht geschnittenen Mantel, altfranzösisch: du mantel mautaillé. Sie nimmt in Frankreich des 13. Jahrhunderts (zwischen 1200 und 1210) ihren Anfang, und zwar in Gestalt des Lais (Le lay du cort mantel), einer kurzen Verserzählung keltischer Stoffe (lai narratif ), und verbreitet sich rasch in Europa.
Living matter is defined by metastability, implying a tightly balanced synthesis and turnover of cellular components. The first step of eukaryotic protein degradation via the ubiquitin-proteasome system (UPS) leads to peptides, which are subsequently degraded to single amino acids by an armada of proteases. A small fraction of peptides, however, escapes further cytosolic destruction and is transported by ATP-binding cassette (ABC) transporters into the endoplasmic reticulum (ER) and lysosomes. The ER-resident heterodimeric transporter associated with antigen processing (TAP) is a crucial component in adaptive immunity for the transport and loading of peptides onto major histocompatibility complex class I (MHC I) molecules. Although the function of the lysosomal resident homodimeric TAPL-like (TAPL) remains, until today, only loosely defined, an involvement in immune defense is anticipated since it is highly expressed in dendritic cells and macrophages. Here, we compare the gene organization and the function of single domains of both peptide transporters. We highlight the structural organization, the modes of substrate binding and translocation as well as physiological functions of both organellar transporters.
The ALICE experiment has measured low-mass dimuon production in pp collisions at √s=7 TeV in the dimuon rapidity region 2.5<y<4. The observed dimuon mass spectrum is described as a superposition of resonance decays (η,ρ,ω,η′,ϕ) into muons and semi-leptonic decays of charmed mesons. The measured production cross sections for ω and ϕ are σω(1<pt<5 GeV/c,2.5<y<4)=5.28±0.54(stat)±0.49(syst) mb and σϕ(1<pt<5 GeV/c,2.5<y<4)=0.940±0.084(stat)±0.076(syst) mb. The differential cross sections d2σ/dydpt are extracted as a function of pt for ω and ϕ. The ratio between the ρ and ω cross section is obtained. Results for the ϕ are compared with other measurements at the same energy and with predictions by models.
he first measurements of the invariant differential cross sections of inclusive π0 and η meson production at mid-rapidity in proton–proton collisions at s=0.9 TeV and s=7 TeV are reported. The π0 measurement covers the ranges 0.4<pT<7 GeV/c and 0.3<pT<25 GeV/c for these two energies, respectively. The production of η mesons was measured at s=√7 TeV in the range 0.4<pT<15 GeV/c. Next-to-Leading Order perturbative QCD calculations, which are consistent with the π0 spectrum at s=0.9 TeV, overestimate those of π0 and η mesons at s=√7 TeV, but agree with the measured η/π0 ratio at s=√7 TeV.
The ALICE Collaboration has made the first measurement at the LHC of J/ψ photoproduction in ultra-peripheral Pb–Pb collisions at sNN=2.76 TeV. The J/ψ is identified via its dimuon decay in the forward rapidity region with the muon spectrometer for events where the hadronic activity is required to be minimal. The analysis is based on an event sample corresponding to an integrated luminosity of about 55 μb−1. The cross section for coherent J/ψ production in the rapidity interval −3.6<y<−2.6 is measured to be dσJ/ψcoh/dy=1.00±0.18(stat)−0.26+0.24(syst) mb. The result is compared to theoretical models for coherent J/ψ production and found to be in good agreement with those models which include nuclear gluon shadowing.
Identical neutral kaon pair correlations are measured in √s=7 TeV pp collisions in the ALICE experiment. One-dimensional Ks0Ks0 correlation functions in terms of the invariant momentum difference of kaon pairs are formed in two multiplicity and two transverse momentum ranges. The femtoscopic parameters for the radius and correlation strength of the kaon source are extracted. The fit includes quantum statistics and final-state interactions of the a0/f0 resonance. Ks0Ks0 correlations show an increase in radius for increasing multiplicity and a slight decrease in radius for increasing transverse mass, mT, as seen in ππ correlations in pp collisions and in heavy-ion collisions. Transverse mass scaling is observed between the Ks0Ks0 and ππ radii. Also, the first observation is made of the decay of the f2′(1525) meson into the Ks0Ks0 channel in pp collisions.
The ALICE Collaboration has measured inclusive J/ψ production in pp collisions at a center-of-mass energy √s=2.76 TeV at the LHC. The results presented in this Letter refer to the rapidity ranges |y|<0.9 and 2.5<y<4 and have been obtained by measuring the electron and muon pair decay channels, respectively. The integrated luminosities for the two channels are Linte=1.1 nb−1 and Lintμ=19.9 nb−1, and the corresponding signal statistics are NJ/ψe+e−=59±14 and NJ/ψμ+μ−=1364±53. We present dσJ/ψ/dy for the two rapidity regions under study and, for the forward-y range, d2σJ/ψ/dydpt in the transverse momentum domain 0<pt<8 GeV/c. The results are compared with previously published results at s=7 TeV and with theoretical calculations.
The ALICE Collaboration reports the measurement of the relative J/ψ yield as a function of charged particle pseudorapidity density dNch/dη in pp collisions at √s=7 TeV at the LHC. J/ψ particles are detected for pt>0, in the rapidity interval |y|<0.9 via decay into e+e−, and in the interval 2.5<y<4.0 via decay into μ+μ− pairs. An approximately linear increase of the J/ψ yields normalized to their event average (dNJ/ψ/dy)/〈dNJ/ψ/dy〉 with (dNch/dη)/〈dNch/dη〉 is observed in both rapidity ranges, where dNch/dη is measured within |η|<1 and pt>0. In the highest multiplicity interval with 〈dNch/dη(bin)〉=24.1, corresponding to four times the minimum bias multiplicity density, an enhancement relative to the minimum bias J/ψ yield by a factor of about 5 at 2.5<y<4 (8 at |y|<0.9) is observed.
The elliptic, v2, triangular, v3, and quadrangular, v4, azimuthal anisotropic flow coefficients are measured for unidentified charged particles, pions, and (anti-)protons in Pb–Pb collisions at √sNN=2.76 TeV with the ALICE detector at the Large Hadron Collider. Results obtained with the event plane and four-particle cumulant methods are reported for the pseudo-rapidity range |η|<0.8 at different collision centralities and as a function of transverse momentum, pT, out to pT=20 GeV/c. The observed non-zero elliptic and triangular flow depends only weakly on transverse momentum for pT>8 GeV/c. The small pT dependence of the difference between elliptic flow results obtained from the event plane and four-particle cumulant methods suggests a common origin of flow fluctuations up to pT=8 GeV/c. The magnitude of the (anti-)proton elliptic and triangular flow is larger than that of pions out to at least pT=8 GeV/c indicating that the particle type dependence persists out to high pT.
The production cross section of electrons from semileptonic decays of beauty hadrons was measured at mid-rapidity (|y|<0.8) in the transverse momentum range 1<pT<8 GeV/c with the ALICE experiment at the CERN LHC in pp collisions at a center of mass energy √s=7 TeV using an integrated luminosity of 2.2 nb−1. Electrons from beauty hadron decays were selected based on the displacement of the decay vertex from the collision vertex. A perturbative QCD calculation agrees with the measurement within uncertainties. The data were extrapolated to the full phase space to determine the total cross section for the production of beauty quark–antiquark pairs.
The inclusive transverse momentum (pT) distributions of primary charged particles are measured in the pseudo-rapidity range |η|<0.8 as a function of event centrality in Pb–Pb collisions at √sNN=2.76 TeV with ALICE at the LHC. The data are presented in the pT range 0.15<pT<50 GeV/c for nine centrality intervals from 70–80% to 0–5%. The results in Pb–Pb are presented in terms of the nuclear modification factor RAA using a pp reference spectrum measured at the same collision energy. We observe that the suppression of high-pT particles strongly depends on event centrality. The yield is most suppressed in central collisions (0–5%) with RAA≈0.13 at pT=6–7 GeV/c. Above pT=7 GeV/c, there is a significant rise in the nuclear modification factor, which reaches RAA≈0.4 for pT>30 GeV/c. In peripheral collisions (70–80%), only moderate suppression (RAA=0.6–0.7) and a weak pT dependence is observed. The measured nuclear modification factors are compared to other measurements and model calculations.
The pT-differential inclusive production cross section of the prompt charm-strange meson Ds+ in the rapidity range |y|<0.5 was measured in proton–proton collisions at s=7 TeV at the LHC using the ALICE detector. The analysis was performed on a data sample of 2.98×108 events collected with a minimum-bias trigger. The corresponding integrated luminosity is Lint=4.8 nb−1. Reconstructing the decay Ds+→ϕπ+, with ϕ→K−K+, and its charge conjugate, about 480 Ds± mesons were counted, after selection cuts, in the transverse momentum range 2<pT<12 GeV/c. The results are compared with predictions from models based on perturbative QCD. The ratios of the cross sections of four D meson species (namely D0, D+, D⁎+ and Ds+) were determined both as a function of pT and integrated over pT after extrapolating to full pT range, together with the strangeness suppression factor in charm fragmentation. The obtained values are found to be compatible within uncertainties with those measured by other experiments in e+e−, ep and pp interactions at various centre-of-mass energies.
A measurement of the multi-strange Ξ− and Ω− baryons and their antiparticles by the ALICE experiment at the CERN Large Hadron Collider (LHC) is presented for inelastic proton–proton collisions at a centre-of-mass energy of 7 TeV. The transverse momentum (pT) distributions were studied at mid-rapidity (|y|<0.5) in the range of 0.6<pT<8.5 GeV/c for Ξ− and Ξ¯+ baryons, and in the range of 0.8<pT<5 GeV/c for Ω− and Ω¯+. Baryons and antibaryons were measured as separate particles and we find that the baryon to antibaryon ratio of both particle species is consistent with unity over the entire range of the measurement. The statistical precision of the current data has allowed us to measure a difference between the mean pT of Ξ− (Ξ¯+) and Ω− (Ω¯+). Particle yields, mean pT, and the spectra in the intermediate pT range are not well described by the PYTHIA Perugia 2011 tune Monte Carlo event generator, which has been tuned to reproduce the early LHC data. The discrepancy is largest for Ω− (Ω¯+). This PYTHIA tune approaches the pT spectra of Ξ− and Ξ¯+ baryons below pT<0.85 GeV/c and describes the Ξ− and Ξ¯+ spectra above pT>6.0 GeV/c. We also illustrate the difference between the experimental data and model by comparing the corresponding ratios of (Ω−+Ω¯+)/(Ξ−+Ξ¯+) as a function of transverse mass.
Heavy flavour decay muon production at forward rapidity in proton–proton collisions at √s=7 TeV
(2012)
The production of muons from heavy flavour decays is measured at forward rapidity in proton–proton collisions at √s=7 TeV collected with the ALICE experiment at the LHC. The analysis is carried out on a data sample corresponding to an integrated luminosity Lint=16.5 nb−1. The transverse momentum and rapidity differential production cross sections of muons from heavy flavour decays are measured in the rapidity range 2.5<y<4, over the transverse momentum range 2<pt<12 GeV/c. The results are compared to predictions based on perturbative QCD calculations.
A measurement of the transverse momentum spectra of jets in Pb-Pb collisions at sNN−−−√=2.76 TeV is reported. Jets are reconstructed from charged particles using the anti-kT jet algorithm with jet resolution parameters R of 0.2 and 0.3 in pseudo-rapidity |η|<0.5. The transverse momentum pT of charged particles is measured down to 0.15 GeV/c which gives access to the low pT fragments of the jet. Jets found in heavy-ion collisions are corrected event-by-event for average background density and on an inclusive basis (via unfolding) for residual background fluctuations and detector effects. A strong suppression of jet production in central events with respect to peripheral events is observed. The suppression is found to be similar to the suppression of charged hadrons, which suggests that substantial energy is radiated at angles larger than the jet resolution parameter R=0.3 considered in the analysis. The fragmentation bias introduced by selecting jets with a high pT leading particle, which rejects jets with a soft fragmentation pattern, has a similar effect on the jet yield for central and peripheral events. The ratio of jet spectra with R=0.2 and R=0.3 is found to be similar in Pb-Pb and simulated PYTHIA pp events, indicating no strong broadening of the radial jet structure in the reconstructed jets with R<0.3.
Transverse momentum spectra of π±, K± and p(p¯) up to pT = 20 GeV/c at mid-rapidity in pp, peripheral (60–80%) and central (0–5%) Pb–Pb collisions at √sNN = 2.76 TeV have been measured using the ALICE detector at the Large Hadron Collider. The proton-to-pion and the kaon-to-pion ratios both show a distinct peak at pT ≈ 3 GeV/c in central Pb–Pb collisions. Below the peak, pT < 3 GeV/c, both ratios are in good agreement with hydrodynamical calculations, suggesting that the peak itself is dominantly the result of radial flow rather than anomalous hadronization processes. For pT > 10 GeV/c particle ratios in pp and Pb–Pb collisions are in agreement and the nuclear modification factors for π±, K± and p(p¯) indicate that, within the systematic and statistical uncertainties, the suppression is the same. This suggests that the chemical composition of leading particles from jets in the medium is similar to that of vacuum jets.
We report on the production of inclusive Υ (1S) and Υ (2S) in p–Pb collisions at √sNN = 5.02 TeV at the LHC. The measurement is performed with the ALICE detector at backward (−4.46 < ycms < −2.96) and forward (2.03 .< ycms < 3.53) rapidity down to zero transverse momentum. The production cross sections of the Υ (1S) and Υ (2S) are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of Υ (1S). A suppression of the inclusive Υ (1S) yield in p–Pb collisions with respect to the yield from pp collisions scaled by the number of binary nucleon–nucleon collisions is observed at forward rapidity but not at backward rapidity. The results are compared to theoretical model calculations including nuclear shadowing or partonic energy loss effect.
The ALICE Collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y| < 0.8 and transverse momentum 1 < pT < 10 GeV/c, in pp collisions at √s = 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD predictions agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, σb→e = 3.47 ± 0.40(stat) +1.12 −1.33(sys) ± 0.07(norm) μb, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) calculations to obtain the total bb production ¯ cross section, σbb¯ = 130 ± 15.1(stat) +42.1 −49.8(sys) +3.4 −3.1(extr) ± 2.5(norm) ± 4.4(BR) μb.
Transverse momentum spectra of π±, K± and p(p¯) up to pT = 20 GeV/c at mid-rapidity in pp and Pb-Pb collisions at sNN−−−√= 2.76 TeV have been measured using the ALICE detector at the Large Hadron Collider. The proton-to-pion and the kaon-to-pion ratios both show a distinct peak at pT≈3GeV/c in central Pb-Pb collisions. Below the peak, pT < 3 GeV/c, both ratios are in good agreement with hydrodynamical calculations, suggesting that the peak itself is dominantly the result of radial flow rather than anomalous hadronization processes. For pT > 10 GeV/c particle ratios in pp and Pb-Pb collisions are in agreement and the nuclear modification factors for π±, K± and p(p¯) indicate that, within the systematic and statistical uncertainties, the suppression is the same. This suggests that the chemical composition of leading particles from jets in the medium is similar to that of vacuum jets.
The pT-differential production cross section of electrons from semileptonic decays of heavy-flavor hadrons has been measured at mid-rapidity in proton-proton collisions at s√=2.76 TeV in the transverse momentum range 0.5 < pT < 12 GeV/c with the ALICE detector at the LHC. The analysis was performed using minimum bias events and events triggered by the electromagnetic calorimeter. Predictions from perturbative QCD calculations agree with the data within the theoretical and experimental uncertainties.
The pT-differential production cross section of electrons from semileptonic decays of heavy-flavor hadrons has been measured at mid-rapidity in proton-proton collisions at s√=2.76 TeV in the transverse momentum range 0.5 < pT < 12 GeV/c with the ALICE detector at the LHC. The analysis was performed using minimum bias events and events triggered by the electromagnetic calorimeter. Predictions from perturbative QCD calculations agree with the data within the theoretical and experimental uncertainties.
We report on the production of inclusive Υ(1S) and Υ(2S) in p-Pb collisions at sNN−−−√=5.02 TeV at the LHC. The measurement is performed with the ALICE detector at backward (−4.46<ycms<−2.96) and forward (2.03<ycms<3.53) rapidity down to zero transverse momentum. The production cross sections of the Υ(1S) and Υ(2S) are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of Υ(1S). A suppression of the inclusive Υ(1S) yield in p-Pb collisions with respect to the yield from pp collisions scaled by the number of binary nucleon-nucleon collisions is observed at forward rapidity but not at backward rapidity. The results are compared to theoretical model calculations including nuclear shadowing or partonic energy loss effects.
We report on the production of inclusive Υ(1S) and Υ(2S) in p-Pb collisions at sNN−−−√=5.02 TeV at the LHC. The measurement is performed with the ALICE detector at backward (−4.46<ycms<−2.96) and forward (2.03<ycms<3.53) rapidity down to zero transverse momentum. The production cross sections of the Υ(1S) and Υ(2S) are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of Υ(1S). A suppression of the inclusive Υ(1S) yield in p-Pb collisions with respect to the yield from pp collisions scaled by the number of binary nucleon-nucleon collisions is observed at forward rapidity but not at backward rapidity. The results are compared to theoretical model calculations including nuclear shadowing or partonic energy loss effects.
The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at centre-of-mass energy s√=7 TeV using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the mid-rapidity region using the sequential recombination kT and anti-kT as well as the SISCone jet finding algorithms with several resolution parameters in the range R=0.2 to 0.6. Differential jet production cross sections measured with the three jet finders are in agreement in the transverse momentum (pT) interval 20<pjet,chT<100 GeV/c. They are also consistent with prior measurements carried out at the LHC by the ATLAS collaboration. The jet charged particle multiplicity rises monotonically with increasing jet pT, in qualitative agreement with prior observations at lower energies. The transverse profiles of leading jets are investigated using radial momentum density distributions as well as distributions of the average radius containing 80% (⟨R80⟩) of the reconstructed jet pT. The fragmentation of leading jets with R=0.4 using scaled pT spectra of the jet constituents is studied. The measurements are compared to model calculations from event generators (PYTHIA, PHOJET, HERWIG). The measured radial density distributions and ⟨R80⟩ distributions are well described by the PYTHIA model (tune Perugia-2011). The fragmentation distributions are better described by HERWIG.
The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at centre-of-mass energy s√=7 TeV using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the mid-rapidity region using the sequential recombination kT and anti-kT as well as the SISCone jet finding algorithms with several resolution parameters in the range R=0.2 to 0.6. Differential jet production cross sections measured with the three jet finders are in agreement in the transverse momentum (pT) interval 20<pjet,chT<100 GeV/c. They are also consistent with prior measurements carried out at the LHC by the ATLAS collaboration. The jet charged particle multiplicity rises monotonically with increasing jet pT, in qualitative agreement with prior observations at lower energies. The transverse profiles of leading jets are investigated using radial momentum density distributions as well as distributions of the average radius containing 80% (⟨R80⟩) of the reconstructed jet pT. The fragmentation of leading jets with R=0.4 using scaled pT spectra of the jet constituents is studied. The measurements are compared to model calculations from event generators (PYTHIA, PHOJET, HERWIG). The measured radial density distributions and ⟨R80⟩ distributions are well described by the PYTHIA model (tune Perugia-2011). The fragmentation distributions are better described by HERWIG.
The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at centre-of-mass energy s√=7 TeV using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the mid-rapidity region using the sequential recombination kT and anti-kT as well as the SISCone jet finding algorithms with several resolution parameters in the range R=0.2 to 0.6. Differential jet production cross sections measured with the three jet finders are in agreement in the transverse momentum (pT) interval 20<pjet,chT<100 GeV/c. They are also consistent with prior measurements carried out at the LHC by the ATLAS collaboration. The jet charged particle multiplicity rises monotonically with increasing jet pT, in qualitative agreement with prior observations at lower energies. The transverse profiles of leading jets are investigated using radial momentum density distributions as well as distributions of the average radius containing 80% (⟨R80⟩) of the reconstructed jet pT. The fragmentation of leading jets with R=0.4 using scaled pT spectra of the jet constituents is studied. The measurements are compared to model calculations from event generators (PYTHIA, PHOJET, HERWIG). The measured radial density distributions and ⟨R80⟩ distributions are well described by the PYTHIA model (tune Perugia-2011). The fragmentation distributions are better described by HERWIG.
Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at s√ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at sNN−−−−√ = 2.76 TeV are studied as a function of the charged-particle multiplicity using the ALICE detector at the LHC. Dynamical fluctuations indicative of correlated particle emission are observed in all systems. The results in pp collisions show little dependence on collision energy. The Monte Carlo event generators PYTHIA and PHOJET are in qualitative agreement with the data. Peripheral Pb-Pb data exhibit a similar multiplicity dependence as that observed in pp. In central Pb-Pb, the results deviate from this trend, featuring a significant reduction of the fluctuation strength. The results in Pb--Pb are in qualitative agreement with previous measurements in Au-Au at lower collision energies and with expectations from models that incorporate collective phenomena.
The ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y|<0.8 and transverse momentum 1<pT<10 GeV/c, in pp collisions at s√= 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD calculations agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, σb→e=3.47±0.40(stat)+1.12−1.33(sys)±0.07(norm)μb, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total bb¯ production cross section, σbb¯=130±15.1(stat)+42.1−49.8(sys)+3.4−3.1(extr)±2.5(norm)±4.4(BR)μb.
The ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y|<0.8 and transverse momentum 1<pT<10 GeV/c, in pp collisions at s√= 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD calculations agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, σb→e=3.47±0.40(stat)+1.12−1.33(sys)±0.07(norm)μb, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total bb¯ production cross section, σbb¯=130±15.1(stat)+42.1−49.8(sys)+3.4−3.1(extr)±2.5(norm)±4.4(BR)μb.
Freeze-out radii extracted from three-pion cumulants in pp, p–Pb and Pb–Pb collisions at the LHC
(2014)
In high-energy collisions, the spatio-temporal size of the particle production region can be measured using the Bose–Einstein correlations of identical bosons at low relative momentum. The source radii are typically extracted using two-pion correlations, and characterize the system at the last stage of interaction, called kinetic freeze-out. In low-multiplicity collisions, unlike in high-multiplicity collisions, two-pion correlations are substantially altered by background correlations, e.g. mini-jets. Such correlations can be suppressed using three-pion cumulant correlations. We present the first measurements of the size of the system at freeze-out extracted from three-pion cumulant correlations in pp, p–Pb and Pb–Pb collisions at the LHC with ALICE. At similar multiplicity, the invariant radii extracted in p–Pb collisions are found to be 5–15% larger than those in pp, while those in Pb–Pb are 35–55% larger than those in p–Pb. Our measurements disfavor models which incorporate substantially stronger collective expansion in p–Pb as compared to pp collisions at similar multiplicity.
Two-particle angular correlations between unidentified charged trigger and associated particles are measured by the ALICE detector in p–Pb collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV. The transverse-momentum range 0.7 < pT,assoc < pT,trig < 5.0 GeV/c is examined, to include correlations induced by jets originating from low momentum-transfer scatterings (minijets). The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range |η| < 0.9. The near-side long-range pseudorapidity correlations observed in high-multiplicity p–Pb collisions are subtracted from both near-side short-range and away-side correlations in order to remove the non-jet-like components. The yields in the jet-like peaks are found to be invariant with event multiplicity with the exception of events with low multiplicity. This invariance is consistent with the particles being produced via the incoherent fragmentation of multiple parton–parton scatterings, while the yield related to the previously observed ridge structures is not jet-related. The number of uncorrelated sources of particle production is found to increase linearly with multiplicity, suggesting no saturation of the number of multi-parton interactions even in the highest multiplicity p–Pb collisions. Further, the number scales only in the intermediate multiplicity region with the number of binary nucleon–nucleon collisions estimated with a Glauber Monte-Carlo simulation.
We report on the measurement of the inclusive Υ (1S) production in Pb–Pb collisions at √sNN = 2.76 TeV carried out at forward rapidity (2.5 < y < 4) and down to zero transverse momentum using its μ+μ−decay channel with the ALICE detector at the Large Hadron Collider. A strong suppression of the inclusive Υ (1S) yield is observed with respect to pp collisions scaled by the number of independent nucleon–nucleon collisions. The nuclear modification factor, for events in the 0–90% centrality range, amounts to 0.30 ± 0.05(stat) ± 0.04(syst). The observed Υ (1S) suppression tends to increase with the centrality of the collision and seems more pronounced than in corresponding mid-rapidity measurements. Our results are compared with model calculations, which are found to underestimate the measured suppression and fail to reproduce its rapidity dependence.
Long-range angular correlations on the near and away side in p–Pb collisions at √sNN=5.02 TeV
(2013)
Angular correlations between charged trigger and associated particles are measured by the ALICE detector in p–Pb collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV for transverse momentum ranges within 0.5<pT,assoc<pT,trig<4 GeV/c. The correlations are measured over two units of pseudorapidity and full azimuthal angle in different intervals of event multiplicity, and expressed as associated yield per trigger particle. Two long-range ridge-like structures, one on the near side and one on the away side, are observed when the per-trigger yield obtained in low-multiplicity events is subtracted from the one in high-multiplicity events. The excess on the near-side is qualitatively similar to that recently reported by the CMS Collaboration, while the excess on the away-side is reported for the first time. The two-ridge structure projected onto azimuthal angle is quantified with the second and third Fourier coefficients as well as by near-side and away-side yields and widths. The yields on the near side and on the away side are equal within the uncertainties for all studied event multiplicity and pT bins, and the widths show no significant evolution with event multiplicity or pT. These findings suggest that the near-side ridge is accompanied by an essentially identical away-side ridge.
We study the beam-energy and system-size dependence of \phi meson production (using the hadronic decay mode \phi -- K+K-) by comparing the new results from Cu+Cu collisions and previously reported Au+Au collisions at \sqrt{s_NN} = 62.4 and 200 GeV measured in the STAR experiment at RHIC. Data presented are from mid-rapidity (|y|<0.5) for 0.4 < pT < 5 GeV/c. At a given beam energy, the transverse momentum distributions for \phi mesons are observed to be similar in yield and shape for Cu+Cu and Au+Au colliding systems with similar average numbers of participating nucleons. The \phi meson yields in nucleus-nucleus collisions, normalised by the average number of participating nucleons, are found to be enhanced relative to those from p+p collisions with a different trend compared to strange baryons. The enhancement for \phi mesons is observed to be higher at \sqrt{s_NN} = 200 GeV compared to 62.4 GeV. These observations for the produced \phi(s\bar{s}) mesons clearly suggest that, at these collision energies, the source of enhancement of strange hadrons is related to the formation of a dense partonic medium in high energy nucleus-nucleus collisions and cannot be alone due to canonical suppression of their production in smaller systems.
The STAR Collaboration at the Relativistic Heavy Ion Collider presents measurements of 𝐽/𝜓→𝑒+𝑒− at midrapidity and high transverse momentum (𝑝𝑇>5 GeV/𝑐) in 𝑝+𝑝 and central Cu+Cu collisions at √𝑠𝑁𝑁=200 GeV. The inclusive 𝐽/𝜓 production cross section for Cu+Cu collisions is found to be consistent at high 𝑝𝑇 with the binary collision-scaled cross section for 𝑝+𝑝 collisions. At a confidence level of 97%, this is in contrast to a suppression of 𝐽/𝜓 production observed at lower 𝑝𝑇. Azimuthal correlations of 𝐽/𝜓 with charged hadrons in 𝑝+𝑝 collisions provide an estimate of the contribution of 𝐵-hadron decays to 𝐽/𝜓 production of 13%±5%.
This is a summary of Elena Abella Pérez's doctoral thesis "Factores ambientales y de manejo que afectan al desarrollo embrionario de la tortuga marina Caretta caretta. Implicaciones en programas de incubación controlada", Estación Biológica de Doñana (CSIC) and Departamento de Biología, Universidad de Las Palmas de Gran Canaria, 29 October 2010.
Der Deutschunterricht in den ersten Jahrzehnten nach 1800 versuchte durch Stilübungen und aus der Rhetorik übernommene Techniken die Schüler zu befähigen, Texte verschiedener Art zu verfassen und sie, wie in Bismarcks Zeugnis vermerkt ist, zur sprachlichen Gewandtheit zu befähigen. Ob die Lektüre literarischer Werke in deutscher Sprache eine der Voraussetzungen dazu sei, war umstritten. Erst in den auf das Jahr 1830 folgenden Jahrzehnten setzte sich die Ansicht durch, daß literarische Bildung, vor allem vermittelt durch die Werke 'klassischer' Schriftsteller, eine der Aufgaben des deutschen Unterrichts sei. Man könnte die Gleichzeitigkeit der Epoche "Vormärz! und des genannten Vorgangs der Aufnahme klassischer deutscher Literatur in den Unterricht der Schulen, zunächst des Gymnasiums, dann aber auch der anderen Schularten, als zufällig ansehen.
Hartmut Abendschein zeigt in seinem Beitrag, wie bibliothekarische Praktiken und Konventionen zum kreativen Ausgangspunkt von verlegerischen und schriftstellerischen Entscheidungen werden können. Die Publikationen seines Verlags edition taberna kritika formieren sich in verschiedenen Reihen, die z. B. durch ihre Metadatensätze aufeinander bezogen sind, sodass das Verlagsprogramm selbst als konzeptionelles Kunstwerk zu verstehen ist.
Between 28 June and 17 September 2018, 27 cases of human West Nile virus infections were recorded in Austria; four cases of West Nile neuroinvasive disease, 11 cases of West Nile fever, six infections detected by blood donation screening and six imported cases. In addition, 18 cases of human Usutu virus infections (all blood donors) were recorded. This is the highest number of annual infections recorded in Austria since the introduction of both viruses.
Hepatitis Delta virus (HDV) is a satellite of Hepatitis B virus with a single-stranded circular RNA genome. HDV RNA genome synthesis is carried out in infected cells by cellular RNA polymerases with the assistance of the small hepatitis delta antigen (S-HDAg). Here we show that S-HDAg binds the bromodomain (BRD) adjacent to zinc finger domain 2B (BAZ2B) protein, a regulatory subunit of BAZ2B-associated remodeling factor (BRF) ISWI chromatin remodeling complexes. shRNA-mediated silencing of BAZ2B or its inactivation with the BAZ2B BRD inhibitor GSK2801 impairs HDV replication in HDV-infected human hepatocytes. S-HDAg contains a short linear interacting motif (SLiM) KacXXR, similar to the one recognized by BAZ2B BRD in histone H3. We found that the integrity of the S-HDAg SLiM sequence is required for S-HDAg interaction with BAZ2B BRD and for HDV RNA replication. Our results suggest that S-HDAg uses a histone mimicry strategy to co-activate the RNA polymerase II-dependent synthesis of HDV RNA and sustain HDV replication.
Measurements of the π±, K±, and proton double differential yields emitted from the surface of the 90-cm-long carbon target (T2K replica) were performed for the incoming 31 GeV/c protons with the NA61/SHINE spectrometer at the CERN SPS using data collected during 2010 run. The double differential π± yields were measured with increased precision compared to the previously published NA61/SHINE results, while the K± and proton yields were obtained for the first time. A strategy for dealing with the dependence of the results on the incoming proton beam profile is proposed. The purpose of these measurements is to reduce significantly the (anti)neutrino flux uncertainty in the T2K long-baseline neutrino experiment by constraining the production of (anti)neutrino ancestors coming from the T2K target.
Inhibitor of Apoptosis (IAP) proteins are expressed at high levels in many cancers and contribute to apoptosis resistance. Therefore, they represent promising anticancer drug targets. Here, we report that small molecule IAP inhibitors at subtoxic concentrations cooperate with monoclonal antibodies against TRAIL receptor 1 (Mapatumumab) or TRAIL receptor 2 (Lexatumumab) to induce apoptosis in neuroblastoma cells in a highly synergistic manner (combination index <0.1). Importantly, we identify RIP1 as a critical regulator of this synergism. RIP1 is required for the formation of a RIP1/FADD/caspase-8 complex that drives caspase-8 activation, cleavage of Bid into tBid, mitochondrial outer membrane permeabilization, full activation of caspase-3 and caspase-dependent apoptosis. Indeed, knockdown of RIP1 abolishes formation of the RIP1/FADD/caspase-8 complex, subsequent caspase activation and apoptosis upon treatment with IAP inhibitor and TRAIL receptor antibodies. Similarly, inhibition of RIP1 kinase activity by Necrostatin-1 inhibits IAP inhibitor- and TRAIL receptor-triggered apoptosis. By comparison, over-expression of the dominant-negative superrepressor IκBα-SR or addition of the TNFα-blocking antibody Enbrel does not inhibit IAP inhibitor- and Lexatumumab-induced apoptosis, pointing to a NF-κB- and TNFα-independent mechanism. Of note, IAP inhibitor also significantly reduces TRAIL receptor-mediated loss of cell viability of primary cultured neuroblastoma cells, underscoring the clinical relevance. By demonstrating that RIP1 plays a key role in the IAP inhibitor-mediated sensitization for Mapatumumab- or Lexatumumab-induced apoptosis, our findings provide strong rationale to develop the combination of IAP inhibitors and TRAIL receptor agonists as a new therapeutic strategy for the treatment of human cancer.
Since Inhibitor of Apoptosis (IAP) proteins have been implicated in cellular adaptation to endoplasmic reticulum (ER) stress, we investigated the regulation of ER stress-induced apoptosis by small-molecule second mitochondria-derived activator of caspase (Smac) mimetics that antagonize IAP proteins. Here, we discover that Smac mimetic suppresses tunicamycin (TM)-induced apoptosis via resolution of the unfolded protein response (UPR) and ER stress. Smac mimetics such as BV6 selectively inhibit apoptosis triggered by pharmacological or genetic inhibition of protein N-glycosylation using TM or knockdown of DPAGT1, the enzyme that catalyzes the first step of protein N-glycosylation. In contrast, BV6 does not rescue cell death induced by other typical ER stressors (i.e., thapsigargin (TG), dithiothreitol, brefeldin A, bortezomib, or 2-deoxyglucose). The protection from TM-triggered apoptosis is found for structurally different Smac mimetics and for genetic knockdown of cellular IAP (cIAP) proteins in several cancer types, underlining the broader relevance. Interestingly, lectin microarray profiling reveals that BV6 counteracts TM-imposed inhibition of protein glycosylation. BV6 consistently abolishes TM-stimulated accumulation of ER stress markers such as glucose-regulated protein 78 (GRP78) and C/EBP homologous protein (CHOP) and reduces protein kinase RNA-like ER kinase (PERK) phosphorylation and X box-binding protein 1 (XBP1) splicing upon TM treatment. BV6-stimulated activation of nuclear factor-κB (NF-κB) contributes to the resolution of ER stress, since NF-κB inhibition by overexpression of dominant-negative IκBα superrepressor counteracts the suppression of TM-stimulated transcriptional activation of CHOP and GRP78 by BV6. Thus, our study is the first to show that Smac mimetic protects from TM-triggered apoptosis by resolving the UPR and ER stress. This provides new insights into the regulation of cellular stress responses by Smac mimetics.
We develop a two-sector incomplete markets integrated assessment model to analyze the effectiveness of green quantitative easing (QE) in complementing fiscal policies for climate change mitigation. We model green QE through an outstanding stock of private assets held by a monetary authority and its portfolio allocation between a clean and a dirty sector of production. Green QE leads to a partial crowding out of private capital in the green sector and to a modest reduction of the global temperature by 0.04 degrees of Celsius until 2100. A moderate global carbon tax of 50 USD per tonne of carbon is 4 times more effective.
A search has been performed for the semileptonic decays D0→K0SK−e+νe, D+→K0SK0Se+νe and D+→K+K−e+νe, using 7.9 fb−1 of e+e− annihilation data collected at the center-of-mass energy s√=3.773 GeV by the BESIII detector operating at the BEPCII collider. No significant signals are observed, and upper limits are set at the 90\% confidence level of 2.13×10−5, 1.54×10−5 and 2.10×10−5 for the branching fractions of D0→K0SK−e+νe, D+→K0SK0Se+νe and D+→K+K−e+νe, respectively.
Using 9.0 fb−1 of e+e− collision data collected at center-of-mass energies from 4.178 to 4.278 GeV with the BESIII detector at the BEPCII collider, we perform the first search for the radiative transition χc1(3872)→γψ2(3823). No χc1(3872)→γψ2(3823) signal is observed. The upper limit on the ratio of branching fractions B(χc1(3872)→γψ2(3823),ψ2(3823)→γχc1)/B(χc1(3872)→π+π−J/ψ) is set as 0.075 at the 90\% confidence level. Our result contradicts theoretical predictions under the assumption that the χc1(3872) is the pure charmonium state χc1(2P).
We search for the di-photon decay of a light pseudoscalar axion-like particle, a, in radiative J/ψ decays, using 10 billion J/ψ events collected with the BESIII detector. We find no evidence of a signal and set upper limits at the 95% confidence level on the product branching fraction B(J/ψ→γa)×B(a→γγ) and the axion-like particle photon coupling constant gaγγ in the ranges of (3.7−48.5)×10−8 and (2.2−101.8)×10−4 GeV−1, respectively, for 0.18≤ma≤2.85 GeV/c2. These are the most stringent limits to date in this mass region.
We search for the di-photon decay of a light pseudoscalar axion-like particle, a, in radiative J/ψ decays, using 10 billion J/ψ events collected with the BESIII detector. We find no evidence of a signal and set upper limits at the 95% confidence level on the product branching fraction B(J/ψ→γa)×B(a→γγ) and the axion-like particle photon coupling constant gaγγ in the ranges of (3.7−48.5)×10−8 and (2.2−101.8)×10−4 GeV−1, respectively, for 0.18≤ma≤2.85 GeV/c2. These are the most stringent limits to date in this mass region.
We search for the di-photon decay of a light pseudoscalar axion-like particle, a, in radiative decays of the J/ψ, using 10 billion J/ψ events collected with the BESIII detector. We find no evidence of a narrow resonance and set upper limits at the 95% confidence level on the product branching fraction B(J/ψ→γa)×B(a→γγ) and the axion-like particle photon coupling constant gaγγ in the ranges of (3.6−49.8)×10−8 and (2.2−103.8)×10−4 GeV−1, respectively, for 0.18≤ma≤2.85 GeV/c2. These are the most stringent limits to date in this mass region.