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The first measurement of ϕ-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy sNN−−−√ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. The ϕ-mesons have been identified in the dimuon decay channel in the transverse momentum (pT) range 1<pT<7 GeV/c, both in the p-going (2.03<y<3.53) and the Pb-going (−4.46<y<−2.96) directions, where y stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for ϕ-meson production is measured for 2.96<|y|<3.53, resulting in a factor ∼0.5 with no significant pT dependence within the uncertainties. The pT dependence of the ϕ nuclear modification factor RpPb exhibits an enhancement up to a factor 1.6 at pT = 3-4 GeV/c in the Pb-going direction. The pT dependence of the ϕ-meson cross section in pp collisions at s√ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for 1<pT<5 GeV/c and 2.5<y<4.
The first study of ϕ-meson production in p-Pb collisions at forward and backward rapidity, at a nucleon-nucleon centre-of-mass energy sNN−−−√=5.02~TeV, has been performed with the ALICE apparatus at the LHC. The ϕ-mesons have been identified in the dimuon decay channel in the transverse momentum (pT) range 1<pT<7 GeV/c, both in the p-going (2.03<y<3.53) and the Pb-going (−4.46<y<−2.96) directions, where y stands for the rapidity in the nucleon-nucleon centre-of-mass, the integrated luminosity amounting to 5.01±0.19~nb−1 and 5.81±0.20~nb−1, respectively, for the two data samples. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward ratio for ϕ-meson production is measured for 2.96<|y|<3.53, resulting in a ratio ∼0.5 with no significant pT dependence within the uncertainties. The pT dependence of the ϕ nuclear modification factor RpPb exhibits an enhancement up to a factor 1.6 at pT = 3-4 GeV/c in the Pb-going direction. The pT dependence of the ϕ-meson cross section in pp collisions at s√ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for 1<pT<5 GeV/c and 2.5<y<4 for a 78±3~nb−1 integrated luminosity sample.
The first study of ϕ-meson production in p-Pb collisions at forward and backward rapidity, at a nucleon-nucleon centre-of-mass energy sNN−−−√=5.02~TeV, has been performed with the ALICE apparatus at the LHC. The ϕ-mesons have been identified in the dimuon decay channel in the transverse momentum (pT) range 1<pT<7 GeV/c, both in the p-going (2.03<y<3.53) and the Pb-going (−4.46<y<−2.96) directions, where y stands for the rapidity in the nucleon-nucleon centre-of-mass, the integrated luminosity amounting to 5.01±0.19~nb−1 and 5.81±0.20~nb−1, respectively, for the two data samples. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward ratio for ϕ-meson production is measured for 2.96<|y|<3.53, resulting in a ratio ∼0.5 with no significant pT dependence within the uncertainties. The pT dependence of the ϕ nuclear modification factor RpPb exhibits an enhancement up to a factor 1.6 at pT = 3-4 GeV/c in the Pb-going direction. The pT dependence of the ϕ-meson cross section in pp collisions at s√ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for 1<pT<5 GeV/c and 2.5<y<4 for a 78±3~nb−1 integrated luminosity sample.
Background: Computed tomography (CT) allows estimation of coronary artery calcium (CAC) progression. We evaluated several progression algorithms in our unselected, population-based cohort for risk prediction of coronary and cardiovascular events.
Methods: In 3281 participants (45–74 years of age), free from cardiovascular disease until the second visit, risk factors, and CTs at baseline (b) and after a mean of 5.1 years (5y) were measured. Hard coronary and cardiovascular events, and total cardiovascular events including revascularization, as well, were recorded during a follow-up time of 7.8±2.2 years after the second CT. The added predictive value of 10 CAC progression algorithms on top of risk factors including baseline CAC was evaluated by using survival analysis, C-statistics, net reclassification improvement, and integrated discrimination index. A subgroup analysis of risk in CAC categories was performed.
Results: We observed 85 (2.6%) hard coronary, 161 (4.9%) hard cardiovascular, and 241 (7.3%) total cardiovascular events. Absolute CAC progression was higher with versus without subsequent coronary events (median, 115 [Q1–Q3, 23–360] versus 8 [0–83], P<0.0001; similar for hard/total cardiovascular events). Some progression algorithms added to the predictive value of baseline CT and risk assessment in terms of C-statistic or integrated discrimination index, especially for total cardiovascular events. However, CAC progression did not improve models including CAC5y and 5-year risk factors. An excellent prognosis was found for 921 participants with double-zero CACb=CAC5y=0 (10-year coronary and hard/total cardiovascular risk: 1.4%, 2.0%, and 2.8%), which was for participants with incident CAC 1.8%, 3.8%, and 6.6%, respectively. When CACb progressed from 1 to 399 to CAC5y≥400, coronary and total cardiovascular risk were nearly 2-fold in comparison with subjects who remained below CAC5y=400. Participants with CACb≥400 had high rates of hard coronary and hard/total cardiovascular events (10-year risk: 12.0%, 13.5%, and 30.9%, respectively).
Conclusions: CAC progression is associated with coronary and cardiovascular event rates, but adds only weakly to risk prediction. What counts is the most recent CAC value and risk factor assessment. Therefore, a repeat scan >5 years after the first scan may be of additional value, except when a double-zero CT scan is present or when the subjects are already at high risk.
Der Mangel von Faktor VIII (FVIII) führt zur häufigsten Gerinnungsstörung, der Hämophilie A. Die rekombinante Expression von FVIII für gentherapeutische Ansätze oder zur Herstellung von FVIII ist zwei bis drei Größenordnungen niedriger verglichen mit anderen Proteinen vergleichbarer Größe. Die Ursachen für die geringe Expression liegen zum großen Teil an der ineffizienten Transkription und dem ineffizientem intrazellulären Transport. (1) Im Rahmen der Untersuchung der FVIII-Sekretion, konnte durch Verwendung von FVIII-GFP Fusionsproteinen zum ersten Mal gezeigt werden, wie FVIII in lebenden Zellen transportiert wird. Außerdem wurde anhand von vergleichenden Immunfluoreszensfärbungen, FVIII-Messungen und Westernblotanalysen demonstriert, dass weder bei der B-Domäne deletierten noch bei der Volllängenvariante signifikante Unterschiede zwischen den GFP-fusionierten und Wildtyp-FVIII-Varianten messbar waren. Offensichtlich wird die Funktionalität von FVIII durch die C-terminal fusionierte GFP-Domäne nicht eingeschränkt. In ersten Lebendzellanalysen konnte gezeigt werden, dass sich FVIII in primären Zellen und Zelllinien hauptsächlich im ER befindet und eine für lumenale ER-Proteine charakteristischen Mobilität aufweist. Beim frühen sekretorischen Transport zeigte sich bei Temperaturblock-Experimenten eine verlängerte Dauer der Akkumulation in ER-Exit-Sites und eine vergleichsweise niedrige Frequenz von ER-Golgi-Bewegungen. Es konnte zum ersten Mal der Nachweis von FVIII-Transport durch vesikuläre tubuläre Cluster erbracht werden. Die Ergebnisse deuten darauf hin, dass der möglicherweise durch Faltungsprobleme blockierte Austritt aus dem ER das Hauptproblem des ineffizienten FVIII-Transports zu sein scheint und weniger der intrazelluläre Transport an sich. Mittels siRNA-Silencing wurde außerdem die überwiegende Beteiligung von COPI am intrazellulären Transport von FVIII deutlich, dessen Herunterregulierung zu einer 78 prozentigen Reduktion der FVIII-Sekretion im Gegensatz zu 32 Prozent bei COPII führte. Dagegen konnte durch Herunterregulierung der Expression der p24-Cargo-Rezeptor Familienmitglieder p24 und p26 und der Clathrin Adapterproteine µ- und -Adaptin bzw. durch physiologischen Knock-out im Falle von ER-Exit-Rezeptor MCFD2 kein Einfluß auf die FVIII-Sekretion festgestellt werden. (2) Als Alternative zu dem ineffizienten FVIII-Expressionsystem in unphysiologischen Zelllinien, bieten primäre Endothelzellen den Vorteil einer hocheffizienten FVIII-Sekretion. Zur Verwendung bei der rekombinanten Produktion benötigt man allerdings eine kontinuierlich wachsende gut charakterisierte Zelllinie. Zur Immortalisierung wurden aus Nabelschnurblut gewonnene Endothelprogenitorzellen mit der aktiven Untereinheit der humanen Telomerase (hTERT) transduziert. Trotz erfolgreicher Transduktion und langfristiger Expression von hTERT, welche im TRAP-Assay normale Aktivität zeigte, gingen die Zellen nach der natürlichen Teilungsspanne in die Seneszenz über. Möglicherweise wird noch ein weiteres Immortalisierungsgen benötigt oder hTERT ist durch die ektopischen Expression in diesen Endothelzellen nicht funktionell. (3) Der Einsatz hämatopoetischer Stammzellen für gentherapeutische Ansätze zur Expression von humanen FVIII ist bislang aufgrund niedriger Expressionseffizienz der Vektoren limitiert. Es wurden daher die Kombinationen verschiedener transkriptioneller und posttranskriptioneller Elemente in FVIII-Expressionsvektoren ausgetestet. Hierbei zeigte sich, dass die Verwendung einer 5’ untranslatierten Region (5’UTR) des hämatopoetisch exprimierten FXIIIA-Gens die FVIII-Sekretion in verschiedenen Zelllinien und primären Zellen deutlich steigerte. Am stärksten war die Wirkung in primären Monozyten, in denen die FVIII-Expression den 6fachen Wert im Vergleich zum Ursprungsvektor ohne 5’UTR erreichte. Leberzellen stellen weitere attraktive Zielzellen für gentherapeutische Ansätze dar, da Sie den primären physiologischen Ort der FVIII-Synthese darstellen. Die häufig für Gentherapievektoren verwendeten ubiquitär exprimierenden viralen Promotoren bewirken zwar hohe Expression in den transduzierten Zellen, haben allerdings den Nachteil durch ektopische Expression vermehrt Immunantworten auszulösen und durch starke Interaktion mit benachbarten Promotoren der Integrationsstelle im Genom möglicherweise tumorgene Effekte zu verursachen. Bei der Untersuchung verschiedener physiologischer Promotoren im Vergleich zum viralen CMV Promotor in Leberzellen konnte mit dem zum ersten mal getesteten minimalen FVIII-Promoter in einem lentiviralen Vektor der dritten Generation in Leberzelllinien eine vergleichsweise hohe Expression von 0,5 IU/ml FVIII /106 Zellen erzielt werden. Der FVIII-Promoter ist daher geeignet für eine lebergerichtete Expression und minimiert dabei das potentielle Risiko der häufig verwendeten ubiquitären viralen Promotoren.
Unmasking a temperature-dependent effect of the P. anserina i-AAA protease on aging and development
(2011)
Different molecular pathways involved in maintaining mitochondrial function are of fundamental importance to control cellular homeostasis. Mitochondrial i-AAA protease is part of such a surveillance system, and PaIAP is the putative ortholog in the fungal aging model Podospora anserina. Here, we investigate the role of PaIAP in aging and development. Deletion of the gene encoding PaIAP resulted in a specific phenotype. When incubated at 27°C, spore germination and fruiting body formation are not different from that of the corresponding wild-type strain. Unexpectedly, the lifespan of the deletion strain is strongly increased. In contrast, cultivation at an elevated temperature of 37°C leads to impairments in spore germination and fruiting body formation and to a reduced lifespan. The higher PaIAP abundance in wild-type strains of the fungus grown at elevated temperature and the phenotype of the deletion strain unmasks a temperature-related role of the protein. The protease appears to be part of a molecular system that has evolved to allow survival under changing temperatures, as they characteristically occur in nature.
The first measurement of two-pion Bose–Einstein correlations in central Pb–Pb collisions at √sNN=2.76 TeV at the Large Hadron Collider is presented. We observe a growing trend with energy now not only for the longitudinal and the outward but also for the sideward pion source radius. The pion homogeneity volume and the decoupling time are significantly larger than those measured at RHIC.
The inclusive charged particle transverse momentum distribution is measured in proton–proton collisions at s=900 GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region (|η|<0.8) over the transverse momentum range 0.15<pT<10 GeV/c. The correlation between transverse momentum and particle multiplicity is also studied. Results are presented for inelastic (INEL) and non-single-diffractive (NSD) events. The average transverse momentum for |η|<0.8 is 〈pT〉INEL=0.483±0.001 (stat.)±0.007 (syst.) GeV/c and 〈pT〉NSD=0.489±0.001 (stat.)±0.007 (syst.) GeV/c, respectively. The data exhibit a slightly larger 〈pT〉 than measurements in wider pseudorapidity intervals. The results are compared to simulations with the Monte Carlo event generators PYTHIA and PHOJET.
The link between atmospheric radicals and newly formed particles at a spruce forest site in Germany
(2013)
It has been claimed for more than a century that atmospheric new particle formation is primarily influenced by the presence of sulphuric acid. However, the activation process of sulphuric acid related clusters into detectable particles is still an unresolved topic. In this study we focus on the PARADE campaign measurements conducted during August/September 2011 at Mt. Kleiner Feldberg in central Germany. During this campaign a set of radicals, organic and inorganic compounds and oxidants and aerosol properties were measured or calculated. We compared a range of organic and inorganic nucleation theories, evaluating their ability to simulate measured particle formation rates at 3 nm in diameter (J3) for a variety of different conditions. Nucleation mechanisms involving only sulphuric acid tentatively captured the observed noon-time daily maximum in J3, but displayed an increasing difference to J3 measurements during the rest of the diurnal cycle. Including large organic radicals, i.e. organic peroxy radicals (RO2) deriving from monoterpenes and their oxidation products in the nucleation mechanism improved the correlation between observed and simulated J3. This supports a recently proposed empirical relationship for new particle formation that has been used in global models. However, the best match between theory and measurements for the site of interest was found for an activation process based on large organic peroxy radicals and stabilized Criegee intermediates (sCI). This novel laboratory derived algorithm simulated the daily pattern and intensity of J3 observed in the ambient data. In this algorithm organic derived radicals are involved in activation and growth and link the formation rate of smallest aerosol particles with OH during daytime and NO3 during nighttime. Because of the RO2s lifetime is controlled by HO2 and NO we conclude that peroxy radicals and NO seem to play an important role for ambient radical chemistry not only with respect to oxidation capacity but also for the activation process of new particle formation. This is supposed to have significant impact of atmospheric radical species on aerosol chemistry and should to be taken into account when studying the impact of new particles in climate feedback cycles.
The link between atmospheric radicals and newly formed particles at a spruce forest site in Germany
(2014)
It has been claimed for more than a century that atmospheric new particle formation is primarily influenced by the presence of sulfuric acid. However, the activation process of sulfuric acid related clusters into detectable particles is still an unresolved topic. In this study we focus on the PARADE campaign measurements conducted during August/September 2011 at Mt Kleiner Feldberg in central Germany. During this campaign a set of radicals, organic and inorganic compounds and oxidants and aerosol properties were measured or calculated. We compared a range of organic and inorganic nucleation theories, evaluating their ability to simulate measured particle formation rates at 3 nm in diameter (J3) for a variety of different conditions. Nucleation mechanisms involving only sulfuric acid tentatively captured the observed noon-time daily maximum in J3, but displayed an increasing difference to J3 measurements during the rest of the diurnal cycle. Including large organic radicals, i.e. organic peroxy radicals (RO2) deriving from monoterpenes and their oxidation products, in the nucleation mechanism improved the correlation between observed and simulated J3. This supports a recently proposed empirical relationship for new particle formation that has been used in global models. However, the best match between theory and measurements for the site of interest was found for an activation process based on large organic peroxy radicals and stabilised Criegee intermediates (sCI). This novel laboratory-derived algorithm simulated the daily pattern and intensity of J3 observed in the ambient data. In this algorithm organic derived radicals are involved in activation and growth and link the formation rate of smallest aerosol particles with OH during daytime and NO3 during night-time. Because the RO2 lifetime is controlled by HO2 and NO we conclude that peroxy radicals and NO seem to play an important role for ambient radical chemistry not only with respect to oxidation capacity but also for the activation process of new particle formation. This is supposed to have significant impact of atmospheric radical species on aerosol chemistry and should be taken into account when studying the impact of new particles in climate feedback cycles.