928 resultados para Charge ratio
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The magnetized MINOS Near Detector, at a depth of 225 mwe, is used to measure the atmospheric muon charge ratio. The ratio of observed positive to negative atmospheric muon rates, using 301 days of data, is measured to be 1.266 +/- 0.001(stat)(-0.014)(+0.015)(syst). This measurement is consistent with previous results from other shallow underground detectors and is 0.108 +/- 0.019(stat + syst) lower than the measurement at the functionally identical MINOS Far Detector at a depth of 2070 mwe. This increase in charge ratio as a function of depth is consistent with an increase in the fraction of muons arising from kaon decay for increasing muon surface energies.
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We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN LHC. Muons were detected in the momentum range from 5 GeV/. c to 1 TeV/. c. The surface flux ratio is measured to be 1.2766±0.0032(stat.)±0.0032(syst.), independent of the muon momentum, below 100 GeV/. c. This is the most precise measurement to date. At higher momenta the data are consistent with an increase of the charge ratio, in agreement with cosmic ray shower models and compatible with previous measurements by deep-underground experiments. © 2010.
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The atmospheric muon charge ratio, defined as the number of positive over negative charged muons, is an interesting quantity for the study of high energy hadronic interactions in atmosphere and the nature of the primary cosmic rays. The measurement of the charge ratio in the TeV muon energy range allows to study the hadronic interactions in kinematic regions not yet explored at accelerators. The OPERA experiment is a hybrid electronic detector/emulsion apparatus, located in the underground Gran Sasso Laboratory, at an average depth of 3800 meters water equivalent (m.w.e.). OPERA is the first large magnetized detector that can measure the muon charge ratio at the LNGS depth, with a wide acceptance for cosmic ray muons coming from above. In this thesis, the muon charge ratio is measured using the spectrometers of the OPERA detector in the highest energy region. The charge ratio was computed separately for single and for multiple muon events, in order to select different primary cosmic ray samples in energy and composition. The measurement as a function of the surface muon energy is used to infer parameters characterizing the particle production in atmosphere, that will be used to constrain Monte Carlo predictions. Finally, the experimental results are interpreted in terms of cosmic ray and particle physics models.
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The OPERA detector, designed to search for νμ → ντ oscillations in the CNGS beam, is located in the underground Gran Sasso laboratory, a privileged location to study TeV-scale cosmic rays. For the analysis here presented, the detector was used to measure the atmospheric muon charge ratio in the TeV region. OPERA collected chargeseparated cosmic ray data between 2008 and 2012. More than 3 million atmospheric muon events were detected and reconstructed, among which about 110000 multiple muon bundles. The charge ratio Rμ ≡ Nμ+/Nμ− was measured separately for single and for multiple muon events. The analysis exploited the inversion of the magnet polarity which was performed on purpose during the 2012 Run. The combination of the two data sets with opposite magnet polarities allowedminimizing systematic uncertainties and reaching an accurate determination of the muon charge ratio. Data were fitted to obtain relevant parameters on the composition of primary cosmic rays and the associated kaon production in the forward fragmentation region. In the surface energy range 1–20 TeV investigated by OPERA, Rμ is well described by a parametric model including only pion and kaon contributions to themuon flux, showing no significant contribution of the prompt component. The energy independence supports the validity of Feynman scaling in the fragmentation region up to 200 TeV/nucleon primary energy.
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Complexes of polyelectrolytes with defined charge distance and different dendrimer counterions Magdalena Chelmecka Max Planck Institute for Polymer Research; Ackermannweg 10; D-55128 Mainz ; Tel.: (+49) 06131- 379 – 226 A study of complexes in solution is of interest to investigate whether the formation of well-defined assemblies like in classical surfactant systems is possible. Aim of this thesis is to investigate the electrostatic self-assembly of linear polycations of varying charge distance with “large” counterions of varying architecture. We especially investigate the morphology of objects formed, but also their stability under salt free condition and after low molecular mass salt addition. As polycations, Poly(dialkylimino)-alkylene salts (Ionenes) I65MeBr and I25MeBr were chosen. Ionenes are synthesized via Menschutkin reaction and characterized by standard methods. Counterions are Polyamidoamine (PAMAM) dendrimers of generations G2.5, G5.5, G7.5 with -COONa surface groups and shape-persistent, Polyphenylene dendrimers of generation G1 with surface -COOH groups. A complex interplay of interactions is expected to direct the self assembly via electrostatic interaction, geometric factors, hydrophobic interaction or hydrogen bonds. Methods used for the investigation of complexes are: UV-spectroscopy, pH-metric techniques, dynamic and static light scattering, small angle neutron scattering, potential measurements and potentiometric titration. Under certain conditions, (i.e. charge ratio of compounds, charge density of ionene and dendrimer also concentration of sample) polyelectrolyte systems composed of ionenes and dendrimers build complexes in solution. System compounds are typical polyelectrolytes, but structures which they build behave not usual for typical polyelectrolytes. In a one diffusion mode regime aggregates of about 100 nm hydrodynamic radius have been found. Such aggregates are core-shell or anisotropic core shell structures in the case of ionenes/PAMAM dendrimers complexes. These complexes are stable even at high ionic strength. In case of ionenes with poly(phenylene) dendrimers, hard sphere-like objects or spherical objects with hairy-like surface have been found in a one diffusion mode regime. Their stability at high ionic strength is lower. For the ionenes/poly(phenylene) dendrimers systems one transition point has been found from one to two diffusion processes, towards increasing ionene concentration, i.e. for the samples with fixed dendrimer concentration towards increasing ionic strength. For the diffusion profile of ionene/PAMAM dendrimers in most cases two transition regimes are observed. One at very low ionene concentration, the second one at high ionene concentrations, which again means for the samples with fixed dendrimer concentration, also at higher ionic strength. Both two mode regimes are separated by the one mode regime. As was confirmed experimentally, the one diffusion mode regime is caused by the motion of well defined assemblies. The two diffusion mode regimes are caused by the movement of different sized species in solution, large aggregates and middle-size aggregates (oligoaggregates). The location and also the number of transition points in the diffusion profiles is dependent on the ionene to dendrimer charge ratio, charge density of the compounds and concentration. No influence of the molecular mass of the ionene has been found. The aggregates are found to be charged on the surface, however this surface charge does not significantly influence the diffusion properties of the system.
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A method was developed to extract adenine nucleotides AMP, ADP, and ATP from marine macroalgal tissue to gain information on the cellular energy charge. Quantification was carried out by high performance liquid chromatography (HPLC). Three species from the rocky shore of the island of Helgoland (German Bight) were examined: Laminaria saccharina (Phaeophyta), Chondrus crispus (Rhodophyta), and Ulva lactuca (Chlorophyta). In L. saccharina and C. crispus, the adenylate energy charge (AEC) was determined in different thallus regions. AEC varied in relation to tissue age and function. Higher AEC values typically occurred in thallus regions with meristematic activity. Furthermore, L. saccharina and U. lactuca were exposed to UV-A and elevated UV-B radiation. The AEC was calculated and the maximal quantum yield of photosystem II (Fv/Fm) was determined as indicators for UV stress. In both species, the AEC remained at high values (0.72 ± 0.04), while Fv/Fm dropped rapidly. The results show that the photosynthesis of the phaeophyte is more resistant to UV radiation than the chlorophyte.
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Summary This study aimed to evaluate the impact of vitrification on membrane lipid profile obtained by mass spectrometry (MS) of in vitro-produced bovine embryos. Matrix-assisted laser desorption ionization-mass spectrometry (MALDI-MS) has been used to obtain individual embryo membrane lipid profiles. Due to conditions of analysis, mainly membrane lipids, most favorably phosphatidylcholines (PCs) and sphingomyelins (SMs) have been detected. The following ions described by their mass-to-charge ratio (m/z) and respective attribution presented increased relative abundance (1.2-20×) in the vitrified group: 703.5 [SM (16:0) + H]+; 722.5 [PC (40:3) + Na]+; 758.5 [PC (34:2) + H]+; 762.5 [PC (34:0) + H]+; 790.5 [PC (36:0) + H]+ and 810.5 [PC (38:4) + H]+ and/or [PC (36:1) + Na]+. The ion with a m/z 744.5 [PCp (34:1) and/or PCe (34:2)] was 3.4-fold more abundant in the fresh group. Interestingly, ions with m/z 722.5 or 744.5 indicate the presence of lipid species, which are more resistant to enzymatic degradation as they contain fatty acyl residues linked through ether type bonds (alkyl ether or plasmalogens, indicated by the lowercase 'e' and 'p', respectively) to the glycerol structure. The results indicate that cryopreservation impacts the membrane lipid profile, and that these alterations can be properly monitored by MALDI-MS. Membrane lipids can therefore be evaluated by MALDI-MS to monitor the effect of cryopreservation on membrane lipids, and to investigate changes in lipid profile that may reflect the metabolic response to the cryopreservation stress or changes in the environmental conditions.
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Chemical reactivity, photolability, and computational studies of the ruthenium nitrosyl complex with a substituted cyclam, fac-[Ru(NO)Cl(2)(kappa(3)N(4),N(8),N(11)(1-carboxypropyl)cyclam)]Cl center dot H(2)O ((1-carboxypropyl) cyclam = 3-(1,4,8,11-tetraazacyclotetradecan-1-yl) propionic acid)), (I) are described. Chloride ligands do not undergo aquation reactions (at 25 degrees C, pH 3). The rate of nitric oxide (NO) dissociation (k(obs-NO)) upon reduction of I is 2.8 s(-1) at 25 +/- 1 degrees C (in 0.5 mol L(-1) HCl), which is close to the highest value found for related complexes. The uncoordinated carboxyl of I has a pK(a) of similar to 3.3, which is close to that of the carboxyl of the non coordinated (1-carboxypropyl) cyclam (pK(a) = 3.4). Two additional pK(a) values were found for I at similar to 8.0 and similar to 11.5. Upon electrochemical reduction or under irradiation with light (lambda(irr) = 350 or 520 nm; pH 7.4), I releases NO in aqueous solution. The cyclam ring N bound to the carboxypropyl group is not coordinated, resulting in a fac configuration that affects the properties and chemical reactivities of I, especially as NO donor, compared with analogous trans complexes. Among the computational models tested, the B3LYP/ECP28MDF, cc-pVDZ resulted in smaller errors for the geometry of I. The computational data helped clarify the experimental acid-base equilibria and indicated the most favourable site for the second deprotonation, which follows that of the carboxyl group. Furthermore, it showed that by changing the pH it is possible to modulate the electron density of I with deprotonation. The calculated NO bond length and the Ru/NO charge ratio indicated that the predominant canonical structure is [Ru(III)NO], but the Ru-NO bond angles and bond index (b.i.) values were less clear; the angles suggested that [Ru(II)NO(+)] could contribute to the electronic structure of I and b.i. values indicated a contribution from [Ru(IV)NO(-)]. Considering that some experimental data are consistent with a [Ru(II)NO(+)] description, while others are in agreement with [Ru(III)NO], the best description for I would be a linear combination of the three canonical forms, with a higher weight for [Ru(II)NO(+)] and [Ru(III)NO].
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The interactions between phosphorylcholine-substituted chitosans (PC-CH) and calf-thymus DNA (ct-DNA) were investigated focusing on the effects of the charge ratio, the pH, and phosphorylcholine content on the size and stability of the complexes using the ethidium bromide fluorescence assay, gel electrophoresis, dynamic light scattering. and fluorescence microscopy. The size and colloidal stability of deacetylated chitosan (CH/DNA) and PC-CH/DNA complexes were strongly dependent on phosphorylcholine content, charge ratios, and pH. The interaction strengths were evaluated from ethidium bromide fluorescence, and at N/P ratios higher than 5.0, no DNA release was observed in any synthesized PC-CH/DNA polyplexes by gel electrophoresis. The PC-CH/DNA polyplexes exhibited a higher resistance to aggregation compared to deacetylated chitosan (CH) at neutral pH. At low pH values highly charged chitosan and its phosphorylcholine derivatives had strong binding affinity with DNA, whereas at higher pH Values CH formed large aggregates and only C-CH derivatives were able to form small nanoparticles with hydrodynamic radii varying from 100 to 150 nm. Nanoparticles synthesized at low ionic strength with PC-CH derivatives containing moderate degrees of substitution (DS = 20% and 40%) remained stable for weeks. Photomicroscopies also confirmed that rhodamine-labeled PC(40)CH derivative nanoparticles presented higher colloidal stability than those synthesized using deacetylated chitosan. Accordingly, due to their improved physicochemical properties these phosphorylcholine-modified chitosans provide new perspectives for controlling the properties of polyplexes. (C) 2009 Elsevier Inc. All rights reserved.
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The kinetics of mechanical alloying have been investigated by examining the effect that ball mass has on the rate at which titanium carbide forms from the elements. By varying the ball density while keeping the ball diameter and the charge ratio constant, the collision energy was independently controlled. Grinding media with a density from 3.8 g cm(-3) (agate) to 16.4 g cm(-3) (tungsten carbide) were used. The reaction rate increases exponentially with ball mass until a critical level is reached, which is determined by the induced temperature rise. Above this level, collisions of higher energy have no advantage. It is also shown that the reaction rate increases exponentially with the rate at which strain accumulates in the reactants. It is suggested that the strain accumulation rate in mechanically induced reactions is analogous to temperature in thermally induced chemical reactions.
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RESUME :Introduction. Les maladies cardiovasculaires représentent la première cause de mortalité dans les pays développés et l'insuffisance cardiaque (IC) est la plus fréquente. Suite à un infarctus, le coeur des patients subit un remodelage ventriculaire pouvant évoluer vers un état d'IC. L'IC se définit comme un état dans lequel le coeur n'est plus capable d'approvisionner suffisamment les organes et cet état s'accompagne souvent de troubles du rythme cardiaque. Le remodelage ventriculaire touche de nombreux gènes codant à la fois pour les voies métaboliques et pour des canaux ioniques favorisant ainsi l'apparition des arythmies responsables de la mort subite des patients atteints d'IC. Comprendre ce passage entre remodelage et IC est crucial afin de pouvoir un jour prévenir l'IC et les complications médicales qui l'accompagnent. Nous nous sommes intéressés aux canaux potassiques dépendants de l'ATP (KATP) car ces canaux ont la capacité de coupler le métabolisme de la cellule à son activité électrique. En effet, les canaux KATP s'ouvrent quand la charge énergétique (rapport ATP/ ADP) de la cellule chute. Dans les cardiomyocytes, l'ouverture des KATP induit une hyperpolarisation de la membrane cellulaire ce qui diminue indirectement la surcharge calcique et de ce fait préserve la cellule. Les canaux KATp sont formés de 4 sous-unités Kir6.x (Kir6.1 ou Kir6.2) formant le pore du canal associées à 4 sous-unités régulatrices SUR. Les propriétés électrophysiologiques ainsi que la sensibilité pharmacologique des canaux KATP dépendent de leur composition et seuls les canaux KATP formés par la sous-unité Kirô.l sont activés par le diazoxyde.Méthodes et résultats. Nous avons d'abord montré dans un modèle in vivo d'IC chez le rat adulte que les sous-unités Kir6.1 et SUR sont surexprimées dans ces conditions pathologiques. Par ailleurs, les cardiomyocytes issus des coeurs infarcis deviennent sensibles au diazoxyde reflétant la surexpression de Kir6.1. Les potentiels d'action qui sont prolongés dans l'IC et qui sont à l'origine d'arythmies majeures sont normalisés par l'ouverture des canaux KATp induite par le diazoxyde. Ainsi, l'ouverture pharmacologique des canaux KATp contribuerait à la cardio-protection. Dans une seconde partie, nous avons déterminé quels étaient les facteurs de transcription responsables de ce changement d'expression des sous-unités formant les KATP. Dans notre modèle, nous avons pu montrer que la surexpression de Kirô.l est due aux facteurs de transcription Fox03 et FoxF2 qui est aussi responsable de la surexpression des sous-unités SUR. Dans la dernière partie de ce travail, nous avons mis au point un modèle d'IC in vitro en cultivant les cardiomyocytes de rats adultes en présence d'angiotensine II (Angll) ou de TNFa. Ce modèle expérimental nous a non seulement permis de mettre en relation l'importance de L'AnglI et du TNFa sur le remodelage des canaux KATP mais aussi de développer un modèle in vitro présentant les mêmes caractéristiques que le modèle in vivo concernant le remodelage des KATP lors de l'IC. Ce dernier modèle expérimental ouvre des perspectives afin de mieux caractériser les voies de signalisation impliquées dans le remodelage des canaux KATp lors de l'IC.Conclusion. Les canaux KATp subissent un remodelage lors de l'IC et les résultats obtenus montrent le potentiel cardio-protecteur de ces canaux.ABSTRACT :Background and aim. Cardiovascular disease is the leading cause of death in developed countries and heart failure (HF) is the most common. Following myocardial infarction, the heart of the patient undergoes ventricular remodeling which may evolve toward a state of HF. HF is defined as a state in which heart is unable to supply enough blood to organs and this state is often accompanied by cardiac arrhythmias. Ventricular remodeling involves many genes coding for both metabolic enzymes and ion channels. Changes in ion channel expression can promote arrhythmias responsible for sudden death in patients with HF. A better understanding of the transition between remodeling and HF is crucial in order to prevent the complications associated to HF We were interested in ATP-dependent potassium channels (KATp) because they couple cell metabolism to electrical activity of the cell. Indeed, KATP channels open when the energy charge (ratio of ATP / ADP) of the cell collapses. In cardiomyocytes, the opening of KATP channels induces hyper- polanzation of the cell membrane which reduces calcium overload and thereby protects the cell. KATp channels are composed by 4 Kir6.x subumts (Kir6.1 or Kir6.2) forming the pore channel associated with 4 regulatory subunits SUR. The electrophysiological properties as well as pharmacological sensitivity of KATp channels depend on their composition and only KATP channels formed by Kir6.1 subunit are activated by diazoxide.Methods and results. Firstly, using an in vivo model of HF in adult rats, we showed that Kir6.1 and SUR subunits are overexpressed in HF. In addition, cardiomyocytes from post-infarction hearts became sensitive to diazoxide reflecting the overexpression of the Kir6.1 subunit. The opening of KATP by diazoxide tended to reduce the action potential duration (APD) which is extended in HF. This increase in APD is known to be a major source of arrhythmias during HF. Therefore, the opening of KATP channels by diazoxide would be cardio-protective. Secondly, we wanted to determine which transcription factors were responsible for this KATP remodeling. In our model of HF, we showed that overexpression of Kir6.1 is due to the transcription factors Fox03 and FOXF2 which is also responsible for SUR subunits overexpression. Thirdly, we developed an in vitro model of HF by cultivation of adult rat cardiomyocytes in the presence of angiotensin II (Angll) or TNFa. This model is very interesting not only because it underlines the importance of Angll and TNFa in KATp remodeling but also because this in vitro model presents the same KATP remodeling as the in vivo model of HF. These findings show that our in vitro model of HF opens up many possibilities to investigate more precisely the signaling pathways involved in remodeling of the KATP channels in HF.Conclusion. KATP channels undergo remodeling during HF and our results show the cardio¬protective potential of KATP channels in this disease.