Symmetric periodic orbits near heteroclinic loops at infinity for a class of polynomial vector fields

For polynomial vector fields in R3, in general, it is very difficult to detect the existence of an open set of periodic orbits in their phase portraits. Here, we characterize a class of polynomial vector fields of arbitrary even degree having an open set of periodic orbits. The main two tools for proving this result are, first, the existence in the phase portrait of a symmetry with respect to a plane and, second, the existence of two symmetric heteroclinic loops.

Les R-loops et leurs conséquences sur l'expression génique chez Escherichia coli.

Des variations importantes du surenroulement de l’ADN peuvent être générées durant la phase d’élongation de la transcription selon le modèle du « twin supercoiled domain ». Selon ce modèle, le déplacement du complexe de transcription génère du surenroulement positif à l’avant, et du surenroulement négatif à l’arrière de l’ARN polymérase. Le rôle essentiel de la topoisomérase I chez Escherichia coli est de prévenir l’accumulation de ce surenroulement négatif générée durant la transcription. En absence de topoisomérase I, l’accumulation de ce surenroulement négatif favorise la formation de R-loops qui ont pour conséquence d’inhiber la croissance bactérienne. Les R-loops sont des hybrides ARN-ADN qui se forment entre l’ARN nouvellement synthétisé et le simple brin d’ADN complémentaire. Dans les cellules déficientes en topoisomérase I, des mutations compensatoires s’accumulent dans les gènes qui codent pour la gyrase, réduisant le niveau de surenroulement négatif du chromosome et favorisant la croissance. Une des ces mutations est une gyrase thermosensible qui s’exprime à 37 °C. La RNase HI, une enzyme qui dégrade la partie ARN d’un R-loop, peut aussi restaurer la croissance en absence de topoisomérase I lorsqu’elle est produite en très grande quantité par rapport à sa concentration physiologique. En présence de topoisomérase I, des R-loops peuvent aussi se former lorsque la RNase HI est inactive. Dans ces souches mutantes, les R-loops induisent la réponse SOS et la réplication constitutive de l’ADN (cSDR). Dans notre étude, nous montrons comment les R-loops formés en absence de topoisomérase I ou RNase HI peuvent affecter négativement la croissance des cellules. Lorsque la topoisomérase I est inactivée, l’accumulation d’hypersurenroulement négatif conduit à la formation de nombreux R-loops, ce qui déclenche la dégradation de l’ARN synthétisé. Issus de la dégradation de l’ARNm de pleine longueur, des ARNm incomplets et traductibles s’accumulent et causent l’inhibition de la synthèse protéique et de la croissance. Le processus par lequel l’ARN est dégradé n’est pas encore complètement élucidé, mais nos résultats soutiennent fortement que la RNase HI présente en concentration physiologique est responsable de ce phénotype. Chose importante, la RNase E qui est l’endoribonuclease majeure de la cellule n’est pas impliquée dans ce processus, et la dégradation de l’ARN survient avant son action. Nous montrons aussi qu’une corrélation parfaite existe entre la concentration de RNase HI, l’accumulation d’hypersurenroulement négatif et l’inhibition de la croissance bactérienne. Lorsque la RNase HI est en excès, l’accumulation de surenroulement négatif est inhibée et la croissance n’est pas affectée. L’inverse se produit Lorsque la RNase HI est en concentration physiologique. En limitant l’accumulation d’hypersurenroulement négatif, la surproduction de la RNase HI prévient alors la dégradation de l’ARN et permet la croissance. Quand la RNase HI est inactivée en présence de topoisomérase I, les R-loops réduisent le niveau d’expression de nombreux gènes, incluant des gènes de résistance aux stress comme rpoH et grpE. Cette inhibition de l’expression génique n’est pas accompagnée de la dégradation de l’ARN contrairement à ce qui se produit en absence de topoisomérase I. Dans le mutant déficient en RNase HI, la diminution de l’expression génique réduit la concentration cellulaire de différentes protéines, ce qui altère négativement le taux de croissance et affecte dramatiquement la survie des cellules exposées aux stress de hautes températures et oxydatifs. Une inactivation de RecA, le facteur essentiel qui déclenche la réponse SOS et le cSDR, ne restaure pas l’expression génique. Ceci démontre que la réponse SOS et le cSDR ne sont pas impliqués dans l’inhibition de l’expression génique en absence de RNase HI. La croissance bactérienne qui est inhibée en absence de topoisomérase I, reprend lorsque l’excès de surenroulement négatif est éliminé. En absence de RNase HI et de topoisomérase I, le surenroulement négatif est très relaxé. Il semble que la réponse cellulaire suite à la formation de R-loops, soit la relaxation du surenroulement négatif. Selon le même principe, des mutations compensatoires dans la gyrase apparaissent en absence de topoisomérase I et réduisent l’accumulation de surenroulement négatif. Ceci supporte fortement l’idée que le surenroulement négatif joue un rôle primordial dans la formation de R-loop. La régulation du surenroulement négatif de l’ADN est donc une tâche essentielle pour la cellule. Elle favorise notamment l’expression génique optimale durant la croissance et l’exposition aux stress, en limitant la formation de R-loops. La topoisomérase I et la RNase HI jouent un rôle important et complémentaire dans ce processus.

Interaction entre la RNase HI et la RNase E dans le métabolisme des R-loops et la dégradation des ARNms chez Escherichia coli.

Chez la bactérie Escherichia coli, la topoisomérase I et la gyrase représentent deux topoisomérases majeures qui participent à la régulation du surenroulement de l’ADN. Celles-ci sont codées respectivement par les gènes topA et par gyrA et gyrB. Chez les mutants topA, l’excès de surenroulement négatif qui est généré en amont de la polymérase ARN lors de la phase d’élongation de la transcription de l’ADN, entraine la formation de R-loops. Les R-loops sont des hybrides ARN-ADN qui in vivo sont formés lorsque l’ARN nouvellement transcrit forme un hybride avec le brin d’ADN matrice, le brin d’ADN complémentaire demeurant sous forme simple brin. La RNase HI est une endoribonucléase codée par le gène rnhA. Elle dégrade l’ARN de R-loops, entre autres, pour empêcher l’initiation de la réplication à des sites autres que l’origine normale, oriC. Chez les mutants rnhA, on observe une réplication indépendante de l’origine oriC. Ce type de réplication appelé cSDR, pourrait donc expliquer, du moins en partie, l’inhibition de la croissance de doubles mutants topA rnhA. A l’aide de la mutagenèse au transposon Tn5, il a été possible d’isoler des suppresseurs extragéniques qui permettaient la croissance des doubles mutants topA rnhA. Plusieurs de ces suppresseurs ont le transposon inséré dans le gène codant pour la RNase E, l’endoribonucléase principale impliquée dans la dégradation des ARNms chez E. coli. La majorité des insertions se retrouvent dans la partie C-terminale de la protéine qui est impliquée dans l’assemblage d’un complexe multiprotéique appelé l’ARN dégradosome. Les résultats obtenus démontrent que ces suppresseurs diminuent le cSDR ainsi que la réponse SOS induite constitutivement en l’absence de la RNase HI. Sachant que la RNase HI est une endoribonucléase tout comme la RNase E, une collaboration entre les deux enzymes suggère que la RNase E pourrait également jouer un rôle potentiel dans le contrôle de la formation des R-loops et bien évidemment de leur retrait au sein de la cellule. À l’opposé, il est possible que la RNase HI puisse avoir comme autre fonction la prise en charge de la maturation et de la dégradation des molécules d’ARNs.

Hysteresis in a system driven by either generalized force or displacement variables: martensitic phase transition in single-crystalline Cu-Zn-Al

We report on experiments aimed at comparing the hysteretic response of a Cu-Zn-Al single crystal undergoing a martensitic transition under strain-driven and stress-driven conditions. Strain-driven experiments were performed using a conventional tensile machine while a special device was designed to perform stress-driven experiments. Significant differences in the hysteresis loops were found. The strain-driven curves show reentrant behavior yield point which is not observed in the stress-driven case. The dissipated energy in the stress-driven curves is larger than in the strain-driven ones. Results from recently proposed models qualitatively agree with experiments.

Effect of annealing atmosphere on phase formation and electrical characteristics of bismuth ferrite thin films

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Effect of processing route on the phase formation and properties of Bi4Ti3O12 ceramics

Our efforts were directed to the preparation of bismuth titanate-Bi4Ti3O12 (BIT) by two procedures: mechanically assisted synthesis and polymeric precursor method to display a variety of their advantages. To follow the nucleation and phase formation of BIT, XRD and Rietveld refinement analysis were used and it was shown that Bi4Ti3O12 ceramic can been successfully prepared from nano-sized powders obtained by both methods. The ferroelectric properties were determined and the loops from BIT obtained by polymeric precursor method were not fully saturated with a remnant polarization of 20 mu C/cm(2) and coercitive field of 1500 kV/cm. BIT obtained from powders prepared by mechanically assisted synthesis shows a remnant polarization of 0.65 mu C/cm(2) and coercitive field of 1050 kV/cm. The grain morphology may be the factor causing the observed differences. (C) 2005 Published by Elsevier Ltd and Techna Group S.r.l.

Robust control applied to power flow control in single-phase inverter with LCL filter, using droop control and D-stability

This paper proposes a new methodology to control the power flow between a distributed generator (DG) and the electrical power distribution grid. It is used the droop voltage control to manage the active and reactive power. Through this control a sinusoidal voltage reference is generated to be tracked by voltage loop and this loop generates the current reference for the current loop. The proposed control introduces feed-forward states improving the control performance in order to obtain high quality for the current injected to the grid. The controllers were obtained through the linear matrix inequalities (LMI) using the D-stability analysis to allocate the closed-loop controller poles. Therefore, the results show quick transient response with low oscillations. Thus, this paper presents the proposed control technique, the main simulation results and a prototype with 1000VA was developed in the laboratory in order to demonstrate the feasibility of the proposed control. © 2012 IEEE.

Physical properties of self-polarized PZT thin films at compositions around the morphotropic phase boundary

The physical properties of self-polarized PbZr1-xTixO3 thin films with no preferential orientation in a range of compositions 0.46 <= x <= 0.50 were investigated. Structural analysis revealed the coexistence of monoclinic-tetragonal and monoclinic-rhombohedral phases at compositions 0.46 <= x <= 0.49, where the monoclinic phase was in the majority and both the tetragonal and the rhombohedral phases in the minority. The dielectric permittivity (epsilon'= 447) reached its maximum at around composition x = 0.48. Asymmetries in the macroscopic and local hysteresis loops confirmed the existence of the self-polarization effect in the studied films.

Dynamic symmetry loss of high-frequency hysteresis loops in single-domain particles with uniaxial anisotropy

Understanding how magnetic materials respond to rapidly varying magnetic fields, as in dynamic hysteresis loops, constitutes a complex and physically interesting problem. But in order to accomplish a thorough investigation, one must necessarily consider the effects of thermal fluctuations. Albeit being present in all real systems, these are seldom included in numerical studies. The notable exceptions are the Ising systems, which have been extensively studied in the past, but describe only one of the many mechanisms of magnetization reversal known to occur. In this paper we employ the Stochastic Landau-Lifshitz formalism to study high-frequency hysteresis loops of single-domain particles with uniaxial anisotropy at an arbitrary temperature. We show that in certain conditions the magnetic response may become predominantly out-of-phase and the loops may undergo a dynamic symmetry loss. This is found to be a direct consequence of the competing responses due to the thermal fluctuations and the gyroscopic motion of the magnetization. We have also found the magnetic behavior to be exceedingly sensitive to temperature variations, not only within the superparamagnetic-ferromagnetic transition range usually considered, but specially at even lower temperatures, where the bulk of interesting phenomena is seen to take place. (C) 2011 Elsevier B.V. All rights reserved.

Magnetic color-flavor-locked stars

Using the solutions of the gap equations of the magnetic-color-flavor-locked (MCFL) phase of paired quark matter in a magnetic field, and taking into consideration the separation between the longitudinal and transverse pressures due to the field-induced breaking of the spatial rotational symmetry, the equation of state (EoS) of the MCFL phase is self-consistently determined. Implications for stellar models of magnetized (self-bound) strange stars and hybrid (MCFL core) stars are discussed.

A reduced model clarifies the role of feedback loops and time delays in the Drosophila circadian oscillator.

Although several detailed models of molecular processes essential for circadian oscillations have been developed, their complexity makes intuitive understanding of the oscillation mechanism difficult. The goal of the present study was to reduce a previously developed, detailed model to a minimal representation of the transcriptional regulation essential for circadian rhythmicity in Drosophila. The reduced model contains only two differential equations, each with time delays. A negative feedback loop is included, in which PER protein represses per transcription by binding the dCLOCK transcription factor. A positive feedback loop is also included, in which dCLOCK indirectly enhances its own formation. The model simulated circadian oscillations, light entrainment, and a phase-response curve with qualitative similarities to experiment. Time delays were found to be essential for simulation of circadian oscillations with this model. To examine the robustness of the simplified model to fluctuations in molecule numbers, a stochastic variant was constructed. Robust circadian oscillations and entrainment to light pulses were simulated with fewer than 80 molecules of each gene product present on average. Circadian oscillations persisted when the positive feedback loop was removed. Moreover, elimination of positive feedback did not decrease the robustness of oscillations to stochastic fluctuations or to variations in parameter values. Such reduced models can aid understanding of the oscillation mechanisms in Drosophila and in other organisms in which feedback regulation of transcription may play an important role.

Analysis of Pressure Head-Flow Loops of Pulsatile Rotodynamic Blood Pumps

The clinical importance of pulsatility is a recurring topic of debate in mechanical circulatory support. Lack of pulsatility has been identified as a possible factor responsible for adverse events and has also demonstrated a role in myocardial perfusion and cardiac recovery. A commonly used method for restoring pulsatility with rotodynamic blood pumps (RBPs) is to modulate the speed profile, synchronized to the cardiac cycle. This introduces additional parameters that influence the (un)loading of the heart, including the timing (phase shift) between the native cardiac cycle and the pump pulses, and the amplitude of speed modulation. In this study, the impact of these parameters upon the heart-RBP interaction was examined in terms of the pressure head-flow (HQ) diagram. The measurements were conducted using a rotodynamic Deltastream DP2 pump in a validated hybrid mock circulation with baroreflex function. The pump was operated with a sinusoidal speed profile, synchronized to the native cardiac cycle. The simulated ventriculo-aortic cannulation showed that the level of (un)loading and the shape of the HQ loops strongly depend on the phase shift. The HQ loops displayed characteristic shapes depending on the phase shift. Increased contribution of native contraction (increased ventricular stroke work [WS ]) resulted in a broadening of the loops. It was found that the previously described linear relationship between WS and the area of the HQ loop for constant pump speeds becomes a family of linear relationships, whose slope depends on the phase shift.

High-resolution in situ oxygen microprofiles, porewater and solid phase geochemistry from the Crimean shelf (Black Sea) from Maria S. Merian cruise MSM15/1

The outer western Crimean shelf of the Black Sea is a natural laboratory to investigate effects of stable oxic versus varying hypoxic conditions on seafloor biogeochemical processes and benthic community structure. Bottom-water oxygen concentrations ranged from normoxic (175 µmol O2/L) and hypoxic (< 63 µmol O2/L) or even anoxic/sulfidic conditions within a few kilometers' distance. Variations in oxygen concentrations between 160 and 10 µmol/L even occurred within hours close to the chemocline at 134 m water depth. Total oxygen uptake, including diffusive as well as fauna-mediated oxygen consumption, decreased from 15 mmol/m**2/d on average in the oxic zone, to 7 mmol/m**2/d on average in the hypoxic zone, correlating with changes in macrobenthos composition. Benthic diffusive oxygen uptake rates, comprising respiration of microorganisms and small meiofauna, were similar in oxic and hypoxic zones (on average 4.5 mmol/m**2/d), but declined to 1.3 mmol/m**2/d in bottom waters with oxygen concentrations below 20 µmol/L. Measurements and modeling of porewater profiles indicated that reoxidation of reduced compounds played only a minor role in diffusive oxygen uptake under the different oxygen conditions, leaving the major fraction to aerobic degradation of organic carbon. Remineralization efficiency decreased from nearly 100 % in the oxic zone, to 50 % in the oxic-hypoxic zone, to 10 % in the hypoxic-anoxic zone. Overall, the faunal remineralization rate was more important, but also more influenced by fluctuating oxygen concentrations, than microbial and geochemical oxidation processes.