Study of ammonia borane and its derivatives: Influence of nanoconfinements and pressures

Recently, ammonia borane has increasingly attracted researchers’ attention because of its merging applications, such as organic synthesis, boron nitride compounds synthesis, and hydrogen storage. This dissertation presents the results from several studies related to ammonia borane. ^ The pressure-induced tetragonal to orthorhombic phase transition in ammonia borane was studied in a diamond anvil cell using in situ Raman spectroscopy. We found a positive Clapeyron-slope for this phase transformation in the experiment, which implies that the phase transition from tetragonal to orthorhombic is exothermic. The result of this study indicates that the rehydrogenation of the high pressure orthorhombic phase is expected to be easier than that of the ambient pressure tetragonal phase due to its lower enthalpy. ^ The high pressure behavior of ammonia borane after thermal decomposition was studied by in situ Raman spectroscopy at high pressures up to 10 GPa. The sample of ammonia borane was first decomposed at ∼140 degree Celcius and ∼0.7 GPa and then compessed step wise in an isolated sample chamber of a diamond anvil cell for Raman spectroscopy measurement. We did not observe the characteristic shift of Raman mode under high pressure due to dihydrogen bonding, indicating that the dihydrogen bonding disappears in the decomposed ammonia borane. Although no chemical rehydrogenation was detected in this study, the decomposed ammonia borane could store extra hydrogen by physical absorption. ^ The effect of nanoconfinement on ammonia borane at high pressures and different temperatures was studied. Ammonia borane was mixed with a type of mesoporous silica, SBA-15, and restricted within a small space of nanometer scale. The nano-scale ammonia borane was decomposed at ∼125 degree Celcius in a diamond anvil cell and rehydrogenated after applying high pressures up to ∼13 GPa at room temperature. The successful rehydrogenation of decomposed nano-scale ammonia borane gives guidance to further investigations on hydrogen storage. ^ In addition, the high pressure behavior of lithium amidoborane, one derivative of ammonia borane, was studied at different temperatures. Lithium amidoborane (LAB) was decomposed and recompressed in a diamond anvil cell. After applying high pressures on the decomposed lithium amidoborane, its recovery peaks were discovered by Raman spectroscopy. This result suggests that the decomposition of LAB is reversible at high pressures.^

High Pressure and Low Temperature Study of Ammonia Borane and Lithium Amidoborane

Hydrogen has been considered as a potentially efficient and environmentally friendly alternative energy solution. However, one of the most important scientific and technical challenges that the “hydrogen economy” faces is the development of safe and economically viable on-board hydrogen storage for fuel cell applications, especially to the transportation sector. Ammonia borane (BH3NH3), a solid state hydrogen storage material, possesses exceptionally high hydrogen content (19.6 wt%).However, a fairly high temperature is required to release all the hydrogen atoms, along with the emission of toxic borazine. Recently research interests are focusing on the improvement of H2 discharge from ammonia borane (AB) including lowering the dehydrogenation temperature and enhancing hydrogen release rate using different techniques. Till now the detailed information about the bonding characteristics of AB is not sufficient to understand details about its phases and structures. Elemental substitution of ammonia borane produces metal amidoboranes. Introduction of metal atoms to the ammonia borane structure may alter the bonding characteristics. Lithium amidoborane is synthesized by ball milling of ammonia borane and lithium hydride. High pressure study of molecular crystal provides unique insight into the intermolecular bonding forces and phase stability. During this dissertation, Raman spectroscopic study of lithium amidoborane has been carried out at high pressure in a diamond anvil cell. It has been identified that there is no dihydrogen bond in the lithium amidoborane structure, whereas dihydrogen bond is the characteristic bond of the parent compound ammonia borane. It has also been identified that the B-H bond becomes weaker, whereas B-N and N-H bonds become stronger than those in the parent compound ammonia borane. At high pressure up to 15 GPa, Raman spectroscopic study indicates two phase transformations of lithium amidoborane, whereas synchrotron X-ray diffraction data indicates only one phase transformation of this material. Pressure and temperature has a significant effect on the structural stability of ammonia borane. This dissertation explored the phase transformation behavior of ammonia borane at high pressure and low temperature using in situ Raman spectroscopy. The P-T phase boundary between the tetragonal (I4mm) and orthorhombic (Pmn21) phases of ammonia borane has been determined. The transition has a positive Clapeyron slope which indicates the transition is of exothermic in nature. Influence of nanoconfinemment on the I4mm to Pmn21 phase transition of ammonia borane was also investigated. Mesoporus silica scaffolds SBA-15 with pore size of ~8 nm and MCM-41 with pore size of 2.1-2.7 nm, were used to nanoconfine ammonia borane. During cooling down, the I4mm to Pmn21 phase transition was not observed in MCM-41 nanoconfined ammonia borane, whereas the SBA-15 nanocondfined ammonia borane shows the phase transition at ~195 K. Four new phases of ammonia borane were also identified at high pressure up to 15 GPa and low temperature down to 90 K.

Étude de propriétés physico-chimiques des membranes lipidiques chargées d’acide palmitique/stérol et de stéarylamine/cholestérol

Les stérosomes, des vésicules artificielles composées d’amphiphiles monoalkylés et d’un grand pourcentage de stérols, sont prometteurs dans plusieurs domaines comme les industries pharmaceutiques et alimentaires. Il existe des stérosomes chargés négativement, positivement et neutres. Dans ce mémoire, nous avons approfondi nos connaissances sur les propriétés physico-chimiques des stérosomes chargés : acide palmitique (PA)/stérol et stéarylamine (SA)/cholestérol (Chol). Premièrement, afin de mesurer la diffusion latérale de PA dans les membranes PA/stérol (30/70 mol/mol) par RMN à gradients pulsés, nous avons tenté de former des bicouches liquide-ordonnées (lo) orientées magnétiquement avec ce mélange. En s'inspirant de l’idée que l’ajout de 1,2-dihexanoyl-sn-glycéro-3-phosphocholine (DHPC), un lipide à courtes chaînes, dans le système 1,2-dimyristoyl-sn-glycéro-3-phosphocholine (DMPC) mène à la formation de bicouches orientées, nous avons étudié la formulation PA perdeutéré/acide hexanoïque (HA)/Chol avec une proportion molaire de 25/18/57 à plusieurs températures; aucune formation de bicouches orientées n’a été observée. Ce résultat pourrait être expliqué par la solubilisation partielle de HA en milieu aqueux. Alors, une quantité insuffisante serait insérée dans la bicouche pour induire son orientation. La formulation PA perdeutéré/DHPC/Chol n’a pas conduit, elle non plus, à des bicouches orientées magnétiquement à des températures et concentrations lipidiques variées. En étudiant le mélange DMPC/DHPC/Chol (67/17/14), nous avons remarqué que la présence de Chol inhibait l'orientation magnétique des bicouches. Tandis que le mélange DMPC/DHPC/stigmastérol (SS) avec les proportions molaires 67/19/14 et 72/21/7 conduisait à des bicouches orientées avec leur normale (n) perpendiculaire au champ magnétique à 40 °C et 50 °C. Ces résultats suggèrent que le mélange PA/SS avec une proportion de lipide à courtes chaînes, HA et DHPC, pourrait mener à des bicouches orientées magnétiquement. Le mélange PA/Chol avec un lipide à courtes chaînes pourrait aussi être étudié en présence des lanthanides. Deuxièmement, nous avons examiné la possibilité de moduler la libération de matériel encapsulé dans des liposomes essentiellement composés de PA et d’un stérol. Il est connu que le mélange PA/Chol (30/70) à pH ≥ 7,5 forme des liposomes très peu perméables. Il est avantageux de pouvoir moduler la perméabilité pour avoir un contrôle sur le temps de libération de leur contenu, qui est un paramètre de grande importance pour les formulations liposomales de médicaments. D’abord, il a été montré que l’acide oléique (OA)/Chol (30/70) est capable de former des vésicules, ce qui n’avait jamais été prouvé auparavant. Par contre, les bicouches OA/Chol (30/70) ne sont pas plus perméables que les bicouches PA/Chol (30/70). L’ajout de 1-palmitoyl-2-oléoyl-sn-glycéro-3-phosphatidylcholine (POPC) dans le mélange PA/Chol n’augmente pas plus la perméabilité. En effet, les cinétiques de relargage de calcéine des vésicules PA/POPC/Chol (15/27.5/57.5), POPC/Chol (40/60) et POPC étaient très semblables à celle de PA/Chol (30/70). Il a été remarqué que les études littéraires se contredisent à propos de la perméabilité à la calcéine des bicouches de phosphatidylcholine (PC). L’explication de ces divergences est inconnue pour le moment. En remplaçant la moitié de la proportion molaire de Chol par le cholate de sodium (SC) dans le mélange PA/Chol (30/70), la membrane n’était pas plus apte à libérer son contenu. Il se pourrait que le SC se retrouvant dans la bicouche n’induit pas une diminution d’empilement. Il est aussi possible que le SC ne s'insère pas dans la membrane à cause de son hydrophilie considérable et il pourrait alors former seul des micelles. En remplaçant complètement le Chol par le sulfate de cholestérol (SChol), un stérol chargé négativement, et en préparant les vésicules à un bas pH, la formulation PA/SChol (30/70) mène à une très grande perméabilité à pH 7.5; le relargage est provoqué par un saut de pH. Nos travaux suggèrent qu'il serait possible de moduler la perméabilité des liposomes en les préparant avec le mélange PA/SChol/Chol en variant les proportions entre 30/63/7 à 30/70/0. Le diagramme pH-composition du mélange PA/SChol/Chol indique que ces proportions conduisent, à pH 7.4, à la coexistence de phases solide et lo en différentes proportions, ce qui pourrait moduler la perméabilité membranaire. Troisièmement, les résultats de perméabilité obtenus avec la calcéine et les difficultés survenues lors de l’extrusion des vésicules encapsulant cette sonde nous ont amené à nous demander si la calcéine interagit avec les bicouches chargées. L’impact de certains anions, dont la calcéine, a été examiné sur les bicouches chargées positivement SA/Chol (50/50). La calorimétrie différentielle à balayage (DSC, de l’anglais differential scanning calorimetry), indique qu’il n’y a aucune transition entre 25 et 90 °C pour les liposomes SA/Chol (50/50) à pH = 7.4. L’ajout de chlorure de sodim (375 mM) n’a pas mené à la formation d’agrégats et aucune transition n’a été observée sur le thermogramme. La formation d’agrégats macroscopiques instantanément après l’ajout d’hydrogénophosphate de sodium (125 mM), de sulfate de sodium (125 mM) et de calcéine (3 mM) a été observée. Une transition a été observée sur les thermogrammes en présence de ces sels. Les agrégats observés pourraient être associés à la transition de phase. L’effet des anions sur la température et l’enthalpie de transition suivent le même ordre que la série d’Hofmeister : sulfate > hydrogénophosphate > chlorure (pas de pic). La calcéine avait l’impact le plus prononcé sur l’agrégation; ceci illustre que la calcéine n’est pas une sonde fluorescente inerte avec le mélange SA/Chol. Elle pourrait être un chaotrope volumineux. De plus, les interactions SA-calcéine plus fortes, menant à l’agrégation des vésicules, que les interactions PC-calcéine pourraient s’expliquer par le fait que la SA est chargée positivement.

Hybrid Monte Carlo algorithm for the double exchange model

The Hybrid Monte Carlo algorithm is adapted to the simulation of a system of classical degrees of freedom coupled to non self-interacting lattices fermions. The diagonalization of the Hamiltonian matrix is avoided by introducing a path-integral formulation of the problem, in d + 1 Euclidean space–time. A perfect action formulation allows to work on the continuum Euclidean time, without need for a Trotter–Suzuki extrapolation. To demonstrate the feasibility of the method we study the Double Exchange Model in three dimensions. The complexity of the algorithm grows only as the system volume, allowing to simulate in lattices as large as 163 on a personal computer. We conclude that the second order paramagnetic–ferromagnetic phase transition of Double Exchange Materials close to half-filling belongs to the Universality Class of the three-dimensional classical Heisenberg model.

Critical behavior of the three-dimensional Ising spin glass

We have simulated, using parallel tempering, the three-dimensional Ising spin glass model with binary couplings in a helicoidal geometry. The largest lattice (L520) has been studied using a dedicated computer (the SUE machine). We have obtained, measuring the correlation length in the critical region, strong evidence for a second-order finite-temperature phase transition, ruling out other possible scenarios like a KosterlitzThouless phase transition. Precise values for the ν and ƞ critical exponents are also presented.

Critical behavior in the site-diluted three-dimensional three-state Potts model

We have studied numerically the effect of quenched site dilution on a weak first-order phase transition in three dimensions. We have simulated the site diluted three-states Potts model studying in detail the secondorder region of its phase diagram. We have found that the n exponent is compatible with the one of the three-dimensional diluted Ising model, whereas the h exponent is definitely different.

Manipulating the structural and electronic properties of epitaxial NaNbO3 films via strain and stoichiometry

Due to their intriguing dielectric, pyroelectric, elasto-electric, or opto-electric properties, oxide ferroelectrics are vital candidates for the fabrication of most electronics. However, these extraordinary properties exist mainly in the temperature regime around the ferroelectric phase transition, which is usually several hundreds of K away from room temperature. Therefore, the manipulation of oxide ferroelectrics, especially moving the ferroelectric transition towards room temperature, is of great interest for application and also basic research. In this thesis, we demonstrate this using examples of NaNbO3 films. We show that the transition temperature of these films can be modified via plastic strain caused by epitaxial film growth on a structurally mismatched substrate, and this strain can be fixed by controlling the stoichiometry. The structural and electronic properties of Na1+xNbO3+δ thin films are carefully examined by among others XRD (e.g. RSM) and TEM and cryoelectronic measurements. Especially the electronic features are carefully analyzed via specially developed interdigitated electrodes in combination with integrated temperature sensor and heater. The electronic data are interpreted using existing as well as novel theories and models, they are proved to be closely correlated to the structural characteristics. The major results are: -Na1+xNbO3+δ thin films can be grown epitaxially on (110)NdGaO3 with a thickness up to 140 nm (thicker films have not been studied). Plastic relaxation of the compressive strain sets in when the thickness of the film exceeds approximately 10 – 15 nm. Films with excess Na are mainly composed of NaNbO3 with minor contribution of Na3NbO4. The latter phase seems to form nanoprecipitates that are homogeneously distributed in the NaNbO3 film which helps to stabilize the film and reduce the relaxation of the strain. -For the nominally stoichiometric films, the compressive strain leads to a broad and frequency-dispersive phase transition at lower temperature (125 – 147 K). This could be either a new transition or a shift in temperature of a known transition. Considering the broadness and frequency dispersion of the transition, this is actually a transition from the dielectric state at high temperature to a relaxor-type ferroelectric state at low temperature. The latter is based on the formation of polar nano-regions (PNRs). Using the electric field dependence of the freezing temperature, allows a direct estimation of the volume (70 to 270 nm3) and diameter (5.2 to 8 nm, spherical approximation) of the PNRs. The values confirm with literature values which were measured by other technologies. -In case of the off-stoichiometric samples, we observe again the classical ferroelectric behavior. However, the thermally hysteretic phase transition which is observed around 620 – 660 K for unstrained material is shifted to room temperature due to the compressive strain. Beside to the temperature shift, the temperature dependence of the permittivity is nearly identical for strained and unstrained materials. -The last but not least, in all cases, a significant anisotropy in the electronic and structural properties is observed which arises automatically from the anisotropic strain caused by the orthorhombic structure of the substrate. However, this anisotropy cannot be explained by the classical model which tries to fit an orthorhombic film onto an orthorhombic substrate. A novel “square lattice” model in which the films adapt a “square” shaped lattice in the plane of the film during the epitaxial growth at elevated temperature (~1000 K) nicely explains the experimental results. In this thesis we sketch a way to manipulate the ferroelectricity of NaNbO3 films via strain and stoichiometry. The results indicate that compressive strain which is generated by the epitaxial growth of the film on mismatched substrate is able to reduce the ferroelectric transition temperature or induce a phase transition at low temperature. Moreover, by adding Na in the NaNbO3 film a secondary phase Na3NbO4 is formed which seems to stabilize the main phase NaNbO3 and the strain and, thus, is able to engineer the ferroelectric behavior from the expected classical ferroelectric for perfect stoichiometry to relaxor-type ferroelectric for slightly off-stoichiometry, back to classical ferroelectric for larger off-stoichiometry. Both strain and stoichiometry are proven as perfect methods to optimize the ferroelectric properties of oxide films.

Coupled wellbore-reservoir simulation of thermal effects during multiphase CO2 injection

T2Well-ECO2M is a coupled wellbore reservoir simulator still under development at Lawrence Berkeley National Laboratory (USA) with the ability to deal with a mixture of H2O-CO2-NaCl and includes the simulation of CO2 phase transition and multiphase flow. The code was originally developed for the simulation of CO2 injection into deep saline aquifers and the modelling of enhanced geothermal systems; however, the focus of this research was to modify and test T2Well-ECO2M to simulate CO2 injection into depleted gas reservoirs. To this end, the original code was properly changed in a few parts and a dedicated injection case was developed to study CO2 phase transition inside of a wellbore and the corresponding thermal effects. In the first scenario, the injection case was run applying the fully numerical approach of wellbore to formation heat exchange calculation. Results were analysed in terms of wellbore pressure and temperature vertical profiles, wellhead and bottomhole conditions, and characteristic reservoir displacement fronts. Special attention was given to the thorough analysis of bottomhole temperature as the critical parameter for hydrate formation. Besides the expected direct effect of wellbore temperature changes on reservoir conditions, the simulation results indicated also the effect of CO2 phase change in the near wellbore zone on BH pressure distribution. To test the implemented software changes, in a second scenario, the same injection case was reproduced using the improved semi-analytical time-convolution approach for wellbore to formation heat exchange calculation. The comparison of the two scenarios showed that the simulation of wellbore and reservoir parameters after one year of continuous CO2 injection are in good agreement with the computation time to solve the time-convolution semi-analytical reduced. The new updated T2Well-ECO2M version has shown to be a robust and performing wellbore-reservoir simulator that can be also used to simulate the CO2 injection into depleted gas reservoirs.

Many-body approach to the BCS-BEC crossover for an imbalanced ultra-cold Fermi gas

The aim of this thesis is the study of the normal phase of a mass imbalanced and polarized ultra-cold Fermi gas in the context of the BCS-BEC crossover, using a diagrammatic approach known as t-matrix approximation. More specifically, the calculations are implemented using the fully self-consistent t-matrix (or Luttinger- Ward) approach, which is already experimentally and numerically validated for the balanced case. An imbalance (polarization) between the two spin populations works against pairing and superfluidity. For sufficiently large polarization (and not too strong attraction) the system remains in the normal phase even at zero temperature. This phase is expected to be well described by the Landau’s Fermi liquid theory. By reducing the spin polarization, a critical imbalance is reached where a quantum phase transition towards a superfluid phase occurs and the Fermi liquid description breaks down. Depending on the strength of the interaction, the exotic superfluid phase at the quantum critical point (QCP) can be either a FFLO phase (Fulde-Ferrell-Larkin-Ovchinnikov) or a Sarma phase. In this regard, the presence of mass imbalance can strongly influence the nature of the QCP, by favouring one of these two exotic types of pairing over the other, depending on whether the majority of the two species is heavier or lighter than the minority. The analysis of the system is made by focusing on the temperature-coupling-polarization phase diagram for different mass ratios of the two components and on the study of different thermodynamic quantities at finite temperature. The evolution towards a non-Fermi liquid behavior at the QCP is investigated by calculating the fermionic quasi-particle residues, the effective masses and the self-energies at zero temperature.

Transition to complete synchronization in phase-coupled oscillators with nearest neighbor coupling

We investigate synchronization in a Kuramoto-like model with nearest neighbor coupling. Upon analyzing the behavior of individual oscillators at the onset of complete synchronization, we show that the time interval between bursts in the time dependence of the frequencies of the oscillators exhibits universal scaling and blows up at the critical coupling strength. We also bring out a key mechanism that leads to phase locking. Finally, we deduce forms for the phases and frequencies at the onset of complete synchronization.

Analytical calculation of the transition to complete phase synchronization in coupled oscillators

Here we present a system of coupled phase oscillators with nearest neighbors coupling, which we study for different boundary conditions. We concentrate at the transition to the total synchronization. We are able to develop exact solutions for the value of the coupling parameter when the system becomes completely synchronized, for the case of periodic boundary conditions as well as for a chain with fixed ends. We compare the results with those calculated numerically.

zyg-11and cul-2 promote the metaphase to anaphase transition and M phase exit of meiosis II and prevent polarity establishment in C.elegans

Résumé Les mécanismes qui coordonnent la progression du cycle cellulaire lors de la méiose avec les événements du développement embryonnaire précoce, y compris la formation des axes de polarité embryonnaire, sont peu compris. Dans le zygote du vers Caenorhabditis elegans, les premiers signes de polarité Antéro-Postérieur (A-P) embryonnaire apparaissent après que la méiose soit terminée. La nature des protéines et des mécanismes moléculaires qui cassent la symétrie du zygote n'est pas connue. Nous démontrons que zyg-11 et cul-2 promeuvent la transition métaphase - anaphase et la sortie de la phase M lors de la seconde division méiotique. Nos résultats indiquent que ZYG-11 agit comme unité recrutant le substrat d'une ligase E3 comprennant CUL-2. Nos résultats montrent aussi que le délai de sortie de la phase M dépend de l'accumulation de la Cyclin B, CYB-3. Nous démontrons que dans des embryons zyg-11(RNAi) ou cul-2(RNAi), une polarité inversée est établie lors du délai de méiosis II. Enfin nous montrons que les défauts de cycle cellulaire et ceux de polarité peuvent être séparés. De plus, nous faisons apparaitre que l'établissement d'une polarité inversée pendant le délai de méiose II des embryons zyg-11(RNAi), comme l'établissement de la A-P polarité des embryons sauvage ne semblent pas requérir les microtubules. Nous montrons également les premiers résultats d'un crible deux hybrides ainsi qu'un crible génomique qui vise à identifier des gènes dont l'inactivation augmente ou supprime les défauts de mutants pour le gène zyg-11, afin d'identifier les gènes qui intéragissent avec ZYG-11 pour assumer ses deux fonctions séparables. Par conséquent, nos trouvailles suggèrent un modèle selon lequel ZYG-11 est une sous-unité qui recrute les substrats d'une ligase E3 basée sur CUL-2 qui promeut la progression du cycle cellulaire et empêche l'établissement de la polarité pendant la méiose II, et où le centrosome agit comme la clé qui polarise l'embryon à la fin de la méiose. Summary The mechanisms that couple meiotic cell cycle progression to subsequent developmental events, including specification of embryonic axes, are poorly understood. In the one cell stage embryos of Caenorhabditis elegans, the first signs of Antero-Posterior (A-P) polarity appear after meiosis completion. A centrosome ¬derived component breaks symmetry of the embryo, but the molecular nature of this polarity signal is not known. We established that zyg-11 and cul-2 promote the metaphase to anaphase transition and M phase exit at meiosis II. Our results indicate that ZYG-11 acts as a substrate recruitment subunit of a CUL-2-based E3 ligase. Moreover, we find that the delayed meiosis II exit of embryos lacking zyg-11 is caused by accumulation of the B-type cyclin, CYB-3. We demonstrate that inverted A-P polarity is established during the meiosis II delay in zyg-11(RNAi) and cul¬2(RNAi) embryos. Importantly, we demonstrate that the polarity defects following zyg-11 or cul-2 inactivation can be uncoupled from the cell cycle defects. Furthermore, we found that microtubules appear dispensable for inverted polarity during the meiosis II delay in zyg-11(RNAi) embryos, as well as for A-P polarity during the first mitotic cell cycle in wild-type embryos. We also show the initial results from a comprehensive yeast two hybrid, as well as an RNAi-based functional genomic enhancer and suppressor screen, that may lead to identification of proteins that interact with zyg-11 to ensure the two functions. Our findings suggest a model in which ZYG-11 is a substrate recruitment subunit of an CUL-2-based E3 ligase that promotes cell cycle progression and prevents polarity establishment during meiosis II, and in which the centrosome acts as a cue to polarize the embryo along the AP axis after exit from the meiotic cell cycle.

Modélisation systémique de la transition pour des familles ayant un adolescent atteint de fibrose kystique en phase pré-transfert vers l'établissement adulte

Les progrès spectaculaires réalisés dans le traitement de la fibrose kystique font en sorte qu'un nombre de plus en plus élevé de familles comptant un adolescent atteint de ce problème de santé, peut maintenant envisager d'effectuer la transition depuis l'adolescent vers l'âge adulte. À ce jour, les recherches à ce sujet demeurent peu nombreuses, principalement en ce qui a trait à la nature des interations entre les adolescents, leurs parents et les professionnels de la santé qui préparent ces familles en vue du transfert, depuis un établissement pédiatrique vers un établissement adulte. L'appréhension de ce phénomène s'est réalisée dans une perspective constructiviste et systémique, ce qui a permis de mettre en relief certaines des multiples facettes du phénomène et de jeter un éclairage novateur sur des dynamiques entre les membres de la famille et entre ces derniers et les professionnels de la santé. Le but de cette étude de cas, de type qualitavive, était de modéliser de manière systémique, le processus de transtion pour des familles ayant un adolescent atteint de la fibrose kystique qui est en phase pré transfert, depuis l'établissement pédiatrique vers le milieu adulte. Des entretiens semi-dirigés ont été réalisés avec sept familles comptant un adolescent atteint de la fibrose kystique. De plus, un entretien de groupe a également été effectué avec une équipe interprofessionnelle oeuvrant dans une clinique qui traite des adolescents atteints de la fibrose kysitque. L'analyse qualitative des données a mené au développement d'un modèle systémique de la transition pour ces familles. Ce modèle souligne qu'en évoluant de façon parallèle, les familles et les professionnels de la santé poursuivent la même finalité de favoriser le développement de l'autonomie de l'adolescent. Ce processus de transition chez ces familles s'inscrit, par ailleurs, dans un espace-temps signifié par le transfert inter-établissements, avec peu de considération pour la souffrance parentale liée au pronostic de la maladie. Ainsi, le développement de l'autonomie est marqué par la confiance qui doit s'établir entre l'adolescent et son parent, en passant par la surveillance du parent envers l'adolescent et par la responsabilisation graduelle chez ce dernier. Cette étude propose donc une modélisation systémique de ce processus de transition qui contribue non seulement au développement du concept de la transition en sciences de la santé, mais aussi de la pratique clinique et de la recherche dans le domaine des soins à la famille aux prises avec un adolescent atteint de la fibrose kystique.

Transition from an anti-phase error-correction-mode to a synchronization mode in the mutual hand tracking

Proactive motion in hand tracking and in finger bending, in which the body motion occurs prior to the reference signal, was reported by the preceding researchers when the target signals were shown to the subjects at relatively high speed or high frequencies. These phenomena indicate that the human sensory-motor system tends to choose an anticipatory mode rather than a reactive mode, when the target motion is relatively fast. The present research was undertaken to study what kind of mode appears in the sensory-motor system when two persons were asked to track the hand position of the partner with each other at various mean tracking frequency. The experimental results showed a transition from a mutual error-correction mode to a synchronization mode occurred in the same region of the tracking frequency with that of the transition from a reactive error-correction mode to a proactive anticipatory mode in the mechanical target tracking experiments. Present research indicated that synchronization of body motion occurred only when both of the pair subjects operated in a proactive anticipatory mode. We also presented mathematical models to explain the behavior of the error-correction mode and the synchronization mode.

Analytical calculation of the transition to complete phase synchronization in coupled oscillators

Here we present a system of coupled phase oscillators with nearest neighbors coupling, which we study for different boundary conditions. We concentrate at the transition to the total synchronization. We are able to develop exact solutions for the value of the coupling parameter when the system becomes completely synchronized, for the case of periodic boundary conditions as well as for a chain with fixed ends. We compare the results with those calculated numerically.