2,768 research outputs found
Anomalous fluctuation regimes at the FFLO transition
Recently some experimental evidences have been obtained in favour of the
existence of the inhomogeneous Fulde-Ferrell-Larkin-Ovchinnikov (FFLO)
superconducting state in heavy-fermion superconductor CeCoIn_{5} and organic
superconductor -(BETS)_{2}FeCl_{4}. However the unambiguous identification of
FFLO state remains very difficult. We present the theoretical studies of the
Gaussian fluctuations near the tricritical point (where the FFLO modulation
appears) and demonstrate that the behavior of the fluctuational specific heat,
paraconductivity and diamagnetism is qualitatively different from the usual
superconducting transition. Special values of the critical exponent and the
crossovers between different fluctuational regimes may provide a unique test
for the FFLO state appearance.Comment: 6 pages, 2 figures. Work supported by ANR Extreme Conditions
Correlated Electrons (ANR-06-BLAN-0220
Influence of temperature, UV-light wavelength and intensity on polypropylene photothermal oxidation
A criterion based on the energy absorbed by photosensitive species was proposed to describe the contribution of UV-light to the initiation of the polypropylene photothermal oxidation whatever the light source. The calculation of this energy was performed using the widely accepted quantum theory. The criterion was then introduced in two different types of analytical models commonly used to describe the combined effects of UV light and temperature on induction time, namely: the reciprocity law and kinetic model. The limitations of both types of analytical models were then investigated: the latter, derived from a realistic mechanistic scheme, was found to be much more relevant than the former, which is presumably valid in a restricted range of light intensities, essentially due to its empirical origin
Competing Turing and Faraday instabilities in longitudinally modulated passive resonators
We experimentally investigate the interplay of Turing and Faraday
(modulational) instabilities in a bistable passive nonlinear resonator. The
Faraday branch is induced via parametric resonance owing to a periodic
modulation of the resonator dispersion. We show that the bistable switching
dynamics is dramatically affected by the competition between the two
instability mechanisms, which dictates two completely novel scenarios. At low
detunings from resonance switching occurs between the stable stationary lower
branch and the Faraday-unstable upper branch, whereas at high detunings we
observe the crossover between the Turing and Faraday periodic structures. The
results are well explained in terms of the universal Lugiato-Lefever model
Algorithmes efficaces pour tester l'identifiabilité locale
International audienceParmi les méthodes utilisées pour tester l'identifiabilité locale d'un système, on peut citer le développement en séries de Taylor des sorties et la méthode des similarités (similarity transformation approach). Nous rappelons que les paramètres non identifiables d'un système peuvent être déterminés par un algorithme probabiliste de complexité polynomiale en la taille de l'entrée. Cet algorithme est basé sur la méthode des développement en séries. Si le modèle considéré est non identifiable, nous montrons que cette méthode permet de calculer des groupes de transformations qui agissent sur les variables non observables et les paramètres non identifiable tout en laissant les entrées, les sorties et les trajectoires du système invariant. Ce calcul permet de certifier et compléter le résultat précédent. La méthode des similarités se base sur la résolution d'un système d'équations aux dérivées partielles pour trouver ce groupe. Notre approche ne repose que sur le calcul du noyau d'une matrice à coefficients polynomiaux et l'intégration sous forme close d'un système différentiel ordinaire de petite taille. Pour finir, nous présentons quelques exemples qui montrent l'efficacité de notre approche
A generalization of flatness to nonlinear systems of partial differential equations. Application to the command of a flexible rod
We introduce a concept of differential flatness for systems described by nonlinear partial differential equations. It generalizes the now classical notion of differential flatness for finite differential systems and its recent extensions to linear partial differential equations. We apply it to the motion planning of a very flexible rod, out of the linear approximation range
Formation of interstellar SH from vibrationally excited H: Quantum study of S + H SH + H reactions and inelastic collisions
The rate constants for the formation, destruction, and collisional excitation
of SH are calculated from quantum mechanical approaches using two new
SH potential energy surfaces (PESs) of and electronic
symmetry. The PESs were developed to describe all adiabatic states correlating
to the SH () + H() channel. The formation of SH
through the S + H reaction is endothermic by 9860 K, and
requires at least two vibrational quanta on the H molecule to yield
significant reactivity. Quasi-classical calculations of the total formation
rate constant for H() are in very good agreement with the quantum
results above 100K. Further quasi-classical calculations are then performed for
, 4, and 5 to cover all vibrationally excited H levels significantly
populated in dense photodissociation regions (PDR). The new calculated
formation and destruction rate constants are two to six times larger than the
previous ones and have been introduced in the Meudon PDR code to simulate the
physical and illuminating conditions in the Orion bar prototypical PDR. New
astrochemical models based on the new molecular data produce four times larger
SH column densities, in agreement with those inferred from recent ALMA
observations of the Orion bar.Comment: 8 pages, 7 figure
Optical Sensors Based on Whispering Gallery Modes in Fluorescent Microbeads: Size Dependence and Influence of Substrate
Whispering gallery modes in surface-fixated fluorescent polystyrene microbeads are studied in view of their capability of sensing changes in the refractive index of the beads’ environment by exposing them to water/glycerol mixtures of varying composition. The mode positions are analyzed by simultaneous fitting for mode number, bead radius, and environmental index. Down to a diameter of 8 μm, the sensor response follows the index of the bulk solution very well. For smaller bead sizes, some deviations occur, in particular for fluid indices not too different from that of water, which might be attributed to the presence of the substrate
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