Corneille. Tome 1 / éd. annotée par Frédéric Godefroy

Collection : Classiques pour tous

Systèmes vésiculaires colloïdaux pour la vectorisation de la 1-β-D-arabinofuranosylcytosine

La 1-β-D-arabinofuranosylcytosine (ara-C) demeure l’agent anticancéreux principalement utilisé dans le traitement de la leucémie myéloblastique aiguë (LMA), malgré sa dégradation et son élimination rapide après une administration parentérale. Son encapsulation dans des vecteurs pharmaceutiques, majoritairement des liposomes, a permis de surmonter ces inconvénients. L’objectif général de ce projet de doctorat était de développer deux systèmes à libération prolongée, à base de phospholipides, de cholestérol et de poly(éthylène glycol) (PEG) afin d’encapsuler l’ara-C et ultimement, d’améliorer son efficacité dans le traitement de la LMA. Des Sphérulites® (vésicules multilamellaires d’un type particulier) ont d’abord été étudiées pour leur forte capacité d’encapsulation, due à leur mode de préparation. Par la suite, une formulation liposomale capable, d’une part de cibler spécifiquement les cellules leucémiques et, d’autre part, de promouvoir la libération intracellulaire de l’ara-C grâce à sa sensibilité au pH, a été mise au point. Les deux formulations se devaient d’avoir un faible diamètre, une stabilité en présence de fluides biologiques et des temps de circulation prolongés chez l’animal. Une préparation de Sphérulites®, composée de Phospholipon 90G, de Solutol HS15 et de cholestérol, a permis d’obtenir des vésicules de 300 nm de diamètre. Un dérivé lipidique de PEG a pu être fixé à leur surface, sans modifier la disposition concentrique des lamelles, ni changer leur stabilité. Les Sphérulites® PEGylées ont été chargées d’ara-C et injectées chez le rat par la voie intraveineuse. Elles ont démontré des temps de circulation significativement prolongés comparativement aux Sphérulites® sans PEG. Cependant, l’ara-C s’est retrouvée éliminée de la circulation sanguine très rapidement, révélant une libération précoce du principe actif à partir de ces vésicules. Les liposomes sensibles au pH (~150 nm) ont été obtenus suite à l’insertion d’un copolymère à base de dioctadécyle, de N-isopropylacrylamide (NIPAM) et d’acide méthacrylique. L’anticorps anti-CD33, soit complet soit son fragment Fab’, a été fixé à la surface des liposomes afin de cibler les cellules leucémiques. Les essais in vitro ont démontré la spécificité de la formulation pour différentes cellules leucémiques (CD33+), sa stabilité en présence de protéines plasmatiques et la libération intracellulaire d’un marqueur fluorescent et de l’ara-C. Enfin, des études menées chez la souris saine et immunodéprimée inoculée de cellules HL60 ont montré que la formulation exposant le fragment Fab’ possédait un profil pharmacocinétique et une biodistribution semblables à ceux des liposomes contrôles non-ciblés. L’encapsulation de l’ara-C a permis d’améliorer grandement ses temps de circulation après une administration intraveineuse. Cependant, bien que les immunoliposomes ont permis de prolonger la survie des souris leucémiques comparativement à l’ara-C libre, l’addition du polymère sensible au pH n’a pas permis d’apporter de réel avantage à la formulation lorsque administrée in vivo. Les résultats obtenus dans ce travail de thèse ont, dans un premier temps, mis en évidence que les Sphérulites® pourraient s’avérer utiles dans la vectorisation d’agents anticancéreux si leur capacité à retenir le principe actif in vivo était améliorée. Dans un second temps, les données présentées avec les immunoliposomes suggèrent qu’ils pourraient apporter un bénéfice notable dans le traitement de la LMA.

Jornades sobre el turisme en els espais litorals: turisme, territori i estratègies de desenvolupament. (Girona, 29, 30, 31 de març i 1 d'abril de 1995)

The congress about tourism in the coastal spaces: "Turisme, territori i estratègies de desenvolupament, has been a place of debate and discussion about nowadays validity of the traditional model of tourisrn and at the sarne time a platform to reformulate this model. Throughout the congress, it has been shown the need to change the tourist model towards a model of sustainable developrnent

Unusual isotope effect in the reaction of chlorosilylene with trimethylsilane-1-d: Absolute rate studies and quantum chemical and Rice–Ramsperger–Kassel–Marcus calculations provide strong evidence for the involvement of an intermediate complex

Time-resolved studies of chlorosilylene, ClSiH, generated by the 193 nm laser flash photolysis of 1-chloro-1- silacyclopent-3-ene, have been carried out to obtain rate constants for its bimolecular reaction with trimethylsilane-1-d, Me3SiD, in the gas phase. The reaction was studied at total pressures up to 100 Torr (with and without added SF6) over the temperature range of 295−407 K. The rate constants were found to be pressure independent and gave the following Arrhenius equation: log[(k/(cm3 molecule−1 s−1)] = (−13.22 ± 0.15) + [(13.20 ± 1.00) kJ mol−1]/(RT ln 10). When compared with previously published kinetic data for the reaction of ClSiH with Me3SiH, kinetic isotope effects, kD/kH, in the range from 7.4 (297 K) to 6.4 (407 K) were obtained. These far exceed values of 0.4−0.5 estimated for a single-step insertion process. Quantum chemical calculations (G3MP2B3 level) confirm not only the involvement of an intermediate complex, but also the existence of a low-energy internal isomerization pathway which can scramble the D and H atom labels. By means of Rice−Ramsperger−Kassel−Marcus modeling and a necessary (but small) refinement of the energy surface, we have shown that this mechanism can reproduce closely the experimental isotope effects. These findings provide the first experimental evidence for the isomerization pathway and thereby offer the most concrete evidence to date for the existence of intermediate complexes in the insertion reactions of silylenes.

A dramatic isotope effect in the reaction of ClSiH with trimethylsilane-1-d: experimental evidence for intermediate complexes in silylene Si-H(D) insertion reactions

A kinetic isotope effect (kD/kH) of 7.4 has been found for the reaction of chlorosilylene with trimethysilane (Me3SiD vs Me3SiH). Such a value can be accounted for by theoretical modelling, but only if an internal rearrangement of the initially form complex is included in the mechanism. This provides the first concrete evidence for such complexes.

Data assimilation with correlated observation errors: experiments with a 1-D shallow water model

Remote sensing observations often have correlated errors, but the correlations are typically ignored in data assimilation for numerical weather prediction. The assumption of zero correlations is often used with data thinning methods, resulting in a loss of information. As operational centres move towards higher-resolution forecasting, there is a requirement to retain data providing detail on appropriate scales. Thus an alternative approach to dealing with observation error correlations is needed. In this article, we consider several approaches to approximating observation error correlation matrices: diagonal approximations, eigendecomposition approximations and Markov matrices. These approximations are applied in incremental variational assimilation experiments with a 1-D shallow water model using synthetic observations. Our experiments quantify analysis accuracy in comparison with a reference or ‘truth’ trajectory, as well as with analyses using the ‘true’ observation error covariance matrix. We show that it is often better to include an approximate correlation structure in the observation error covariance matrix than to incorrectly assume error independence. Furthermore, by choosing a suitable matrix approximation, it is feasible and computationally cheap to include error correlation structure in a variational data assimilation algorithm.

Can the pi(+) chi(c1) resonance structures be D*(D)over-bar* and D(1)(D)over-bar molecules?

We use QCD sum rules to study the recently observed resonance-like structures in the pi(+)chi(c1) mass distribution, Z(1)(+) (4050) and Z(2)(+) (4250), considered as D*(+) (D) over bar*(0) and D(1)(+) (D) over bar (0) + D(+) (D) over bar (0)(1) molecules with the quantum number J(P) = 0(+) and J(P) = 1-, respectively. We consider the contributions of condensates up to dimension eight and work at leading order in alpha(s). We obtain m(D*D*) = (4.15 +/- 0.12) GeV, around 100 MeV above the D*D* threshold, and m(D1D) = (4.19 +/- 0.22) GeV, around 100 MeV below the D(1)D threshold. We conclude that the D*(+)(D) over bar*(0) state is probably a virtual state that is not related with the Z(1)(+) (4050) resonance-like structure. In the case of the D(1)D molecular state, considering the errors, its mass is consistent with both Z(1)(+)(4050) and Z(2)(+)(4250) resonance-like structures. Therefore, we conclude that no definite conclusion can be drawn for this state from the present analysis. (C) 2008 Elsevier B.V All rights reserved.

Spontaneous breaking of superconformal invariance in (2+1) D supersymmetric Chern-Simons-matter theories in the large N limit

In this work we study the spontaneous breaking of superconformal and gauge invariances in the Abelian N = 1,2 three-dimensional supersymmetric Chern-Simons-matter (SCSM) theories in a large N flavor limit. We compute the Kahlerian effective superpotential at subleading order in 1/N and show that the Coleman-Weinberg mechanism is responsible for the dynamical generation of a mass scale in the N = 1 model. This effect appears due to two-loop diagrams that are logarithmic divergent. We also show that the Coleman-Weinberg mechanism fails when we lift from the N = 1 to the N = 2 SCSM model. (C) 2010 Elsevier B.V All rights reserved.

Quadratic gravity in (2+1)D with a topological Chern-Simons term

Three-dimensional quadratic gravity, unlike general relativity in (2+1)D, is dynamically nontrivial and has a well behaved nonrelativistic potential. Here we analyse the changes that occur when a topological Chem-Simons term is added to this theory. It is found that the harmless massive scalar mode of the latter gives rise to a troublesome massive spin-0 ghost, while the massive spin-2 ghost is replaced by two massive physical particles both of spin 2. We also found that light deflection does not have the 'wrong sign' such as in the framework of three-dimensional quadratic gravity.