Le rôle d’Akt dans la réponse cellulaire aux dommages à l’ADN induits par les ultraviolets dans les cellules de mélanomes humains

Le mélanome malin est l’un des cancers les plus mortels dont l’incidence continue à augmenter chaque année avec peu de traitement efficace à long terme. Il est causé et initié principalement par l’exposition excessive aux rayons ultraviolets engendrant des photoproduits hautement génotoxiques. Il est bien connu que la cascade de signalisation PI3K/Akt joue un rôle crucial dans la régulation des processus qui sont généralement dérégulés durant le développement tumoral comme la prolifération, le contrôle du cycle cellulaire et l’apoptose. Néanmoins, l’implication de cette voie moléculaire dans la réponse aux dommages à l’ADN est peu caractérisée. Chez les mammifères, trois isoformes de la protéine kinase Akt ont été identifiées: Akt1, Akt2 et Akt3. Bien qu’elles soient très homologues en termes de séquence, plusieurs études ont montré que ces isoformes ont des fonctions biologiques distinctes, et nous suggérons qu’elles puissent contribuer différemment à la régulation de la réponse génotoxique. Les objectifs de ce projet étaient de: (i) évaluer l’activation d’Akt dans les cellules de mélanomes (ii) déterminer l’impact de l’inhibition de cette activité sur la régulation de la réponse cellulaire aux UV (iii) vérifier si la perte d’expression de l’un ou de l’autre des isoformes d’Akt peut réguler la réponse aux UV. Nous avons démontré qu’Akt est transitoirement hyperactivée par phosphorylation suite aux irradiations UV dans les lignées cellulaires de mélanomes. Afin de déterminer l'importance de cette activation dans la réponse cellulaire aux UV, notre approche était de diminuer (i) la phosphorylation d’Akt par l’usage d’inhibiteurs pharmacologiques ou (ii) l’expression de chaque isoforme d’Akt par l’approche des ARN interférents. Nous avons montré que l’inhibition de la phosphorylation d’Akt amène à l’augmentation du taux de l’apoptose induit par les UV d’une manière isoforme spécifique, alors qu’elle n’a aucun effet sur la régulation de la voie de réparation par excision de nucléotides (NER), qui est la seule voie humaine pour éliminer les dommages à l’ADN induits par les UV. En somme, notre étude constitue un nouvel aspect qui permet de mieux comprendre les mécanismes moléculaires du développement de mélanomes malins suites aux irradiations ultraviolettes.

Réaction de photocyclodéshydrogénation par catalyse photorédox

Cette thèse présente une nouvelle méthode pour accomplir la réaction de Mallory en utilisant la lumière visible. Pour atteindre ce but, la chimie photorédox qui s'est développée ces dernières années permettra une utilisation efficace de la lumière visible. De plus, la chimie en flux continu sera utilisé afin d'augmenter la surface irradiée du mélange réactionnel. Au cours de ces travaux, une nouvelle méthodologie photochimique utilisant un photocatalyseur de cuivre avec la lumière visible a été efficace pour la synthèse du 5hélicène. Un mécanisme de désactivation oxydante est proposé pour cette réaction. Par ailleurs, cette nouvelle méthodologie a été utilisée pour la synthèse d'un dérivé du 5hélicène et d'un 4hélicène-pyrène hybride. Par la suite, la méthodologie photochimique utilisant un photocatalyseur de cuivre avec la lumière visible a servi à la synthèse de divers carbazoles substitués au niveau de l'azote par des groupements aryles et alkyles. Au cours de cette synthèse, la réaction a révélé un problème de régiosélectivité. Ce dernier a été étudié par la synthèse de nouvelles triarylamines. Finalement, il a été découvert que l'utilisation d'un photocatalyseur de fer peut remplacer le photocatalyseur de cuivre en utilisant l'oxygène comme oxydant pour la synthèse de 9-phénylcarbazole.

Films minces de copolymères à blocs supramoléculaires et photosensibles

La technique de trempage («dip-coating») est un procédé rapide et efficace pour former des films minces de copolymères à blocs (CPB) d’épaisseur et de nano-morphologies variées. Très peu d’études ont toutefois porté sur le trempage des CPB supramoléculaires et/ou photosensibles. Le trempage du CPB poly(styrène-b-4-vinyl pyridine) (PS-P4VP) a premièrement été étudié avec des petites molécules (PM) d’acide 1-naphtoïque (NCOOH) et de 1-naphtol (NOH) capables de former des ponts hydrogène (ponts H) avec le bloc P4VP dans 4 solvants (tétrahydrofurane (THF), p-dioxane, toluène et chloroforme). Le ratio d’incorporation (RI) molaire PM/VP dans les films trempés augmente avec la vitesse de retrait mais sa variation dépend fortement du solvant et de la PM utilisés. Le RI et la morphologie des films minces dépendent de la possibilité (ou non) du solvant à former des ponts H avec la PM et de sa sélectivité au bloc de PS menant (ou non) à des micelles de P4VP/PM en solution dont la rigidité influence l’état cinétique du système en film mince. La dépendance en une courbe en V de l’épaisseur des films en fonction la vitesse de retrait définit deux régimes, nommés régimes capillaire et de drainage. Ces régimes influencent différemment le RI et la morphologie finale. Nous nous sommes ensuite intéressés aux complexes de PS-P4VP avec des azobenzènes (AB) photosensibles, le 4-hydroxy-4’-butyl-azobenzène (BHAB) et le 4-hydroxy-4’-cyano-azobenzène (CHAB). Ces AB peuvent non seulement former des ponts H avec le bloc P4VP mais aussi s'isomériser entre les formes trans et cis sous illumination. Les expériences avec PS-P4VP/BHAB dans le THF et le toluène ont révélé que l'irradiation pendant le trempage permet de provoquer une transition entre les morphologies sphérique et cylindrique à basses vitesses de retrait. Ces transitions sont expliquées par l’augmentation du ratio molaire BHAB/VP pris dans les films sous illumination et par le plus grand volume des isomères BHAB-cis par rapport aux BHAB-trans. L'irradiation permet également de moduler l'épaisseur des films sans égard à la présence des AB. Finalement, des solutions de PS-P4VP/CHAB et PS-P4VP/BHAB dans le THF avec un CPB de masse molaire plus élevée ont été étudiées afin de comprendre l’effet d'un temps de demi-vie plus court de l’AB et de la présence de micelles en solution. Le photocontrôle morphologique perd de son efficacité avec le CHAB car l’augmentation du RI de CHAB dans les films illuminés par rapport aux films non irradiés est moins prononcée que pour les complexes de BHAB. Le choix du PS-P4VP est également important puisque la présence de micelles dans les solutions de THF du PS-P4VP(36,5k-16k), même si elle n’influence pas les RI BHAB/VP, fige davantage la morphologie sphérique en solution par rapport à une solution non-micellaire de PS-P4VP(24k-9,5k), limitant les possibilités de transition morphologique.

The Role of Diffusion in ISOL Targets for the Production of Radioactive Ion Beams

On line isotope separation techniques (ISOL) for production of ion beams of short-lived radionuclides require fast separation of nuclear reaction products from irradiated target materials followed by a transfer into an ion source. As a first step in this transport chain the release of nuclear reaction products from refractory metals has been studied systematically and will be reviewed. High-energy protons (500 - 1000 MeV) produce a large number of radionuclides in irradiated materials via the nuclear reactions spallation, fission and fragmentation. Foils and powders of Re, W, Ta, Hf, Mo, Nb, Zr, Y, Ti and C were irradiated with protons (600 - 1000 MeV) at the Dubna synchrocyclotron, the CERN synchrocyclotron and at the CERN PS-booster to produce different nuclear reaction products. The main topic of the paper is the determination of diffusion coefficients of the nuclear reaction products in the target matrix, data evaluation and a systematic interpretation of the data. The influence of the ionic radius of the diffusing species and the lattice type of the host material used as matrix or target on the diffusion will be evaluated from these systematics. Special attention was directed to the release of group I, II and III-elements. Arrhenius plots lead to activation energies of the diffusion process.

Vacuum-ultraviolet photochemically initiated modification of polystyrene surfaces: morphological changes and mechanistic investigations

Vacuum-ultraviolet (VUV) irradiation (kexc: 172 ± 12 nm) of polystyrene films in the presence of oxygen produced not only oxidatively functionalized surfaces, but generated also morphological changes. Whereas OH- and C=O-functionalized surfaces might be used for e.g. secondary functionalization, enhanced aggregation or printing, processes leading to morphological changes open new possibilities of microstructurization. Series of experiments made under different experimental conditions brought evidence of two different reaction pathways: introduction of OH- and C=O-groups at the polystyrene pathways is mainly due to the reaction of reactive oxygen species (hydroxyl radicals, atomic oxygen, ozone) produced in the gas phase between the VUV-radiation source and the substrate. However, oxidative fragmentation leading to morphological changes, oxidation products of low molecular weight and eventually to mineralization of the organic substrate is initiated by electronic excitation of the polymer leading to C–C-bond homolysis and to a complex oxidation manifold after trapping of the C-centred radicals by molecular oxygen. The pathways of oxidative functionalization or fragmentation could be differentiated by FTIR-ATR analysis of irradiated polystyrene surfaces before and after washing with acetonitrile and microscopic fluorescence analysis of the surfaces secondarily functionalized with the N,N,N-tridodecyl-triaza-triangulenium (TATA) cation. Ozonization of the polystyrene leads to oxidative functionalization of the polymer surface but cannot initiate the fragmentation of the polymer backbone. Oxidative fragmentation is initiated by electronic excitation of the polymer (contact-mode AFM analysis), and evidence of the generation of intermediate C-centred radicals is given e.g. by experiments in the absence of oxygen leading to cross-linking (solubility effects, optical microscopy, friction-mode AFM) and disproportionation (fluorescence).

Prompt electron emission and collisional ionization of ambient gas during pulsed laser ablation of silver

A silver target kept under partial vacuum conditions was irradiated with focused nanosecond pulses at 1:06 mm from a Nd:YAG laser. The electron emission monitored with a Langmuir probe shows a clear twin-peak distribution. The first peak which is very sharp has only a small delay and it indicates prompt electron emission with energy as much as 60 5 eV. Also the prompt electron emission shows a temporal profile with a width that is same as that for the laser pulse whereas the second peak is broader, covers several microseconds, and represents the low-energy electrons (2 0:5 eV) associated with the laser-induced silver plasma as revealed by time-of-flight measurements. It has been found that prompt electrons ejected from the target collisionally excite and ionize ambient gas molecules. Clearly resolved rotational structure is observed in the emission spectra of ambient nitrogen molecules. Combined with time-resolved spectroscopy, the prompt electrons can be used as excitation sources for various collisional excitation–relaxation experiments. The electron density corresponding to the first peak is estimated to be of the order of 1017 cm?--3 and it is found that the density increases as a function of distance away from the target. Dependence of probe current on laser intensity shows plasma shielding at high laser intensities.

Possibility of waveguide formation on organic nonlinear crystal methyl para-hydroxy benzoate using high energy ion irradiation

Organic nonlinear optical single crystals of Methyl para-Hydroxy Benzoate (MHB) have been grown using gel-solution technique. These crystals are cut along z-axis and are bombarded with Ag14+ ions of energy 100 MeV. The results show an increase in refractive index at the ion irradiated region. The dielectric constant of the irradiated crystal is increased more than 15 times compared to that of a nonirradiated crystal. The result of these changes and comparative study of second harmonic generation (SHG) efficiency before and after irradiation is discussed.

Simultaneous determination of nonlinear optical and thermo-optic parameters of liquid samples

The authors apply the theory of photothermal lens formation and also that of pure optical nonlinearity to account for the phase modulation in a beam as it traverses a nonlinear medium. It is used to simultaneously determine the nonlinear optical refraction and the thermo-optic coefficient. They demonstrate this technique using some metal phthalocyanines dissolved in dimethyl sulfoxide, irradiated by a Q-switched Nd:YAG laser with 10 Hz repetition rate and a pulse width of 8 ns. The mechanism for reverse saturable absorption in these materials is also discussed.

Spatial and time resolved analysis of CN bands in the laser induced plasma from graphite

Analysis of the emission bands of the CN molecules in the plasma generated from a graphite target irradiated with 1-06/~m radiation pulses from a Q-switched Nd:YAG laser has been done. Depending on the position of the sampled volume of the plasma plume, the intensity distribution in the emission spectra is found to change drastically. The vibrational temperature and population distribution in the different vibrational levels have been studied as function of distance from the target for different time delays with respect to the incidence of the laser pulse. The translational temperature calculated from time of flight is found to be higher than the observed vibrational temperature for CN molecules and the reason for this is explained.

Realization of a Scanning Photoacoustic Technique: Thermal properties of Bulk and Film Samples

Among the large number of photothcrmal techniques available, photoacoustics assumes a very significant place because of its essential simplicity and the variety of applications it finds in science and technology. The photoacoustic (PA) effect is the generation of an acoustic signal when a sample, kept inside an enclosed volume, is irradiated by an intensity modulated beam of radiation. The radiation absorbed by the sample is converted into thermal waves by nonradiative de-excitation processes. The propagating thermal waves cause a corresponding expansion and contraction of the gas medium surrounding the sample, which in tum can be detected as sound waves by a sensitive microphone. These sound waves have the same frequency as the initial modulation frequency of light. Lock-in detection method enables one to have a sufficiently high signal to noise ratio for the detected signal. The PA signal amplitude depends on the optical absorption coefficient of the sample and its thermal properties. The PA signal phase is a function of the thermal diffusivity of the sample.Measurement of the PA amplitude and phase enables one to get valuable information about the thermal and optical properties of the sample. Since the PA signal depends on the optical and thennal properties of the sample, their variation will get reflected in the PA signal. Therefore, if the PA signal is collected from various points on a sample surface it will give a profile of the variations in the optical/thennal properties across the sample surface. Since the optical and thermal properties are affected by the presence of defects, interfaces, change of material etc. these will get reflected in the PA signal. By varying the modulation frequency, we can get information about the subsurface features also. This is the basic principle of PA imaging or PA depth profiling. It is a quickly expanding field with potential applications in thin film technology, chemical engineering, biology, medical diagnosis etc. Since it is a non-destructive method, PA imaging has added advantages over some of the other imaging techniques. A major part of the work presented in this thesis is concemed with the development of a PA imaging setup that can be used to detect the presence of surface and subsmface defects in solid samples.Determination of thermal transport properties such as thermal diffusivity, effusivity, conductivity and heat capacity of materials is another application of photothennal effect. There are various methods, depending on the nature of the sample, to determine these properties. However, there are only a few methods developed to determine all these properties simultaneously. Even though a few techniques to determine the above thermal properties individually for a coating can be found in literature, no technique is available for the simultaneous measurement of these parameters for a coating. We have developed a scanning photoacoustic technique that can be used to determine all the above thermal transport properties simultaneously in the case of opaque coatings such as paints. Another work that we have presented in this thesis is the determination of thermal effusivity of many bulk solids by a scanning photoacoustic technique. This is one of the very few methods developed to determine thermal effiisivity directly.

Photoacoustic investigation of the optical and thermal properties of selected amorphous chalcogenide semiconductors

This thesis work has mainly concentrated on the investigation of the ,optical and thermal properties of binary semiconducting chalcogenide glasses belonging to the AivB¥5x and AZBXEX families. The technique used for these studies is a relatively new one namely, the photoacoustic (PA) technique. This technique is based on the detection of acoustic signal produced in an enclosed volume when the sample is irradiated by an intensity modulated radiation. The signal produced depends upon the optical properties of the sample, and the thermal properties of the sample, backing material and the surrounding gas. For the present studies an efficient signal beam gas-microphone PA spectrometer, consisting of a high power Xenon lamp, monochromator, light beam chopper, PA cell with microphone and lock-in amplifier, has been set up. Two PA cells have been fabricated: one for room temperature measurements and another for measurements at high temperatures. With the high temperature PA cell measurements can be taken upto 250°C. Provisions are incorporated. in both the cells to change the volume and to use different backing materials for the sample. The cells have been calibrated by measuring the frequency response of the cells using carbon black as the sample

Studies On The Effect Of Laser Radiation And Other Mutagens On Plants

The effect of lasers of three wavelengths in the visible region - 476, 488 and 514 nm on mitotic and meiotic cell divisions, growth, yield and activity of specific enzymes were studied in two taxonomically diverse plant species — A/lium cepa L. and Vicia faba. The effect of laser exposures was compared with the effect of two physical mutagens (Gamma and Ultraviolet radiations) and two chemical mutagens (Ethyl Methane Sulphonate and Hydroxyl amine). The study indicated that lasers could be mutagenic causing aberration in the mitotic and meiotic cell divisions while also producing changes in the growth and yield of the plants. Lasers of higher wavelengths 488 and 514 nm caused aberrations in the early stages of mitotic cell division whereas lasers of lower wavelengths (476 nm) caused more aberrations in the later stages of mitotic cell division. Laser exposure of 488 nm wavelength at power density 400 mW induced higher mitotic and meiotic aberrations and also induced higher pollen sterility than lasers of 476 and 514 nm. The frequency of mitotic aberrations induced by lasers was lesser than that caused by y-irradiation but comparable to that induced by EMS and HA. Lasers cause mutations in higher frequencies than UV. Lasers had a stimulatory effect on growth and yield in both plant species. This stimulatory effect of lasers on germination could not however be correlated to the activity of amylase and protease, the key enzymes in seed gennination. Enzymes such as peroxidase and catalase, involved in scavenging of free oxygen radicals often produced by irradiation, did not show increased activity in laser irradiated samples. Further studies are required for elucidating the exact mechanisms by which lasers cause mutations

Swift heavy ion induced surface modification for tailoring coercivity in Fe–Ni based amorphous thin films

Fe–Ni based amorphous thin films were prepared by thermal evaporation. These films were irradiated by 108 MeV Ag8+ ions at room temperature with fluences ranging from 1 1012 to 3 1013 ions/cm2 using a 15 UD Pelletron accelerator. Glancing angle x-ray diffraction studies showed that the irradiated films retain their amorphous nature. The topographical evolution of the films under swift heavy ion SHI bombardment was probed using atomic force microscope and it was noticed that surface roughening was taking place with ion beam irradiation. Magnetic measurements using a vibrating sample magnetometer showed that the coercivity of the films increases with an increase in the ion fluence. The observed coercivity changes are correlated with topographical evolution of the films under SHI irradiation. The ability to modify the magnetic properties via SHI irradiation could be utilized for applications in thin film magnetism

Photoluminescence studies on RF plasma-polymerized thin films

Conjugated polymers in the form of thin films play an important role in the field of materials science due to their interesting properties. Polymer thin films find extensive applications in the fabrication of devices, such as light emitting devices, rechargeable batteries, super capacitors, and are used as intermetallic dielectrics and EMI shieldings. Polymer thin films prepared by plasma-polymerization are highly cross-linked, pinhole free, and their permittivity lie in the ultra low k-regime. Electronic and photonic applications of plasma-polymerized thin films attracted the attention of various researchers. Modification of polymer thin films by swift heavy ions is well established and ion irradiation of polymers can induce irreversible changes in their structural, electrical, and optical properties. Polyaniline and polyfurfural thin films prepared by RF plasmapolymerization were irradiated with 92MeV silicon ions for various fluences of 1×1011 ions cm−2, 1×1012 ions cm−2, and 1×1013 ions cm−2. FTIR have been recorded on the pristine and silicon ion irradiated polymer thin films for structural evaluation. Photoluminescence (PL) spectra were recorded for RF plasma-polymerized thin film samples before and after irradiation. In this paper the effect of swift heavy ions on the structural and photoluminescence spectra of plasma-polymerized thin films are investigated.

Swift heavy ion induced surface and microstructural evolution in metallic glass thin films

Swift heavy ion induced changes in microstructure and surface morphology of vapor deposited Fe–Ni based metallic glass thin films have been investigated by using atomic force microscopy, X-ray diffraction and transmission electron microscopy. Ion beam irradiation was carried out at room temperature with 103 MeV Au9+ beam with fluences ranging from 3 1011 to 3 1013 ions/cm2. The atomic force microscopy images were subjected to power spectral density analysis and roughness analysis using an image analysis software. Clusters were found in the image of as-deposited samples, which indicates that the film growth is dominated by the island growth mode. As-deposited films were amorphous as evidenced from X-ray diffraction; however, high resolution transmission electron microscopy measurements revealed a short range atomic order in the samples with crystallites of size around 3 nm embedded in an amorphous matrix. X-ray diffraction pattern of the as-deposited films after irradiation does not show any appreciable changes, indicating that the passage of swift heavy ions stabilizes the short range atomic ordering, or even creates further amorphization. The crystallinity of the as-deposited Fe–Ni based films was improved by thermal annealing, and diffraction results indicated that ion beam irradiation on annealed samples results in grain fragmentation. On bombarding annealed films, the surface roughness of the films decreased initially, then, at higher fluences it increased. The observed change in surface morphology of the irradiated films is attributed to the interplay between ion induced sputtering, volume diffusion and surface diffusion