Far infrared reflectance and optical properties of organic superconductor (TMTSF)2ClO4 /

Polarized reflectance measurements of the quasi I-D charge-transfer salt (TMTSFh CI04 were carried out using a Martin-Puplett-type polarizing interferometer and a 3He refrigerator cryostat, at several temperatures between 0.45 K and 26 K, in the far infrared, in the 10 to 70 cm- 1 frequency range. Bis-tetramethyl-tetraselena-fulvalene perchlorate crystals, grown electrochemically and supplied by K. Behnia, of dimensions 2 to 4 by 0.4 by 0.2 mm, were assembled on a flat surface to form a mosaic of 1.5 by 3 mm. The needle shaped crystals were positioned parallel to each other along their long axis, which is the stacking direction of the planar TMTSF cations, exposing the ab plane face (parallel to which the sheets of CI04 anions are positioned). Reflectance measurements were performed with radiation polarized along the stacking direction in the sample. Measurements were carried out following either a fast (15-20 K per minute) or slow (0.1 K per minute) cooling of the sample. Slow cooling permits the anions to order near 24 K, and the sample is expected to be superconducting below 1.2 K, while fast cooling yields an insulating state at low temperatures. Upon the slow cooling the reflectance shows dependence with temperature and exhibits the 28 cm- 1 feature reported previously [1]. Thermoreflectance for both the 'slow' and 'fast' cooling of the sample calculated relative to the 26 K reflectance data indicates that the reflectance is temperature dependent, for the slow cooling case only. A low frequency edge in the absolute reflectance is assigned an electronic origin given its strong temperature dependence in the relaxed state. We attribute the peak in the absolute reflectance near 30 cm-1 to a phonon coupled to the electronic background. Both the low frequency edge and the 30 cm-1 feature are noted te shift towards higher frequcncy, upon cntering the superconducting state, by an amount of the order of the expected superconducting energy gap. Kramers-Kronig analysis was carried out to determine the optical conductivity for the slowly cooled sample from the measured reflectance. In order to do so the low frequency data was extrapolated to zero frequency using a Hagen-Ru bens behaviour, and the high frequency data was extended with the data of Cao et al. [2], and Kikuchi et al. [3]. The real part of the optical conductivity exhibits an asymmetric peak at 35 cm-1, and its background at lower frequencies seems to be losing spectral weight with lowering of the temperature, leading us to presume that a narrow peak is forming at even lower frequencies.

The infared optical properties of Sr2RuO4 and SmTiO3 including an object-oriented resistivity interface /

The perovskite crystal structure is host to many different materials from insulating to superconducting providing a diverse range of intrinsic character and complexity. A better fundamental description of these materials in terms of their electronic, optical and magnetic properties undoubtedly precedes an effective realization of their application potential. SmTiOa, a distorted perovskite has a strongly localized electronic structure and undergoes an antiferromagnetic transition at 50 K in its nominally stoichiometric form. Sr2Ru04 is a layered perovskite superconductor (ie. Tc % 1 K) bearing the same structure as the high-tem|>erature superconductor La2_xSrrCu04. Polarized reflectance measurements were carried out on both of these materials revealing several interesting features in the far-infrared range of the spectrum. In the case of SmTiOa, although insulating, evidence indicates the presence of a finite background optical conductivity. As the temperature is lowered through the ordering temperature a resonance feature appears to narrow and strengthen near 120 cm~^ A nearby phonon mode appears to also couple to this magnetic transition as revealed by a growing asymmetry in the optica] conductivity. Experiments on a doped sample with a greater itinerant character and lower Neel temperature = 40 K also indicate the presence of this strongly temperature dependent mode even at twice the ordering temperature. Although the mode appears to be sensitive to the magnetic transition it is unclear whether a magnon assignment is appropriate. At very least, evidence suggests an interesting interaction between magnetic and electronic excitations. Although Sr2Ru04 is highly anisotropic it is metallic in three-dimensions at low temperatures and reveals its coherent transport in an inter-plane Drude-like component to the highest temperatures measured (ie. 90 K). An extended Drude analysis is used to probe the frequency dependent scattering character revealing a peak in both the mass enhancement and scattering rate near 80 cm~* and 100 cm~* respectively. All of these experimental observations appear relatively consistent with a Fermi-liquid picture of charge transport. To supplement the optical measurements a resistivity station was set up with an event driven object oriented user interface. The program controls a Keithley Current Source, HP Nano-Voltmeter and Switching Unit as well as a LakeShore Temperature Controller in order to obtain a plot of the Resistivity as a function of temperature. The system allows for resistivity measurements ranging from 4 K to 290 K using an external probe or between 0.4 K to 295 K using a Helium - 3 Cryostat. Several materials of known resistivity have confirmed the system to be robust and capable of measuring metallic samples distinguishing features of several fiQ-cm.

Far infrared optical properties of V and Cr doped Sb2Te3 /

The far infrared reflectance of Sb2Te3 , Sbi.97Vo.o3Te3 and Sbi.94Cr .o6Te3 was measured near normal incidence at different temperatures (between 45K and 300K). The direct current resistivities of the above samples were also measured between the temperatures of 4K and 300K. Also Kramers Kronig (KK) analyses were performed on the reflectance spectra to obtain the optical conductivities. In the doped samples, it was observed that a phonon at 62cm-1 softens to about 55cm-1 on decreasing the temperature from 295K to 45K. Also, it was observed that the plasma frequency of the doped samples is independent of doping. The scattering rate for the vanadium doped sample was seen to be greater than that for the chromium doped sample despite the fact that vanadium impurity density is less than that of chromium. The Drude-Lorentz model fits to the KK optical conductivity show that the samples used in this work are conventional metals. Definitive measurements of the temperature dependence of the scattering rate across the ferromagnetic transition await equipment changes allowing measurements at low temperature using the mercury cadmium telluride (MCT) detector.

Crystal growth, Raman scattering and optical properties of the superconductor Cd2Re2O7(16O, 18O)/

Using the Physical Vapor Transport method, single crystals of Cd2Re207 have been grown, and crystals of dimensions up to 8x6x2 mm have been achieved. X-ray diffraction from a single crystal of Cd2Re207 has showed the crystal growth in the (111) plane. Powder X-ray diffraction measurements were performed on ^^O and ^^O samples, however no difference was observed. Assigning the space group Fd3m to Cd2Re207 at room temperature and using structure factor analysis, the powder X-ray diffraction pattern of the sample was explained through systematic reflection absences. The temperatiure dependence of the resistivity measurement of ^^O has revealed two structural phase transitions at 120 and 200 K, and the superconducting transition at 1.0 K. Using Factor Group Analysis on three different structiures of Cd2Re207, the number of IR and Raman active phonon modes close to the Brillouin zone centre have been determined and the results have been compared to the temperature-dependence of the Raman shifts of ^^O and ^*0 samples. After scaling (via removing Bose-Einstein and Rayleigh scattering factors from the scattered light) all spectra, each spectrum was fitted with a number of Lorentzian peaks. The temperature-dependence of the FWHM and Raman shift of mode Eg, shows the effects of the two structurjil phase transitions above Tc. The absolute reflectance of Cd2Re207 - '^O single crystals in the far-infrared spectral region (7-700 cm~^) has been measured in the superconducting state (0.5 K), right above the superconducting state (1.5 K), and in the normal state (4.2 K). Thermal reflectance of the sample at 0.5 K and 1.5 K indicates a strong absorption feature close to 10 cm~^ in the superconducting state with a reference temperature of 4.2 K. By means of Kramers-Kronig analysis, the absolute reflectance was used to calculate the optical conductivity and dielectric function. The real part of optical conductivity shows five distinct active phonon modes at 44, 200, 300, 375, and 575 cm~' at all temperatures including a Drude-like behavior at low frequencies. The imaginary part of the calculated dielectric function indicates a mode softening of the mode 44 cm~' below Tc.

An analysis of decoupling procedures in generating thermal Green's functions of O([lambda]â ´) by the Zubarev equation of motion method

The Zubarev equation of motion method has been applied to an anharmonic crystal of O( ,,4). All possible decoupling schemes have been interpreted in order to determine finite temperature expressions for the one phonon Green's function (and self energy) to 0()\4) for a crystal in which every atom is on a site of inversion symmetry. In order to provide a check of these results, the Helmholtz free energy expressions derived from the self energy expressions, have been shown to agree in the high temperature limit with the results obtained from the diagrammatic method. Expressions for the correlation functions that are related to the mean square displacement have been derived to 0(1\4) in the high temperature limit.

Magnetic and high pressure studies in the YPd5B3C3 system

The macroscopic properties of the superconducting phase in the multiphase compound YPd5B3 C.3 have been investigated. The onset of superconductivity was observed at 22.6 K, zero resistance at 21.2 K, the lower critical field Hel at 5 K was determined to be Hel (5) rv 310 Gauss and the compound was found to be an extreme type-II superconductor with the upper critical field in excess of 55000 Gauss at 15 K. From the upper and lower critical field values obtained, several important parameters of the superconducting state were determined at T = 15 K. The Ginzburg-Landau paramater was determined to be ~ > 9 corresponding to a coherence length ~ rv 80A and magnetic penetration depth of 800A. In addition measurements of the superconducting transition temperature Te(P) under purely hydrostatically applied pressure have been carried out. Te(P) of YPd5B3 C.3 decreases linearly with dTe/dP rv -8.814 X 10-5 J

On the equation of state and atomic mean square displacement of crystals

We have presented a Green's function method for the calculation of the atomic mean square displacement (MSD) for an anharmonic Hamil toni an . This method effectively sums a whole class of anharmonic contributions to MSD in the perturbation expansion in the high temperature limit. Using this formalism we have calculated the MSD for a nearest neighbour fcc Lennard Jones solid. The results show an improvement over the lowest order perturbation theory results, the difference with Monte Carlo calculations at temperatures close to melting is reduced from 11% to 3%. We also calculated the MSD for the Alkali metals Nat K/ Cs where a sixth neighbour interaction potential derived from the pseudopotential theory was employed in the calculations. The MSD by this method increases by 2.5% to 3.5% over the respective perturbation theory results. The MSD was calculated for Aluminum where different pseudopotential functions and a phenomenological Morse potential were used. The results show that the pseudopotentials provide better agreement with experimental data than the Morse potential. An excellent agreement with experiment over the whole temperature range is achieved with the Harrison modified point-ion pseudopotential with Hubbard-Sham screening function. We have calculated the thermodynamic properties of solid Kr by minimizing the total energy consisting of static and vibrational components, employing different schemes: The quasiharmonic theory (QH), ).2 and).4 perturbation theory, all terms up to 0 ().4) of the improved self consistent phonon theory (ISC), the ring diagrams up to o ().4) (RING), the iteration scheme (ITER) derived from the Greens's function method and a scheme consisting of ITER plus the remaining contributions of 0 ().4) which are not included in ITER which we call E(FULL). We have calculated the lattice constant, the volume expansion, the isothermal and adiabatic bulk modulus, the specific heat at constant volume and at constant pressure, and the Gruneisen parameter from two different potential functions: Lennard-Jones and Aziz. The Aziz potential gives generally a better agreement with experimental data than the LJ potential for the QH, ).2, ).4 and E(FULL) schemes. When only a partial sum of the).4 diagrams is used in the calculations (e.g. RING and ISC) the LJ results are in better agreement with experiment. The iteration scheme brings a definitive improvement over the).2 PT for both potentials.

Pressure dependence of spin fluctuations in metallic glasses Zrâ â Niâ â ,Zrâ â (Nix/Feâ â â -x)â â and /Zrx/feâ â â -x

The superconducting transition temperature Tc of metallic glasses ZrxFelOO-x (x=80, 75), Zr75(NixFelOO-x)25 (x=75, 50, 25), and CU2SZr75 were measured under quasi-hydrostatic pressure up to 8 OPa (80kbar). The volume (pressure) dependence of the electron-phonon coupling parameters Aep for CU25Zr75 was calculated using the McMillan equatio11. Using this volume dependence of Aep and the modified McMillan equation which incorporates spin-fluctuations, the volume dependence of the spin fluctuation parameter, Asf, was determined in Zr75Ni25, ZrxFelOO-x , a11d Zr75(NixFelOO-x)25. It was found that with increasing pressure, spinfluctuations are suppressed at a faster rate in ZrxFe lOO-x and Zr75(NixFelOO-x)25, as Fe concentration is increased. The rate of suppression of spin-fluctuations with pressure was also found to be higher in Fe-Zr glasses than in Ni-Zr glasses of similar composition.

Thermodynamic properties and Debye-Waller factor of fee materials

We have calculated the equation of state and the various thermodynamic properties of monatomic fcc crystals by minimizing the Helmholtz free energy derived in the high temperature limit for the quasiharmonic theory, QH, and the lowest-order (cubic and quartic), 'A2, anharmonic terms of the perturbation theory, PT. The total energy in each case is obtained by adding the static energy. The calculation of the thermal properties was carried out for a nearest-neighbour central-force model of the fcc lattice by means of the appropriate thermodynamic relations. We have calculated the lattice constant, the thermal expansion, the coefficient of volume expansion, the specific heat at constant volume and at constant pressure, the isothermal and adiabatic bulk moduli, and the Griineisen parameter, for the rare-gas solids Kr and Xe, and gold. Morse potential and modified Morse potential were each used to represent the atomic interaction for the three fcc materials. For most of the calculated thermodynamic properties from the QH theory, the results for Kr and Xe with the modified Morse potential show an improvement over the results for the Morse potential when compared with the experimental data. However, the results of the 'A 2 equation of state with the modified Morse potential are in good agreement with experiment only in the case of the specific heat at constant volume and at constant pressure. For Au we have calculated the lattice contribution from the QH and 'A 2 PT and the electronic contribution to the thermal properties. The electronic contribution was taken into account by using the free electron model. The results of the thermodynamic properties calculated with the modified Morse potential were similar to those obtained with the Morse potential. U sing the minimized equation of state we also calculated the Mossbauer recoilless fraction for Kr and Xe and the Debye-Waller factor (DWF) for Pb, AI, eu, Ag, and Au. The Mossbauer recoilless fraction was obtained for the above two potentials and Lennard-Jones potential. The L-J potential gives the best agreement with experiment for Kr. No experimental data exists for Xe. At low temperature the calculated DWF results for Pb, AI, and eu show a good agreement with experimental values, but at high temperature the experimental DWF results increase very rapidly. For Ag the computed values were below the expected results at all temperatures. The DWF results of the modified Morse potential for Pb, AI, eu and Ag were slightly better than those of the Morse potential. In the case of Au the calculated values were in poor agreement with experimental results. We have calculated the quasiharmonic phonon dispersion curves for Kr, Xe, eu, Ag, and Au. The calculated and experimental results of the frequencies agree quite well for all the materials except for Au where the longitudinal modes show serious discrepancies with the experimental results. In addition, the two lowest-order anharmonic contributions to the phonon frequency were derived using the Green's function method. The A 2 phonon dispersion curves have been calculated only for eu, and the results were similar to those of the QH dispersion curves. Finally, an expression for the Griineisen parameter "( has been derived from the anharmonic frequencies, and calculated for these materials. The "( results are comparable with those obtained from the thermodynamic definition.

Pressure dependence of superconducting properties of MgB2 /

We prepared samples of MgB2 and ran sets of experiments aimed for investigation of superconducting properties under pressure. We found the value of pressure derivative of the transition temperature -1.2 ± 0.05 K/GPa. Then, using McMillan formula, we found that the main contribution to the change of the transition temperature under the pressure is due to the change in phonon frequencies. Griineisen parameter was calculated to be 7g = 2.4. Our results suggest that MgB2 is a conventional superconductor.

The design of a reflectance spectrometer and its calibration using SrTiO3 /

A new Ultra-High Vacuum (UHV) reflectance spectrometer was successfully designed, making use of a Janis Industries ST-400 sample cryostat, IR Labs bolometer, and Briiker IFS 66 v/S spectrometer. Two of the noteworthy features include an in situ gold evaporator and internal reference path, both of which allow for the experiment to progress with a completely undisturbed sample position. As tested, the system was designed to operate between 4.2 K and 325 K over a frequency range of 60 - 670 cm~^. This frequency range can easily be extended through the addition of appUcable detectors. Tests were performed on SrTiOa, a highly ionic incipient ferroelectric insulator with a well known reflectance. The presence and temperatmre dependence of the lowest frequency "soft" mode were measured, as was the presence of the other two infrared modes. During the structural phase transition from cubic to tetragonal perovskite, the splitting of the second phonon mode was also observed. All of the collected data indicate good agreement with previous measurements, with a minor discrepency between the actual and recorded sample temperatures.

Optical Properties of Sb2Te3, and Dilute Magnetic Semiconductors Sb1.97 VO.03 Te3 and Sb1.94 CrO.06 Te3

This thesis reports on the optical properties of the dilute magnetic semiconductors, Sb1.97 V 0.03 Te3 and Sb1.94Cr0.06Te3, along with the parent compound Sb2Te3' These materials develop a ferromagnetic state at low temperature with Curie temperatures of 22 K and 16 K respectively. All three samples were oriented such that the electric field vector of the light was perpendicular to the c-axis. The reflectance profile of these samples in the mid-infrared (500 to 3000 cm-1) shows a pronounced plasma edge which retracts with decreasing temperature. The far-infrared region of these samples exhibits a phonon at ~ 60 cm-1 which softens as temperature decreases. Kramers-Kronig analysis and a Drude-Lorentz model were employed to determine the optical constants of the bulk samples. The real part of the optical conductivity is shown to consist of intraband contributions at frequencies below the energy gap (~0.26 eV) and interband contributions at frequencies above the energy gap. The temperature dependence of the scattering rate show that a mix of phonon and impurity scattering are present, while the signature of traditional spin disorder (magnetic) scattering was difficult to confirm.

Interactions protéiques et relation dynamique entre phosphorylation / sumoylation / ubiquitination des protéines TIF1α, β et PML: détection in vivo par BRET

Trois protéines de la famille TRIM (Motif TRIpartite), TIF1α, β (Transcriptional Intermediary Factor 1) et PML (ProMyelocytic Leukaemia¬), font l’objet de cette étude. TIF1α est connu comme un coactivateur des récepteurs nucléaires et TIF1β comme le corépresseur universel des protéines KRAB-multidoigt de zinc dont le prototype étudié ici est ZNF74. PML possède divers rôles dont le plus caractérisé est celui d’être l’organisateur principal et essentiel des PML-NBs (PML-Nuclear Bodies), des macrostructures nucléaires très dynamiques regroupant et coordonnant plus de 40 protéines. Il est à noter que la fonction de TIF1α, β et PML est régulée par une modification post-traductionnelle, la sumoylation, qui implique le couplage covalent de la petite protéine SUMO (Small Ubiquitin like MOdifier) à des lysines de ces trois protéines cibles. Cette thèse propose de développer des méthodes utilisant le BRET (Bioluminescence Resonance Energy Transfert) afin de détecter dans des cellules vivantes et en temps réel des interactions non-covalentes de protéines nucléaires mais aussi leur couplage covalent à SUMO. En effet, le BRET n’a jamais été exploré jusqu’alors pour étudier les interactions non-covalentes et covalentes de protéines nucléaires. L’étude de l’interaction de protéines transcriptionnellement actives est parfois difficile par des méthodes classiques du fait de leur grande propension à agréger (famille TRIM) ou de leur association à la matrice nucléaire (ZNF74). L’homo et l’hétérodimérisation de TIF1α, β ainsi que leur interaction avec ZNF74 sont ici testées sur des protéines entières dans des cellules vivantes de mammifères répondant aux résultats conflictuels de la littérature et démontrant que le BRET peut être avantageusement utilisé comme alternative aux essais plus classiques basés sur la transcription. Du fait de l’hétérodimérisation confirmée de TIF1α et β, le premier article présenté ouvre la possibilité d’une relation étroite entre les récepteurs nucléaires et les protéines KRAB- multidoigt de zinc. Des études précédentes ont démontré que la sumoylation de PML est impliquée dans sa dégradation induite par l’As2O3 et dépendante de RNF4, une E3 ubiquitine ligase ayant pour substrat des chaînes de SUMO (polySUMO). Dans le second article, grâce au développement d’une nouvelle application du BRET pour la détection d’interactions covalentes et non-covalentes avec SUMO (BRETSUMO), nous établissons un nouveau lien entre la sumoylation de PML et sa dégradation. Nous confirmons que le recrutement de RNF4 dépend de SUMO mais démontrons également l’implication du SBD (Sumo Binding Domain) de PML dans sa dégradation induite par l’As2O3 et/ou RNF4. De plus, nous démontrons que des sérines, au sein du SBD de PML, qui sont connues comme des cibles de phosphorylation par la voie de la kinase CK2, régulent les interactions non-covalentes de ce SBD mettant en évidence, pour la première fois, que les interactions avec un SBD peuvent dépendre d’un évènement de phosphorylation (“SBD phospho-switch”). Nos résultats nous amènent à proposer l’hypothèse que le recrutement de PML sumoylé au niveau des PML-NBs via son SBD, favorise le recrutement d’une autre activité E3 ubiquitine ligase, outre celle de RNF4, PML étant lui-même un potentiel candidat. Ceci suggère l’existence d’une nouvelle relation dynamique entre phosphorylation, sumoylation et ubiquitination de PML. Finalement, il est suggéré que PML est dégradé par deux voies différentes dépendantes de l’ubiquitine et du protéasome; la voie de CK2 et la voie de RNF4. Enfin une étude sur la sumoylation de TIF1β est également présentée en annexe. Cette étude caractérise les 6 lysines cibles de SUMO sur TIF1β et démontre que la sumoylation est nécessaire à l’activité répressive de TIF1β mais n’est pas impliquée dans son homodimérisation ou son interaction avec la boîte KRAB. La sumoylation est cependant nécessaire au recrutement d’histones déacétylases, dépendante de son homodimérisation et de l’intégrité du domaine PHD. Alors que l’on ne connaît pas de régulateur physiologique de la sumoylation outre les enzymes directement impliquées dans la machinerie de sumoylation, nous mettons en évidence que la sumoylation de TIF1β est positivement régulée par son interaction avec le domaine KRAB et suggérons que ces facteurs transcriptionnels recrutent TIF1β à l’ADN au niveau de promoteur et augmentent son activité répressive en favorisant sa sumoylation.

Étude du comportement électromécanique du ventricule gauche canin sous différents modes de stimulation

La thérapie de resynchronisation cardiaque (CRT) est un traitement qui diminue la mortalité et améliore la qualité de vie des patients atteints d’insuffisance cardiaque et présentant un dyssynchronisme de la contraction ventriculaire gauche. Malgré le succès de cette thérapie, plus de 30% des patients ne présentent pas l’amélioration désirée. Plusieurs études portant sur le synchronisme électrique ou mécanique de la contraction ont été effectuées mais peu d’entres elles se sont attardées sur le couplage électromécanique à l'échelle macroscopique. Ce projet a comme objectif d’observer le comportement électromécanique des ventricules canins en présence d’un resynchronisateur cardiaque. Un logiciel a été développé pour permettre l’analyse des informations provenant de la cartographie endocardique sans contact et de la ventriculographie isotopique tomographique chez 12 sujets canins insuffisants. Pour observer la réponse mécanique suite à l’activation électrique, nous avons premièrement recalé les surfaces issues des 2 modalités. Ensuite, nous avons défini les limites du cycle cardiaque, analysé les signaux électriques et les courbes de déplacement de la paroi endocardique. Le début de la contraction est défini par un déplacement radial de 10% vers le centre du ventricule. Les résultats démontrent que la durée d’activation du ventricule gauche et la largeur du QRS augmentent en présence d’une stimulation externe et que les délais électromécaniques sont indépendants dans les modes de stimulation étudiés (sinusal, LVbasal, RVapex ou BIV) avec une moyenne de 84,56±7,19 ms. Finalement, nous avons noté que la stimulation basolatérale procure une fonction cardiaque optimale malgré une durée prolongée du QRS.

Rôle de l’extrémité C-terminale dans l’expression du canal calcique Cav1.2 à la membrane plasmique

Le canal calcique de type L, Cav1.2, joue un rôle clé dans le couplage excitation-contraction des myocytes ventriculaires. Il a été montré que la sous-unité Cavα1 était sujette à l’épissage alternatif et que ce phénomène pouvait mener à une protéine tronquée en C-terminal au niveau de l’exon 45 (Liao, Yong et al. 2005). D’autres groupes ont étudié différentes délétions au niveau de l’extrémité C-terminale (De Jongh, Warner et al. 1991; Gao, Cuadra et al. 2001). Les courants mesurés dans la configuration cellule entière, était significativement plus grands que le canal « pleine longueur ». Nous avons décidé de tester certaines de ces délétions (ΔC2030, ΔC1935, ΔC1856, ΔC1733, ΔC1700) en présence ou en absence de la sous-unité auxiliaire Cavβ3, susceptible d’interagir avec l’extrémité C-terminale de la sous-unité Cavα1 par l’intermédiaire de son domaine SH3 (Lao, Kobrinsky et al. 2008). Les résultats obtenus dans les ovocytes de Xénope ont mis en évidence que les sous-unités Cavα1.2 tronquées montraient des courants globaux plus élevés que le canal « pleine longueur » en présence de la sous-unité auxiliaire Cavβ3 et que les sous-unités Cavα1.2 tronquées donnaient des courants en absence de la sous-unité Cavβ3 contrairement à la sous-unité Cavα1.2 « pleine longueur ». Afin de vérifier si l’augmentation des courants macroscopiques était le résultat d’une augmentation du nombre de sous-unités Cavα1.2 à la membrane, nous avons choisi de quantifier la fluorescence spécifiquement due à cette sous-unité en utilisant la méthode de cytométrie de flux (FACS : « Fluorescence Activated Cell Sorting »). L’épitope HA a été inséré dans une région extracellulaire de la sous-unité Cavα1 du canal calcique Cav1.2 et un anticorps anti-HA couplé au FITC (« Fluorescein IsoThioCyanate ») a été utilisé pour observer la fluorescence. Nos résultats confirment que la sous-unité Cavα1-HA du canal calcique Cav1.2, s’exprime à la membrane plasmique en présence de la sous-unité auxiliaire Cavβ3, et qu’en absence de celle-ci, ne s’exprime que peu ou pas à la membrane. Les mêmes résultats ont été obtenus pour les trois délétions testées dans les mêmes conditions soit Cavα1.2-HA ΔC1935, Cavα1.2-HA ΔC1856 et Cavα1.2-HA ΔC1733. Ensemble, ces résultats suggèrent que l’augmentation des courants macroscopiques observés après une délétion partielle du C-terminal n’est pas causée par une augmentation du nombre de protéines Cavα1.2 à la membrane.