Graphite is the strongest diamagnet of all known materials to date. Recent studies of the thickness dependence of the resistance of graphite have demonstrated the heterogeneity of the charge distribution in bulk graphite and prompted the study of its magnetic properties. The studies of the thickness dependence of the magnetic susceptibility of graphite, done in this work, showed that two-dimensional interfaces between the crystalline (Bernal or rhombohedral stacking order) blocks in graphite make a dominant contribution to its diamagnetic susceptibility. Previously proposed models of diamagnetism in graphite are not suitable for explaining its magnetic properties, and therefore new concepts should be considered. Additionally, the studies of the transport and magnetic properties of graphite and multilayer graphene indicated the existence of superconductivity at the interfaces in well-ordered graphite. The possibility of creating permanent circulating currents around artificial holes in highly oriented graphite was studied by highly sensitive magnetization measurements. The obtained results provide hints for the possible existence of superconducting regions inside the bulk highly ordered graphite. In the present thesis, a further thickness dependent phenomenon on the depinning line (DL) of the flux line lattice of the high-Tc superconductor Bi2Sr2CaCu2O8+δ was studied. This geometrical effect shifts to notably lower temperatures in micrometer ring, compared with bulk crystals and thin flakes. The shift is related to a decrease in the overall pinning potential as a result of size effects, caused by: a) the thickness of the sample being smaller than the pinning correlation length, and b) the increase in the effective London penetration depth of the vortices (Pearl vortices). The large shift of the DL to lower temperatures may significantly influence the suitability of such elements for device applications in microstrip antennas and THz emitters.

The Bi2Sr2CaCu2O7+d, i.e. Bi2212 phase of bismuth derived high temperature superconductors (HTS), powder precursor were synthesized via sol – gel technique using ethylendiamintetraacetic acid (Chelaton II) as a chelating agent. Metal nitrate’s solutions were mixed with EDTA suspension. The pH value was adjusted to 9 by NH4OH by reason forming of stable metal’s complexes. The mixture was heated to 80 °C for gelation. Solution taken before solid gel was form is used for preparation of Bi2212 layer on to a-Al2O3 surface via spin coating deposition’s technique. Reactive powder used for bulk sample preparation was made by calcination (800 °C) of pyrolyzed xerogel (500 °C). Sintering in oxygen atmosphere was proceeding at temperature from 850 to 880 °C. Bulk sample properties were compared with sample prepared by common ceramic method. Simultaneous TG-DTA, IR spectroscopy and heating microscopy were used for sample characterization. Furthermore, construction of furnace for sintering in O2 atmosphere was described.

High-temperature superconductors belong to the group of strongly correlated materials. In these compounds, complex repulsive electron interactions and a large number of degrees of freedom lead to a rich variety of states of matter. Exotic phases like the pseudogap, charge-, spin- and pair-density waves, but also the remarkable phenomenon of superconductivity emerge, depending on doping level and temperature. However, up to now it is unclear what exactly causes these states, to what extent they are coexisting or competing, and where their borders in the phase diagram lie. A better understanding could help in finding the mechanism behind high-temperature superconductivity, but would also provide a better insight into the puzzling behavior of strongly correlated materials. This thesis tries to resolve some of these questions with focus on the underdoped pseudogap regime. Mesa structures of bismuth-based cuprate superconductors were studied using intrinsic tunneling, which allows spectroscopic characterizations of electronic density of states inside the material. A micro/nano fabrication method was developed to further reduce mesa areas into the sub square-micrometer range, in order to minimize the effect of crystal defects and measurement artifacts caused by heating induced by the measurement current. The comparison of energy scales in Bi-2201 and Bi-2212 cuprates shows that the pseudogap phenomenon is not connected to superconductivity, but possibly represents a competing spin-singlet order that is universal to all cuprates. The analysis of the upper critical field in Bi-2201 reveals a low anisotropy, which gives evidence of paramagnetically limited superconductivity. Furthermore, a new electrical doping method is demonstrated, which enables the reversible tuning the doping level of Bi-2212 and study a broad doping range upon a single sample. Using this method, two distinct critical points were observed under the superconducting dome in the phase diagram: one at the overdoped side, associated with the onset of the pseudogap and a metal to insulator transition, and one at optimal doping, associated with an enhanced "dressed" electron energy. Finally, a novel angular-dependent magnetotunneling technique is introduced, which allows for the separation of the superconducting and non-superconducting contributions to the pseudogap phenomenon. The method reveals that after an abrupt decay of the energy gap for T→Tc, weak superconducting correlations persist up to several tens of degrees above Tc.

Dans le contexte d'un contrat de la Délégation Générale pour l'Armement (DGA) avec la société Nexans, le CRTBT-CNRS a développé une bobine supraconductrice de stockage d'énergie, ou SMES Superconducting Magnetic Energy Storage), avec des rubans PIT Bi-2212 pour un fonctionnement à 20 K. L'utilisation d'un bobinage supraconducteur permet de stocker l'énergie électrique sous forme magnétique sans conversion d'énergie, ceci pendant des temps très longs. Le bobinage stocke 800!kJ à décharger en 1 s pour atteindre une puissance de 500 kW sur la charge, ce qui génère une tension maximale de 5 kV. La cryogénie est réalisée avec des pièces en cuivre qui relient les cryoréfrigérateurs et le bobinage, avec différence de température de 2 K au maximum. L'interface HT (Haute Tension) entre les drains et le bobinage a une tenue diélectrique de 5 kV et permet de refroidir efficacement les amenées de courant et les 26 galettes, soit 40 km de ruban. L'énergie dissipée dans le cuivre et le bobinage pendant la décharge représente 1 l'énergie stockée. Des mesures thermiques à 20 K ont été réalisées sur des échantillons pour mesurer l'interface!HT par exemple, puis sur un bobinage de dimensions réduites pour valider les solutions retenues. Le procédé de coétamage des rubans supraconducteurs développés par Nexans permet d'adapter la géométrie du conducteur à sa situation dans le bobinage. Les essais des dix premières galettes bobinées a validé la cryogénie développée. L'étude d'extrapolation pour un SMES de 20 MJ présente une géométrie torique adaptée à un refroidissement par thermosiphon avec un câble bi-étagé Rutherford / 6+1 en fils ronds de Bi-2212.

Dans ce mémoire, nous avons approché l'étude du diagramme de phase (T,p) des cuprates à travers l'étude des effets du dopage sur les propriétés électroniques de deux systèmes La2-xSrxCuO4 et Bi2Sr2Ca1-xYxCu2-yZnyO8+d.  Dans un premier temps, la conductivité optique de deux échantillons La2-xSrxCuO4 a été analysée, dans les plans et perpendiculairement aux plans : un composé sous-dopé (x = 0,08) et le composé optimalement dopé (x = 0,15). Suivant l'axe c et à faibles fréquences, nous avons observé une diminution de la conductivité optique en diminuant la température pour l'échantillon sous-dopé. Dans les plans et pour le même composé, nous avons montré que le taux de diffusion diminuait et que la masse effective augmentait, lorsque la température diminue et à faibles fréquences. Puisque ces résultats ne sont obtenus que sur l'échantillon sous-dopé, ils peuvent correspondre à une signature de la phase de pseudo-gap.<br /> Dans le but de comparer et d'étudier le comportement du cuprate Bi-2212, nous avons synthétisé des échantillons de composition Bi2Sr2Ca1-xYxCu2-yZnyO8+d. La substitution à l'yttrium modifie la concentration des porteurs et la substitution au zinc conduit à la suppression de la supraconductivité. Nous avons d'abord analysé des échantillons céramiques. Deux voies d'élaboration ont été confrontées : la voie solide et la voie citrate modifiée. Cette dernière a montré une meilleure cristallinité et un caractère monophasé des poudres, caractéristiques importantes pour la croissance cristalline. Les mesures de transport ont montré que les céramiques évoluaient d'un régime métallique vers un comportement semi-conducteur, à haute température, en fonction de la substitution à l'yttrium mais également au zinc.<br /> Finalement, nous nous sommes intéressés à la croissance de monocristaux de Bi2Sr2Ca1-xYxCu2-yZnyO8+d dans un four à image. Les expériences ont montré que la croissance était délicate. Après avoir optimisé les paramètres de la fusion pour la composition non-dopée, nous avons fait croître des monocristaux de taille 15 x 5 x 0,2 mm3. Pour les substitutions, l'yttrium empêche la croissance de larges monocristaux qui n'excèdent pas la taille de 3 x 1,5 x 0,2 mm3. La limite de solubilité du zinc sur site cuivre a été définie à 0,03. A partir de ces résultats, des monocristaux de composition Bi1,99Sr2,01Ca0,76Y0,3Cu1,9Zn0,03O8+d ont été synthétisés et caractérisés.

In this thesis, the tunneling between individual atomic layers in structures of Bi2Sr2CaCu2O8+x based high-temperature superconductors are experimentally studied employing the intrinsic Josephson effect. A special attention is paid to the fabrication of small mesa structures using micro and nanofabrication techniques. In the first part of the thesis, the periodic Fraunhofer-like modulation of the critical current of the junctions as a function of in-plane magnetic field is investigated. A transition from a modulation with a half flux quantum to a flux quantum periodicity is demonstrated with increasing field and decreasing junction length. It is interpreted in terms of the transformation of the static fluxon lattice of stacked, strongly coupled intrinsic Josephson junctions and compared with theoretical predictions. A fluxon phase diagram is constructed.Numerical simulations have been carried out to complement the experimental data. In the second part of the thesis, different resonant phenomena are studied in the dynamic flux-flow state at high magnetic fields, including Eck-resonances and Fiske steps. Different resonant modes and their velocities, including superluminal modes, are identified. In the third part, different experiments attempting to detect radiation from small mesa structures using different setups based on hot-electron bolometer mixers and calorimeters are described. No distinct radiation with emission powers higher than about 500pW could be detected. Furthermore, the interaction with external GHz-radiation is studied. Resonances attributed to an induced flux-flow are observed, and the reflectivity of the sample can be tuned by switching mesas between the superconducting and quasiparticle state. In the last part, the resistive switching of mesas at high bias is studied. It is attributed to a persistent electrical doping of the crystal. Superconducting properties such as the critical current and temperature and the tunneling spectra are analyzed at different doping states of the same sample. The dynamics of the doping is studied, and attributed to two mechanisms; a charge-transfer effect and oxygen reordering