In recent years, BiFeO3 (BFO) has attracted much attention due to that exhibits ferroelectric and antiferromagnetic properties at room temperature. It potentially develops the spintronics and multiple-state memories. BFO suffered from serious leakage, therefore the BFO discussed in this report has doped 10% Pb to reduce the leakage problem. The thin films are synthesized by radio frequency (RF) sputtering technique. The conductive SrRuO3 (SRO) thin film is deposited on the SrTiO3 (STO) substrate as a buffer layer and bottom electrode for piezoelectric measurements and subsequently deposited the multiferroics- BFO thin film. Atomic force microscopy (AFM) and piezoresponse force microscopy (PFM) are used to observe the morphologies and domain images in nanometer scale by different parameters and avoid the disturbance of leakage reasonably. The variations of piezoelectric properties through grain-grain boundary and domain-domain boundary are also studied in this report.

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In recent years, multiferroics was one of the most popular materials and were widely studied by many scientists. Among all we interested the most is BiFeO3, which exist a room temperature ferromagnetic and ferroelectric properties with high ferromagnetic transition temperature Tc that can provide various kind of applications. However, the drawback of the BiFeO3 is difficult to synthesize the pure phase and to eliminate the leakage of the current. According to others¡¦ reports, with a proper doping can reduce the evaporation of Bi atoms and stabilize the crystal structure. Therefore, we choose Pb as the mixed elements and wish to reduce the unstable oxygen vacancies around the Bi atoms and to increase the dielectric property of Bi1-xPbxFeO3. In our experiment, SrRuO3 is chosen as the buffer layer material, which can grow as a strain relaxed film on the substrate. It is found that the strain relaxation transforms the SrRuO3 crystal structure to a nearly cubic one which has a lattice matching with Bi1-xPbxFeO3. As a result of this, we might improve the leakage problems of Bi1-xPbxFeO3.

Rhombohedral perovskite BiFeO3 is a single phase multiferroic compound exhibiting both magnetic (Neel temperature ~370˚C) and ferroelectric (Curie point ~840˚C) ordering well above the room temperature. Ferroelectricity in BiFeO3 is due to stereochemically active 6slone pair in Biion which causes large relative displacements of Bi and O ions along the [111] direction. Long range spiral modulation of the canted antiferromagnetic spin arrangement in Feeffectively cancels the macroscopic magnetization due to Dzyaloshinskii–Moriya interaction and thereby prevents linear magneto-electric effect. Synthesizing dense pure BiFeO3 by conventional solid state method is difficult due to the formation of thermodynamically stable secondary phases such as Bi2Fe4O9, Bi25FeO39 and Bi46Fe2O72. To stabilize the perovskite phase and to suppress the cycloid several groups have adopted different strategies such as thin film growth, different synthesis methods and chemical substitution. Of the various substitutions reported in the literature, PbTiO3 substitution has shown very interesting features, such as (i) unusually large tetragonality (c/a~1.19), (ii) formation of morphotropic phase boundary (MPB) and (iii) high curie point Tc~650C. MPB ferroelectric systems such as lead zirconate titanate (PZT) are known to exhibit high piezoelectric response due to the coupling between strain and polarization. Hence the existence of magnetic ordering in BiFeO3-PbTiO3 offers an interesting scenario where polarization, strain and magnetization may couple together. The high Curie point also makes the system an interesting candidate for high temperature piezoelectric application. However its potential as a high temperature piezoelectric material has not been realized yet. A detailed review of literature suggests a lack of clear agreement with regards to the composition range of the reported MPB itself. Different research groups have reported different composition range of MPB for this system even for almost similar synthesis conditions. The present thesis deals with broadly two parts, firstly with the preparation of pure BiFeO3 by co-precipitation and hydrothermal methods and its thermal stability and secondly resolving the cause of discrepancy in range of MPB reported in BiFeO3-PbTiO3 solid solution. Detailed examination of this system (BiFeO3-PbTiO3) around the reported MPB composition by temperature dependent X-ray, electron and neutron diffraction techniques, in conjunction with a systematic correlation of sintering temperature and time with microstructural and phase formation behavior revealed the fact that the formation of MPB or the single ferroelectric phase is critically dependent on the grain size. This phenomenon is also intimately related to the abnormal grain growth in this system. Chapter 1 gives the brief overview of the literature on the topics relevant to the present study. The literature survey starts with a brief introduction about the perovskite oxides; their ferroelectric, magnetic and multiferroic properties were discussed in further sections. A brief outline on the grain growth mechanism is described. An overview of BiFeO3 and various synthesis methods, different chemical substitutions and their effect on properties are provided. A brief review of published literature on BiFeO3-PbTiO3 solid solution and its properties is also presented. Chapter 2 deals with the synthesis of pure BiFeO3, heat treatment and characterisation. BiFeO3 was synthesised by (a) co-precipitation and (b) hydrothermal methods. In co-precipitation method, calcination of precipitate at different temperature resulted in the formation of BiFeO3 along with secondary phases (Bi2Fe4O9 and Bi24FeO39). The optimum calcination temperature to prepare pure BiFeO3 was found to be 560C. The synthesized pure BiFeO3 exhibits weak ferromagnetic hysteresis at room temperature, the degree of which increases slightly at 10K (-263C). The hydrothermal treatment was carried out in (a) carbonate and (b) hydroxide precipitates with KOH as mineralizer. BiFeO3 prepared using hydroxide precipitate was stable till 800C whereas with carbonate precipitate it was stable only till 600C. Chapter 3 deals with the stability of phases in (1-x)BiFeO3 -(x)PbTiO3 solid solution. Samples prepared by conventional solid state route sometimes remain as dense pellet and on certain occasions it disintegrate completely into powder observed after sintering. Irrespective of the composition, sintering time and temperature, powder X-ray Diffraction (XRD) pattern of the survived pellet (crushed into powder) shows coexistence of rhombohedral (R3c) and tetragonal (P4mm) phases and the disintegrated powder (without crushing) show 100% tetragonal (P4mm) phase. Very high spontaneous tetragonal strain (c/a-1) ~0.19 at MPB is believed to be the origin for disintegration. But in all the survived pellets at least a minor fraction of rhombohedral phase (5-7%) is present. Systematic sintering studies with the time and temperature shows, decreasing the sintering temperature and time will increase the lifetime of the pellet and by increasing the sintering temperature and time the pellet will disintegrate. In this work we have conclusively proved that the wide composition range of MPB reported in the literature is due to kinetic arrest of the metastable rhombohedral phase and that if sufficient temperature and time is given, the metastable phase disappears. The suppression/formation of minor rhombohedral phase is expected due to the play of local kinetic factors during the transformation process. This makes the system behave in an unpredictable way with regard to the fraction of rhombohedral phase that is observed at room temperature. A systematic X-ray and neutron powder diffraction study of the giant tetragonality multiferroic (1-x)BiFeO3 -(x)PbTiO3 have shown that the compositions close to the morphotropic phase boundary of this system present two different structural phase transition scenarios on cooling from the cubic phase: (i) Pm3m P4mm(T2)+P4mm(T1) P4mm (T1) and (ii) Pm3m P4mm(T2) + P4mm(T1) + R3c P4mm (T1) + R3c. The comparatively larger tetragonality of the T1 phase as compared to the coexisting isostructural T2 phase is shown to be a result of significantly greater degree of overlap of the Pb/Bi-6s and Ti/Fe-3d with the O-2p orbitals as compared to that in the T2 phase. High temperature electron diffraction studies show that the metastable rhombohedral phase is present in the cubic matrix well above the Curie point as nuclei. Life time of the metastable R3c nuclei is very sensitive to composition and temperature, and nearly diverges at x → 0.27. MPB like state appears only if the system is cooled before the metastable R3c nuclei could vanish. Issue of the metastable rhombohedral state is developed further in Chapter 4. A one-to-one correlation was found between the grain size and phase formation behavior. Fine grained (~1µm) microstructure (usually pellets) shows phase coexistence (R3c+P4mm) and the disintegrated coarse grains (~10µm) show tetragonal (P4mm) phase. Microstructural analysis revealed the disintegration was caused by abnormal grain growth along with the disappearance of metastable rhombohedral phase. Abnormal grain growth starts at the periphery/crack i.e., at the free surface and move towards the canter of the pellet. Size reduction of disintegrated coarse grains (~10µm) to fine grains (~1µm) by crushing the sample showed that the system switching form pure tetragonal (P4mm) state to the MPB state comprising of tetragonal and rhombohedral phases (R3c+P4mm). In another approach the smaller sized particles of x=0.20 were synthesized by sol gel method. It was reported that in conventional solid state route x=0.20 exhibits pure rhombohedral phase. The sol-gel sample calcined at 500C (particle size ~15nm) stabilizes tetragonal metastable phase along with the stable rhombohedral phase, the morphotropic phase boundary state. Samples calcined at higher temperature, 800C (particle size ~50nm) also showed stable rhombohedral phase. Ferromagnetic behavior was observed in the sample having phase coexistence and the sample with pure rhombohedral phase showed antiferromagnetic behavior. Hence this material is a promising candidate which can be tuned to exhibit different behavior just by adopting different grain size. Chapter 5 deals with the magnetic structure of (1-x)BiFeO3 -xPbTiO3 solid solution with change in composition and temperature. Magnetic structure was studied using powder neutron diffraction in the composition range x=0.05 -0.35. Rietveld analysis was carried out for the nuclear and magnetic phases, by considering R3c phase for the nuclear structure. To account for the magnetic Bragg peak at d=4.59Å, three antiferromagnetic models were considered for the magnetic structure: (i) helical spin arrangement as in BiFeO3, (ii) commensurate G-type antiferromagnetic ordering with moments in the a-b plane (of the hexagonal cell), and (iii) commensurate G-type ordering with moments parallel to the c-axis (of the hexagonal cell). The third model was found to be suitable to explain the magnetic peak accurately and the better fitting of magnetic peak was observed in this model compared to others. At room temperature the MPB compositions have rhombohedral and tetragonal nuclear phases along with the rhombohedral magnetic phase. Addition of PbTiO3 in BiFeO3 not only changes the magnetic structure but also reduces the magnetic moment due to the substitution of Ti in Fesite. High temperature neutron diffraction studies reveal the magnetic transition at ~300C for x=0.20, ~95C for x=0.27 and ~150C for x=0.35. The Neel temperature observed in neutron diffraction studies were also confirmed by DSC and by temperature dependent dielectric studies. For x=0.20, anomalous variation in the lattice parameters and the octahedral tilt angle was observed across the magnetic transition temperature. In the magnetic phase, the c-parameter was contracted and the octahedral tilt angle slightly increased. This result suggests a coupling between spin, lattice and structural degrees of freedom around the transition temperature. Temperature dependent powder neutron diffraction study at low temperature from 300K (27C) to 4K (-269C) in x=0.35 shows the evolution of tetragonal magnetic phase at 200K (-73C) whose intensity is increasing with decrease in temperature. Below 200K, x=0.35 has rhombohedral and tetragonal magnetic and nuclear phases. While in x=0.27 at low temperature, rhombohedral magnetic and nuclear phases are present along with the tetragonal nuclear phase alone (the tetragonal magnetic phase is absent). We propose this discrepancy in the Neel temperature and the magnetic phase formation can be due to the probabilistic nature of the existence of metastable rhombohedral phase which was discussed earlier.

La directive européenne RoHS de 2002 prévoit l’interdiction progressive des composés à base de plomb. Or les matériaux piézoélectriques qui présentent le couplage ferroélectrique-ferroélastique le plus fort et qui sont à ce titre largement utilisés en tant que capteurs piézoélectriques ou plus récemment pour des applications de récupération d'énergie, sont justement à base de plomb. La solution solide Bi1-xGaxFeO3 a donc été explorée à la recherche d’une zone de phase morphotropique. Deux phases ferroélectriques peuvent alors coexister et l'instabilité de la polarisation résultante peut alors améliorer la réponse électromécanique. Des gradients de composition de BGFO-x épitaxiés en films minces ont été déposés par ablation laser sur des électrodes de La0,8Sr0,2MnO3. Ils ont été caractérisés par WDX et RBS. Les structures cristallines ont été déterminées par micro-diffraction des rayon-X. La réponse piézoélectrique d33eff est mesurée à différentes échelles, par PFM (quelques nm) et par interférométrie laser (quelques µm) en fonction du gradient. Au lieu d’une analyse d’un choix de compositions ponctuelles qui risquait de passer à côté de la plus intéressante, la continuité inhérente à la méthode combinatoire a permis de mettre en évidence une augmentation remarquable de la réponse piézoélectrique autour 7 % de Ga, justement au voisinage d’un changement de symétrie. / The European RoHS directive in 2002 predicts a progressive prohibition of lead-based compounds. Or the piezoelectric materials that exhibit the strongest ferroelectric-ferroelastic coupling and are widely used as such as piezoelectric sensors or more recently for energy recovery applications are precisely lead based. The solid solution Bi1-xGaxFeO3 has been explored in search of a morphotropic phase boundary (MPB). Two ferroelectric phases can then coexist and the instability of the resulting polarization can then improve the electromechanical response. Gradients composition BGFO-x epitaxial thin films were deposited by pulsed laser deposition on La0,8Sr0,2MnO3 electrodes. They were characterized by WDX and RBS. The crystal structures were determined by micro X-ray diffraction. The effective piezoelectric response d33eff is measured at different scales, by PFM (a few nm) and by laser interferometry (a few microns) along the gradient. Instead of an analysis of a range of compositions that point might miss the most interesting, the inherent continuity combinatorial method was used to highlight a remarkable increase in piezoelectric response around 7% Ga, precisely in the vicinity of a change of symmetry.

Ce travail de thèse expérimentale a été consacré à la synthèse par des méthodes de chimie par voie humide de nanoparticules à base du multiferroïque BiFeO3 et à leur caractérisation, avec comme objectif finale des applications photocatalytiques. Ce matériau présente une bande interdite, avec un gap de 2.6eV, qui permet la photo-génération de porteurs de charges dans le visible faisant ainsi de BiFeO3 un système intéressant pour des processus photo-induits. Ce travail s’est en particulier focalisé à caractériser les propriétés de nanoparticules à base de BiFeO3 en vue de comprendre l’effet de ses propriétés sur leur potentiel dans des applications liées à la photocatalyse. Tout d’abord, l’étude des effets de taille sur les propriétés structurales, de transitions de phase, et physico-chimiques des particules a été réalisée, en gardant comme principal objectif de découpler les propriétés liées à la surface de celles du massif/cœur de la particule. Pour cela, une maîtrise et une optimisation des procédés de synthèse de particules aux échelles nano- et micro-micrométriques de BiFeO3 a été nécessaire pour obtenir des composés de taille variable et de très bonne qualité cristalline. Malgré la diminution de la taille des particules, on constate que, grâce au contrôle de paramètres de synthèse, nos nanoparticules présentent des propriétés très proches à celles du massif de BiFeO3, gardant la structure rhomboédrique R3c avec des faibles effets de contrainte. Afin de contrôler indirectement par le dopage les propriétés optiques des composés à base de BiFeO3, on a réussi à réaliser un dopage très homogène en La3+, et un dopage partiel en Ca2+, sur le site de Bi3+. Les propriétés optiques des nanoparticules et leurs applications dans les premières expériences photocatalytiques sur la dégradation du colorant rhodamine B ont montré la complexité de la physico-chimie de leur surface et du processus d’interaction lumière-particule. Après analyse des données d’absorbance optique en fonction de la taille de nanoparticules, on observe que la bande interdite déduite pour ces différentes particules n’est pas le facteur prédominant sur les performances photocatalytiques. D’autres facteurs ont pu être identifiés comme étant à l’origine de la localisation de charges photo-générées, tels que des états de surface liés à une fine couche de peau ou skin layer sur les nanoparticules, présentant des défauts structuraux, une réduction de l’état d’oxydation du Fe3+ vers le Fe2+ et la stabilisation d’autres adsorbats, tels que FeOOH ; tous ces facteurs peuvent contribuer au changement dans les performances photocatalytiques. Les résultats photocatalytiques restent très encourageants pour poursuivre les études de nanoparticules à base de BiFeO3, montrant une dégradation de la rhodamine B à 50% au bout de 4h de réaction photocatalytique pour certaines des nanoparticules étudiées. / This experimental PhD work has been dedicated to the synthesis, by wet chemistry methods, and characterization of nanoparticles based on multiferroic BiFeO3, with the aim of using them for photocatalytic applications. This material presents a bandgap of 2.6eV, which allows the charge carrier photoexcitation in the visible range, making BiFeO3 a very interesting system for photoinduced processes. This thesis has been particularly focused on characterizing the properties of BiFeO3 nanoparticles in view of understanding the relationship of their properties on their potential use for photocatalytic applications. First of all, the topic of the size effect on the structural properties, phase transitions, and physics and chemistry of the particles has been developed, keeping as first aim to separate the properties related to the surface from those arising from the bulk/core of the particle. To do so, the mastering and optimization of the synthesis processes of BiFeO3 particles at the nano and microscale were needed, to finally obtain different size compounds with high crystalline quality. Despite the size reduction of the particles, we notice that, thanks to the control of the synthesis process, our BiFeO3 nanoparticles present properties very close to those of the bulk BiFeO3 material, keeping the rhombohedral structure R3c with weak strain effects. In order to indirectly tune the optical properties exploiting the doping, we have succeeded in realizing a homogenous La3+ doping, and a partial Ca2+ doping, on the Bi3+ site. The optical properties of the nanoparticles and their use on the first photocatalytic experiments for degrading rhodamine B dye have shown the complexity of the physics and chemistry phenomena at their surface and of the light-particle processes. After analyzing optical absorbance data as a function of the particle size, we observe that the deduced bandgap for different particles is not the main parameter directing the photocatalytic performances. Other factors have been identified to be at the origin of the localization of the photoexcited charges, as the surface states linked to the skin layer of the nanoparticles, depicting structural defects, a reduction of the oxidation state of Fe3+ towards Fe2+ and the stabilization of other adsorbates, such as FeOOH; all these parameters may contribute to the change on the photocatalytic performances. The photocatalytic results are very encouraging, motivating to continue the study of BiFeO3 based nanoparticles, though depicting a 50% rhodamine B degradation after 4h of photocatalytic reaction using some of the present nanoparticles.

Le matériau BiFeO3 (BFO) est le sujet de très nombreuses études fondamentales dans le domaine des matériaux multiferroïques. Cet intérêt est du au fait que cet oxyde présente deux ordres à longue distance à la température ambiante : ferroélectricité et antiferromagnétisme de type G (ce dernier est aussi non colinéaire avec la présence de faible ferromagnétisme ainsi qu’une modulation de spin de type cycloïdale possédant une longueur d’onde de 620 angstrœm). Il est alors possible d’étudier les comportements de couplage entre les propriétés électrique et magnétique. Ce travail concerne principalement la synthèse, les structures haute température, et les propriétés physiques (électronique et magnétique principalement) du matériau BiFeO3 ayant subi des recuits de différentes pressions partielles d’oxygène. La première étape de ce travail concerne l’étude de la synthèse afin de déterminer le protocole optimal de réalisation des céramiques. Les recuits sous atmosphère ont eu pour but de modifier la stœchiométrie en oxygène du matériau, afin d’affecter ses propriétés physiques. Des modifications de faible amplitude de certaines propriétés ont été détectées, mais à l’inverse, la température de Néel et la température de Curie ne sont pas affectées.Concernant la nature des structures haute température, les phases beta et gamma, sujettes à de nombreuses controverses dans la littérature, ont été étudiées par diffraction des rayons X et analyse DSC sur BFO pur ou avec excès de bismuth. Cet excès a permis de stabiliser la phase gamma entre 940 et 950°C, en évitant sa décomposition. Pour compléter ce travail sur BFO en phase pure, nous avons dopé des céramiques avec 10 % de Zr4+ pour étudier le comportement structurale à haute température, ainsi que les propriétés magnétiques et électriques de cette nouvelle composition. Enfin, des simulations numériques sur le composé stœchiométrique, lacunaire en bismuth ou en oxygène ont été réalisées pour comprendre les évolutions structurale, électronique et magnétique du matériau suite aux recuits. La dernière partie est une étude sur le comportement basse température de BFO pur sous différentes formes : nanotubes, céramiques et monocristaux. Nous avons analysé le comportement électrique (impédance, pyroélectricité, RPE et électrostriction), magnétique (aimantation en fonction de la température et du champ magnétique) et structurale (rayon X en thêta-2thêta et rasant, DSC, microRaman et résonance d’ultrasons). Suite à ces études, trois températures sont observées comme présentant un comportement particulier : 140 et 200 K, qui semblent liées par de nombreuses techniques d’analyses et ressortent comme étant une transition à la surface de BFO, mais aussi 180 K où nous avons un écart à la linéarité de la dilatation thermique et un effet d’électrostriction. / BiFeO3 material is the subject of number fundamental studies in multiferroic materials. This interest is mainly cause by the existence of two long range order at room temperature : ferroelectricity and G type antiferromagnetism (this one is also no collinear with the presence of a weak ferromagnetism, and a cycloidal spin modulation with a wave length of 620 angstrom). So, it is possible to study coupling behaviour between electrical and magnetic properties.This work is mainly about the synthesis, high temperature structures, and physical properties (principally electronic and magnetic one) in BFO material after sintering it under different oxygen partial pressure. The first step of this work is about the synthesis study in order to optimize the protocol of ceramic formation. The sintering under atmosphere are done in order to change the oxygen stoichiometry of BFO, we expected to affect this physical properties. We saw some weak modifications of few properties, but Néel and Curie temperature are not altered.Concerning the nature of BFO high temperature structure, beta and gamma phase, which are subject of number controversies in literature, were studied with X-rays and DSC analysis, in pure or in bismuth excess phase. This excess leads to stabilize the gamma phase between 940 and 950°C, and avoid decomposition. To complete this work on pure phase BFO, we doped ceramic with 10 % of Zr4+ in order to study the high temperature structural behaviour, electrical and magnetic properties of this new composition. At last, numerical simulation on the stoichiometric, bismuth or oxygen lacunar system are done to understand structural, electrical and magnetic evolution after the sintering.The last part is a study on behaviour of pure phase BFO at low temperature with different form : nanotube, ceramic and single crystal. We analysed electrical (impedance, pyroelectricity, EPR and electrostriction), magnetic (magnetization function of temperature and magnetic field) and structural comportment (X-rays in theta-2theta and grazing incidence, DSC, microRaman and ultrasonic resonance). It reveals that tree temperature show a specific behaviour : 140 and 200 K, which are link by several analysis technical and seems to be a surface transition (skin effect) in BFO, but also 180 K where we found a non constant evolution in the thermal dilatation, and an electrostriction effect.

Ce travail de thèse porte sur la réalisation de deux instruments adaptés à l’étude de couches minces par spectrométrie Mössbauer du 57Fe par électrons de conversion (CEMS) et à leur utilisation pour la caractérisation de films épitaxiés de ferrite de bismuth BiFeO3 (BFO). Le premier dispositif est constitué d’un compteur proportionnel couplé à un module thermoélectrique. Il permet l’acquisition de manière simple et économique de spectres Mössbauer sur une gamme de température variant de 245 à 375K et sous une induction magnétique externe allant jusqu’à 1,4 T. Un second dispositif a été développé sur la base d’un channeltron™et d’un cryostat à circulation d’hélium pour des acquisitions allant jusqu’à 4 K. Les analyses CEMS ont été réalisées sur des couches minces de différentes épaisseurs de BFO (110) et (001) épitaxiées sur LaAlO3 et SrTiO3. Au-delà d’une épaisseur critique, les couches de BFO (110) présentent un mélange de phases magnétiques colinéaire et cycloïdale. La phase colinéaire présente un axe d’anisotropie suivant [001] dans le plan de la couche et lamodulation cycloïdale se propage dans un plan perpendiculaire à celui-ci. Des effets combinés de contraintes et dimensionnalité ont été avancés pour expliquer la déstabilisation de la cycloïde pour les couches les plus fines. Dans les couches minces de BFO (001) présentant une phase tétragonale de BFO, les mesures CEMS ont montré que la température de mise en ordre magnétique se rapproche de l’ambiante lorsque l’épaisseur des couches diminue. / This work is devoted to the development of two Mössbauer detectors dedicated to thin films studies by conversion electron Mössbauer spectrometry (CEMS), and to their use for the characterization of bismuth ferrite BiFeO3 (BFO) epitaxials thin films. The first designed instrument is composed of a proportional counter and a thermoelectric module. It allows CEMS acquisitions of Mössbauer spectra from 245 to 375K with an external magnetic field upto 1.4 T. The second device is based on a commercial channeltron™ and a continuous flow cryostat allowing measurements downto 4 K. The CEMS measurements have been performed on (110) and (001) oriented BFO layers with various thickness deposited on LaAlO3 et SrTiO3 substrates. Beyond a critical thickness, the (110) BFO exhibits a mixing of collinear and cycloidal magnetic phases. The collinear phase shows an anisotropy axis [001] direction which is located in the sample plane. The cycloid propagation plane have been found to be perpendicular to the sample plane. Both epitaxial strain and size effects have been proposed to explain the cycloid destabilization in the thinner films. In (001) BFO thin films, exhibiting a BFO tetragonal phase, the CEMS measurements have shown that the magnetic ordering temperature tends to decrease with the layer thickness.

There has been significant interest in BiFeO₃ over the past decade. This interest has focused on the magnetic and electrical properties, which in the long term may prove useful in device applications. This thesis focuses on the synthesis, electrical characterisation, and structural origin of the electrical properties of rare earth doped bismuth ferrite. Two systems have been studied: BiFeO₃ doped with lanthanum and neodymium (Bi₁₋ₓREₓFeO₃ RE= La, Nd). Specific examples have been highlighted focusing on a detailed structural analysis of a lanthanum doped bismuth ferrite, Bi₀.₅La₀.₅FeO₃, and a neodymium analogue, Bi₀.₇Nd₀.₃FeO₃. Both adopt an orthorhombic GdFeO₃-type structure (space group: Pnma) with G-type antiferromagnetism. Structural variations were investigated by Rietveld refinement of temperature dependent powder neutron diffraction using a combination of both conventional “bond angle/bond length” and symmetry-mode analysis. The latter was particularly useful as it allowed the effects of A-site displacements and octahedral tilts/distortions to be considered separately. This in-depth structural analysis was complemented with ac-immittance spectroscopy using the multi-formulism approach of combined impedance and modulus data to correlate structural changes with the bulk electrical properties. This approach was essential due to the complex nature of the electrical response with contributions from different electroactive regions. The structural variations occur due to a changing balance between magnetic properties and other bonding contributions in the respective systems. This results in changes in the magnitude of the octahedral tilts, and A-site displacements giving rise to phenomena such as negative thermal expansion and invariant lattice parameters i.e., the invar effect. More specifically, analysis of Bi₀.₅La₀.₅FeO₃ highlights a structural link between changes in the relative dielectric permittivity and changes in the FeO₆ octahedral tilt magnitudes, accompanied by a structural distortion of the octahedra with corresponding A-site displacement along the c-axis; this behaviour is unusual due to an increasing in-phase tilt mode with increasing temperature. The anomalous orthorhombic distortion is driven by magnetostriction at the onset of antiferromagnetic ordering resulting in an Invar effect along the magnetic c-axis and anisotropic displacement of the A-site Bi³⁺ and La³⁺ along the a-axis. This contrasts with the neodymium analogue Bi₀.₇Nd₀.₃FeO₃ in which a combination of increasing A-site displacements in the ac-plane and decrease in both in-phase and anti-phase tilts combine with superexchange giving rise to negative thermal expansion at low temperature. The A-site displacements correlate with the orthorhombic strain. By carefully changing the synthesis conditions, a significant change in bulk conductivity was observed for a number for Bi₁₋ₓLaₓFeO₃ compositions. A series of Bi₀.₆La0.₄FeO₃ samples are discussed, where changes in the second step of the synthesis result in significantly different bulk conductivities. This behaviour is also observed in other compositions e.g. Bi₀.₇₅La₀.₂₅FeO₃. Changes in the electrical behaviour as a function of temperature are discussed in terms of phase composition and concentration gradients of defects. Activation energies associated with the conduction process(es) in Bi₁₋ₓLaₓFeO₃ samples, regardless of composition, fall within one of two broad regimes, circa. 0.5 eV or 1.0 eV, associated with polaron hopping or migration of charge via oxygen vacancies, respectively. The use of symmetry-mode analysis, in combination with conventional crystallographic analysis and electrical analysis using multi-formulism approach, presents a new paradigm for investigation of structure-property relationships in rare earth doped BiFeO₃.

Ces quinze dernières années, l'élaboration d'oxydes fonctionnels sous forme de couches minces a connu un essor important. En microélectronique, ainsi qu'en spintronique, il est important de pouvoir synthétiser des films cristallins avec une épaisseur nanométrique et une interface abrupte. Dans cette configuration, les propriétés des films diffèrent des propriétés du matériau massif, notamment de part l'importance des conditions à l'interface entre le film et le substrat. Cette étude est focalisée sur la croissance par MOCVD a injection pulsée d'oxydes a base de fer : Fe3O4, g-Fe2O3 et BiFeO3. L'originalité de ce travail découle des études in situ des premiers stades de la croissance des films par AFM (microscope a force atomique) sous ultravide.