This thesis provides several nanomaterial systems that can be used as contrast agents in magnetic resonance imaging (MRI) and for optical fluorescence imaging. Nanoparticle systems described in this thesis fall under three categories: (a) graphene oxide-nanoparticle composites for MRI contrast agent application, (b) core-shell nanoparticles for MRI contrast agent application and (c) nanoparticle systems for both MRI and optical fluorescence imaging. In the case of graphene oxide based nano-composites, the following observations were made: (i) in the case of graphene oxide-Fe3O4 nanoparticle composite, it was observed that high extent of oxidation of the graphene oxide and large spacing between the graphene oxide sheets containing Fe3O4 nanoparticles provides the optimum structure for yielding a very high transverse proton relaxivity value, (ii) in the case of graphene oxide-Gd2O3 nanoparticle composite, it was observed that this composite exhibits high value for both longitudinal and transverse relaxivity values making it a potential materials for multi-contrast study of pathologies with a single agent, (iii) in the case of graphene oxide-CoFe2O4 nanoparticle composites, it was observed that an increase in the reflux time of the reaction mixture containing this composite led to appreciable variations in the proton relaxivity values. Transverse relaxivity value of the water protons increased monotonically with increase in the reflux time. Whereas, the longitudinal relaxivity value initially increased and then decreased with increase in the reflux time. In the case of coreshell nanoparticles for MRI contrast agent application two different core-shell systems were investigated. They are MnFe2O3-Fe3O4 core-shell nanoparticles and CoFe2O4-MnFe2O4 coreshell nanoparticles. Investigations of both the core-shell nanoparticle systems revealed that the proton relaxivity value obtained in the dispersion of the core-shell nanoparticles was considerably greater than the proton relaxivity value obtained in the presence of single phase nanoparticles of the core and shell phases. Very high value of transverse relaxivity in the case core-shell nanoparticles was due to the large magnetic inhomogeneity created by the core-shell nanoparticles in the water medium surrounding it. In the case of nanoparticle systems for both MRI and optical fluorescence imaging, two different systems were investigated. They were CoFe2O4-ZnO core-shell nanoparticles and Gd doped ZnS nanoparticles [Zn1-xGdxS, x= 0.1, 0.2 and 0.3] formed on graphene oxide sheets or coated with chitosan. In the case of CoFe2O4-ZnO core-shell nanoparticles it was observed that fluorescent CoFe2O4-ZnO core-shell nanoparticles with the unique geometry in which CoFe2O4 ferrite nanoparticles agglomerates were present within larger sized hollow ZnO capsules yields very high value of transverse proton relaxivity when compared to the proton relaxivity value exhibited by the individual CoFe2O4-ZnO coreshell nanoparticles. In the case of Gd doped ZnS nanoparticles, two different systems were synthesized and the values of the longitudinal and transverse proton relaxivity obtained were compared. These systems were (i) graphene oxide- Zn1-xGdxS (x= 0.1, 0.2 and 0.3) nanoparticle composites and (ii) chitosan coated Zn1-xGdxS (x= 0.1, 0.2 and 0.3) nanoparticles. It was observed that Gd doped ZnS nanoparticles in both cases exhibit both longitudinal and transverse relaxivity values. The relaxivity values showed a clear dependence on the composition of the nanoparticles and the nanoparticle environment (presence and absence of graphene oxide). It was also observed that Gd doped ZnS nanoparticle can be used for florescence imaging.

Les chitooligosaccharides (COS) présentent des propriétés biologiques intéressantes telles que l'activité antimicrobienne, antifongique et antitumorale. Dans ce travail, nous avons utilisé les COS pour des applications très diverses, telles que l'ingénierie des cellules neuronales (blocage de la formation du réseau périneuronal), la complexation des cations Fe2+ et Fe3+ pour la synthèse de particules supermagnatiques et enfin pour le développement de conjugués fonctionnels à base de COS. Dans le cadre de ces études en partenariat, nous avons travaillé sur l'élaboration de chitooligosaccharides à structure contrôlée afin d’étudier leurs propriétés physico-chimiques ou biologiques. Des modifications de chitooligosaccharides ont été effectuées dans ce travail de deux façons: la modification par N-substitution et la modification par le groupe aldéhyde du résidu 2,5-anhydro-D-mannofuranose (amf) à l'extrémité réductrice des chitooligosaccharides. Les premiers types de COS consistent en la désamination suivie d'une réaction de N-réacétylation afin de contrôler (partiellement) à la fois le degré moyen d'acétylation et le degré moyen de polymérisation. La seconde stratégie consiste en la synthèse de nouveaux COS fonctionnalisés à leur extrémité réductrice par amination réductrice et oximation avec différents groupes chimiques cliquables (c'est-à-dire alcyne, alcène, azide, thiol et hydrazide). En fonction des COS fonctionnalisé ciblé, différentes techniques d'analyse ont été réalisées pour analyser pleinement leurs caractéristiques structurales telles que la spectroscopie RMN, la spectrométrie de masse MALDI-TOF, la chromatographie HPLC, la spectroscopie RAMAN et la chromatographie SEC. Des structures chimiques spécifiques de chitooligosaccharides modifiés ont été étudiées dans le but de les utiliser pour moduler le réseau périneural de neurones et l'établissement de connexions synaptiques. Nous avons également montré que les COS solubles permettent la précipitation des nanoparticules supramagnétiques de Fe3O4 avec un revêtement COS en les rendant moins toxiques. Enfin, les COS fonctionnalisés à leur extrémité réductrice pourraient être des intermédiaires utiles pour le développement de nouveaux conjugués fonctionnels à base de chitosane / Chitooligosaccharides (COS) classically present several biological properties such as anti-microbial, anti-tumor and anti-fungal activity. In this work, we used COS for widely different applications, such as tissue engeneering of neuronal cells (blocking of perineuronal net formation), the complexation of iron cations (Fe2+ and Fe3+) for the synthesis of supermagnatic particle and finally for the development of advanced functional COS-based conjugates. In this partnership studies, we worked on the elaboration of controlled structure chitooligosaccharides in order to decipher their physico-chemical or biological properties. Further modification of chitooligosaccharides was performed in this thesis in two ways: modification via amine N-substitution and the modification via the 2,5-anhydro-D-mannofuranose (amf) aldehyde group located at the reducing end of chitooligosaccharides. The first COS types consist in the nitrous depolymerization followed by N-acetylation in order to (partly) control both the mean degree of N-acetylation and the degree of polymerization. The second consist in the synthesis of new COS-based building blocks functionalized at their reducing end by reductive amination and oximation with different clickable chemical groups (i.e. alkyne, alkene, azide, thiol, and hydrazide). Depending on the targeted functionalized COS, different analysis techniques were carried out to fully characterize such as NMR spectroscopy, MALDI-TOF mass spectrometry, HPLC-chromotography, RAMAN spectroscopy and SEC chromatography. Specific chitooligosaccharides were studied in the objective to use them to modulate the perineuronal net of neurons, and the establishment of synaptic connections. We also showed that water soluble COS permit the precipitation of supramagnetic Fe3O4 nanoparticles with a COS coating and succeded in decreasing their toxicity. Finally we have shown that COS-based building blocks could be useful intermediates for the development of advanced functional COS-based conjugates such as COS-b-PEG diblock copolymers

Ce travail s'inscrit dans les recherches actives des nouvelles propriétés magnétiques et électriques dans les hétérostructures artificielles. Nous avons élaboré et étudié un système du type « Oxyde ferrimagnétique / Métal non magnétique / Oxyde ferrimagnétique » dans lequel les électrons sont confinés dans la couche métallique 2D et subissent de nombreuses réflexions aux interfaces « métal / isolant magnétique ». L'élaboration de ce système impose une maîtrise de la croissance des différentes couches et de la planéité des interfaces. Les dépôts sont épitaxiés afin de limiter les diffusions des électrons aux joints de grains par pulvérisation cathodique dans un bâti UHV, les caractérisations structurales sont essentiellement réalisées par microscopie électronique haute résolution et diffraction des rayons X.<br />Nous avons étudié la croissance épitaxiale de couches simples de Fe3O4 et de CoFe2O4 sur Al2O3(0001) et MgO(001) afin d'obtenir respectivement une direction de croissance [111] et [001]. Nous nous sommes également intéressés à la croissance épitaxiale et à l'anisotropie d'échange de bicouches Fe3O4(5nm à 50nm)/NiO(66nm) dans ces deux mêmes directions de croissance. Nous avons ensuite étudié la croissance de métaux non oxydables (Pt, Au et Ag) sur les surfaces (001) et (111) de Fe3O4.<br />Ces résultats ont permis d'élaborer les systèmes épitaxiés Fe3O4/M(M=Au,Pt)/ CoFe2O4 sur Al2O3(0001). Les propriétés électriques montrent que les électrons sont confinés dans la couche métallique et qu'apparaît une GMR atteignant près de 1,8% à 10K due exclusivement aux réflexions électroniques sur les interfaces métal/oxyde avec certainement une contribution des réflexions spéculaires.

Graphene has been shown to be very powerful as a transducer in many biosensor applications due to its high sensitivity. This enables smaller surfaces and therefore less material consumption when producing sensors and concequently cheaper and more portable sensors compared to the commercially available sensors today. The electrical properties of graphene are very sensitive to gas exposure why presence of molecules or small changes in concentration could easily be detected when using graphene as a sensing layer. Graphene is sensitive towards many molecules and in order to detect and possibly identify gas molecules the surface needs to be functionalized. The intention of this project was to use nanoparticles (NPs) to further increase sensitivity and specificity towards selected molecules and also enable biofunctionalization of the NPs, and by that tune the electrical properties of the graphene. This study proposes the use of Fe3O4 and TiO2 NPs to enable sensitive detection of volatile gases and possibly further functionalization of the NPs using biomolecules as a detecting agent in a liquid-phasebiosensor application. The interaction between graphene and NPs have been investigated using several surface charactarization methods and electrical measurements for detection of gaseous molecules and also molecules in a liquid solution. The characterizing methods used are XPS, AFM with surface-potential mapping and Raman spectroscopy with reflectance mapping in order to investigate the NPs interaction with the graphene surface. Sensors where manufactured for gas-phase detection of CO, formaldehyde, benzene and NH3 specifically and display differences in sensitivity and behavior of the Fe3O4 and TiO2 NPs respectively. For liquid measurements the difference in behavior in two buffers was investigated using an in-house flow-cell setup. The surface charecterizing measurements indicated that just a small difference could be found between the two NPs, however a significant change in sensor response could be detected as a function of coverage. The liquid and gas-phase measurements rendered information on differences in sensitivity between the NPs and between analytes where TiO2 showed a higher level of sensitivity towards most of the gases investigated. Both Fe3O4 and TiO2 NP coated graphene showed capability to detect formaldehyde and benzene down to 50 ppb and 5 ppb respectively. The sensitive gas detection could help protecting individuals being exposed to a hazardous level of volatile gases if concentrations increase rapidly or at a long term exposure with lower concentrations, improving saftey and health where these gases are present.

Les nanoparticules d'oxyde de fer de structure spinelle ouvrent de nombreuses voies dans le domaine biomédical. Parmi les applications possibles, les propriétés superparamagnétiques des cristallites d'une dizaine de nanomètres permettent de les utiliser pour le diagnostic médical, notamment en Imagerie par Résonance Magnétique (IRM).Ce travail a consisté à élaborer des suspensions colloïdales de nanoparticules de magnétite ou de maghémite (nommées USPIO pour Ultrasmall SuperParamagnetic Iron Oxide) compatibles avec les conditions physiologiques (pH = 7,4 et [NaCl] = 0,15 M).Par co-précipitation classique, des USPIO, de taille de cristallites de 8 nm, de surface spécifique de 110 m².g-1 et agrégés en assemblages d'environ 20 nm ont été obtenus. Pour stabiliser ces nano-objets, deux voies ont été explorées. Des agents électrostatiques (acide citrique et DMSA) ont modifié la charge nette de surface des oxydes de fer. La stabilisation stérique a également été explorée par greffage de méthoxy-PEG couplés à des fonctions silanes (mPEG-Si). Par combinaison de mPEG2000-Si et de DMSA, des suspensions stables ont également été obtenues. De plus, les fonctions thiols apportées par le DMSA et présentes à la surface des agrégats se trouvent protégées de leur oxydation naturelle par l'encombrement stérique des chaînes de polymère (la formation de ponts disulfures est évitée). La post-fonctionnalisation de ces nanoparticules via ces fonctions thiols est alors possible plusieurs semaines après leur synthèse. Ce concept a été validé par post-greffage d'un fluorophore (0,48 RITC/nm²) pour la détection in vitro en microscopie à fluorescence.En parallèle de cette étude en " batch ", des nanoparticules d'oxyde de fer ont été synthétisées en continu à l'aide d'un procédé hydrothermal pouvant s'étendre au domaine eau supercritique. En voie hydrothermale classique, des USPIO stabilisés par des ions citrates ont été obtenus en continu. Grâce aux propriétés physicochimiques de l'eau supercritique, la co-précipitation de magnétite a été possible sans l'utilisation de base.La cytotoxicité et l'internalisation cellulaire de ces USPIO ont été évaluées sur trois modèles cellulaires (macrophages RAW, hépatocytes HepG2 et cardiomyocytes) et les efficacités comme agents de contraste en IRM de ces nanoparticles ont été mesurées sur gel et sur modèle murin et comparées à un agent de contraste commercial à base d'oxyde de fer. Les nanohybrides étudiés n'ont pas présenté de cytotoxicité et ont développé des pouvoirs contrastants comparables à l'agent commercial. La biodistribution hépatique des nanoparticules couplées au mPEG-Si a été retardée de plus de 3 heures ouvrant la voie à des détections spécifiques.

This thesis consists of two parts. The first part deals with the magnetic properties of Fe3O4 nanocrystals and their possible application in water remediation. The second part is on the delamination of layered materials and the preparation of new layered hybrids from the delaminated sheets. In recent years, nanoscale magnetic particles have attracted considerable attention because of their potential applications in industry, medicine and environmental remediation. The most commonly studied magnetic nanoparticles are metals, bimetals and metal oxides. Of these, magnetite, Fe3O4, nanoparticles have been the most intensively investigated as they are, non-toxic, stable and easy to synthesize. Magnetic properties of nanoparticles such as the saturation magnetization, coercivity and blocking temperature are influenced both by size and shape. Below a critical size magnetic particles can become single domain and above a critical temperature (T B , the blocking temperature) thermal fluctuations can induce random flipping of magnetic moments resulting in loss of magnetic order. At temperatures above the blocking temperature the particles are superparamagnetic. Magnetic nanocrystals of similar dimensions but with different shapes show variation in magnetic properties especially in the value of the blocking temperature, because of differences in the surface anisotropy contribution. The properties of magnetic nanoparticles are briefly reviewed in Chapter 1. The objective of the present study was to synthesize Fe3O4 nanocrystals of different morphologies, to understand the difference in magnetic properties associated with shape and to explore the possibility of using Fe3O4 nanocrystals in water remediation. In the present study, oleate capped magnetite (Fe3O4) nanocrystals of spherical and cubic morphologies of comparable dimensions (∼10nm) have been synthesized by thermal decomposition of FeOOH in high-boiling octadecene solvent (Chapter 2). The nanocrystals were characterized by XRD, TEM and XPS spectroscopy. The nanoparticles of different morphologies exhibit very different blocking temperatures. Cubic nanocrystals have a higher blocking temperature (T B = 190 K) as compared to spheres (T B = 142 K). From the shift in the hysteresis loop it is demonstrated that the higher blocking temperature is a consequence of exchange bias or exchange anisotropy that manifests when a ferromagnetic material is in physical contact with an antiferromagnetic material. In nanoparticles, the presence of an exchange bias field leads to higher blocking temperatures T B because of the magnetic exchange coupling induced at the interface between the ferromagnet and antiferromagnet. It is shown that in these iron oxide nanocrystals the exchange bias field originates from trace amounts of the antiferromagnet wustite, FeO, present along with the ferrimagnetic Fe3O4 phase. It is also shown that the higher FeO content in nanocrystals of cubic morphology is responsible for the larger exchange bias fields that in turn lead to a higher blocking temperature. Magnetic nanoparticles with moderate magnetization can be easily separated from dispersions by applying low intensity magnetic fields. Oleate capped spherical and cubic iron oxide nanocrystals have considerable magnetic moment and hence have the potential as host-carriers for magnetic separation in environmental remediation. These nanocrystals are, however, dispersible only in non-polar solvents like chloroform, toluene, etc. Environmental remediation requires that the nanocrystals be water dispersible. This was achieved by functionalizing the surface of the iron oxide nanocrystals by coordinating carboxymethyl-β-cyclodextrin (CMCD) cavities (Chapter 3). The hydroxyl groups located at the rim of the anchored cyclodextrin cavity renders the surface of the functionalized nanocrystal hydrophilic. The integrity of the anchored CMCD molecules are preserved on capping and their hydrophobic cavities available for host-guest chemistry. The CMCD capped iron oxide particles are water dispersible and separable in modest magnetic fields (<0.5 T). Small molecules like naphthalene and naphthol can be removed from aqueous media by forming inclusion complexes with the anchored cavities of the CMCD-Fe3O4 nanocrystals followed by separation of the nanocrystals by application of a magnetic field. The adsorption properties of the iron oxide surface towards arsenic ions are unaffected by the CMCD capping so it too can be simultaneously removed in the separation process. To extend the application of the iron oxide nanocrystals so that they can both capture and destroy organic contaminants present in water, cyclodextrin functionalized water dispersible core-shell Fe3O4@TiO2 (CMCD-Fe3O4@TiO2) nanocrystals have been synthesized (Chapter 4). The application of these particles for the photocatalytic degradation of endocrine disrupting chemicals (EDC), bisphenol A and dibutyl phthalate, in water is demonstrated. EDC molecules that may be present in water are captured by the CMCD-Fe3O4@TiO2 nanoparticles by inclusion within the anchored cavities. Once included they are photocatalytically destroyed by the TiO2 shell on UV light illumination. The magnetism associated with the crystalline Fe3O4 core allows for the magnetic separation of the particles from the aqueous dispersion once photocatalytic degradation is complete. An attractive feature of these ‘capture and destroy’ nanomaterials is that they may be completely removed from the dispersion and reused with little or no loss of catalytic activity. The second part of the thesis deals with the intercalation of surfactants in inorganic layered solids and their subsequent delamination of the functionalized solid in non-polar solvents. The solids investigated were - the anionic layered double hydroxides (LDH), the 2:1 smectite clay, montmorillonite (MMT), layered metal thiophosphates (CdPS3) and graphite oxide (GO). Layered Double Hydroxides (LDH) are lamellar solids of the general chemical formula [M0(1−x)Mx(OH)2], where M0 is a divalent metal ion and M a trivalent ion. The structure of the Mg-Al layered double hydroxide (Mg-Al LDH) may be derived from that of brucite, Mg(OH)2, by isomorphous substitution of a part of the Mg2+ by trivalent Al3+ ions with electrical neutrality maintained by interlamellar exchangeable ions like nitrate or carbonate. The ion exchange intercalation of the anionic surfactant dodecyl sulfate (DDS) in an Mg-Al LDH and the subsequent delamination of the surfactant intercalated LDH in non-polar solvent is reviewed in Chapter 5. Delamination results in a clear dispersion of neutral nanosheets. The delaminated sheets are neutral as the surfactant chains remain anchored to the inorganic sheet. On solvent evaporation, the sheets re-stack to give back the original surfactant intercalated solid. This strategy for delamination of layered solids by intercalation of an appropriate surfactant followed by dispersing in a non-polar solvent has been extended to montmorillonite (MMT) and cadmium thiophosphates (CdPS3) by ion-exchange intercalation of the cationic surfactant dioctadecyldimethylammonium bromide (DODMA) followed by sonication in non-polar solvents e.g. toluene or chloroform as in the case of the LDH (Chapter 6). The nanosheets of the MMT and CdPS3 are electrically neutral as the surfactant chains remain anchored to the inorganic sheet even after exfoliation. Graphite oxide (GO) too can be delaminated by functionalizing the sheets by covalently linking oleylamine chains to the GO sheets via an amide bond. The oleylamine functionalized GO is easily delaminated in non-polar solvents to give electrically neutral GO nanosheets. It is shown in Chapter 7 that the 1:1 mixtures of dispersions of montmorillonite-DODMA with Mg-Al LDH-DDS nanosheets can self assemble, on solvent evaporation, to give a new layered solid with periodically alternating montmorillonite and LDH layers. In this method attractive forces between the neutral exfoliated nanosheets of cationic and anionic ensures self-assembly of a perfectly periodic alternating layered structure. The method has been extended to synthesize new layered solids in which surfactant tethered cationic and anionic inorganic sheets alternate. The hybrid solids synthesized are CdPS3—MgAl-LDH, CdPS3—CoAl-LDH, GO—MgAl-LDH, GO—CoAl-LDH. The procedure outlined in Chapter 7 allows for a simple, but versatile, method for generating new periodically ordered layered hybrid solids by self-assembly.

No description available.

Since many years, the importance of thin layers increases for lots of technical uses. Beginning in the field of microelectronics, the use of thin layers spread increasingly to other areas. Coatings for surface refining and optimisation of the mechanical properties for material engineering, customisation of the surface chemistry in catalysts, as well influencing of the transmission and reflection characteristics of surfaces in optics are only some examples of the high scientific and economic weight of the thin layer technology. Thin magnetic layers are the basis of many known storage media ranging from the tape recorder to the hard disk up to the credit card. Nowadays, these thin layers again gain interest in the research field of nanoelectronics as ultrathin layers. So-called spinvalve-read/write heads being already installed in actual hard disks use the Tunnel Magneto Resistance effect for a significant rise in memory density synonymous capacity. Such read/writeheads consist of a magnetic layersystem. This use of the magnetic as well as the electric characteristics of the electrons is called spintronics. The iron oxide magnetite exhibits a high iron portion, is strong antiferrimagnetic and has a high Curie-temperature. Since many years, it is used as a magnetic pigment on already mentioned magnetic tapes. Literature [1, 2, 3, 4] considers ultrathin epitaxial layers of magnetite on magnesium oxide for uses in the spintronics as a most promising candidate, because it inheres a complete spin polarisation at Fermi-level. Moreover, thin magnetite layers serve in the chemical industry as a catalyst in the Haber- Bosch-procedure and to the dehydration of ethylbenzene to styrene. Being already used and considered to be of ongoing interest, ultrathin magnetite layers offer a wide range of technological applications in many modern industrial and scientific fields. Because there is, nevertheless, a variety of other iron oxide (cf. chapter 4), it is a matter to determine the special growth conditions of magnetite. These ultrathin iron oxide layers were grown reactively on the (001)-surfaces of the magnesium oxide substrate by molecular beam epitaxy. Besides, the surface is examined by the diffraction of low-energy electrons concerning its crystalline structure. X-ray photo electron spectroscopy approaching the stochiometry completes these first characterisations. Other investigations are carried out at HASYLAB / DESY in Hamburg by X-ray reflectivity and X-ray diffraction. The exact thickness of the layers, its crystal properties in bulk, as well as the thickness of the crystalline portion of the layers can be determined among other features of the system. The evaluation of XRR-and XRD-investigations is done via simulations with in chapter 5 introduced software packages. The reader finds the theoretical backgrounds to the used techniques in chapter 3. The experimental setups in Osnabr¨uck and Hamburg as well as the backgrounds to the preparation are presented in chapter 5. Because the formation of the different iron oxides is described in literature [5, 6, 7, 8] as mostly depending on annealing temperatures, the experimental results in chapter 6 are graded accordingly. The dependence on temperature, layer thickness and annealing time should be examined for the iron oxides possible on this substrate. The aim of this work is the preparation of ultrathin epitaxial iron oxide layers with thicknesses up to few nanometers. The main goal is to find the growth parameters for ultrathin crystalline magnetite layers.

This work investigates the growth dynamic of the reactive molecular beam epitaxy of Fe3O4 films, and its impact on the cation distribution as well as on the magnetic and structural properties at the surface and the interfaces. In order to study the structure and composition of Fe3O4 films during growth, time-resolved high-energy x-ray diffraction (tr-HEXRD) and time-resolved hard x-ray photoelectron spectroscopy (tr-HAXPES) measurements are used to monitor the deposition process of Fe3O4 ultrathin films on SrTiO3(001), MgO(001) and NiO/MgO(001). For Fe3O4\SrTiO3(001) is found that the film first grows in a disordered island structure, between thicknesses of 1.5nm to 3nm in FeO islands and finally in the inverse spinel structure of Fe3O4, displaying (111) nanofacets on the surface. The films on MgO(001) and NiO/MgO(001) show a similar result, with the exception that the films are not disordered in the early growth stage, but form islands which immediately exhibit a crystalline FeO phase up to a thickness of 1nm. After that, the films grown in the inverse spinel structure on both MgO(001) and NiO/MgO(001). Additionally, the tr-HAXPES measurements of Fe3O4/SrTiO3(001) demonstrate that the FeO phase is only stable during the deposition process, but turns into a Fe3O4 phase when the deposition is interrupted. This suggests that this FeO layer is a strictly dynamic property of the growth process, and might not be retained in the as-grown films. In order to characterize the as-grown films, a technique is introduced to extract the cation depth distribution of Fe3O4 films from magnetooptical depth profiles obtained by fitting x-ray resonant magnetic reflectivity (XRMR) curves. To this end, x-ray absorption (XAS) and x-ray magnetic circular dichroism (XMCD) spectra are recorded as well as XRMR curves to obtain magnetooptical depth profiles. To attribute these magnetooptical depth profiles to the depth distribution of the cations, multiplet calculations are fitted to the XMCD data. From these calculations, the cation contributions at the three resonant energies of the XMCD spectrum can be evaluated. Recording XRMR curves at those energies allows to resolve the magnetooptical depth profiles of the three iron cation species in Fe3O4. This technique is used to resolve the cation stoichiometry at the surface of Fe3O4/MgO(001) films and at the interfaces of Fe3O4/MgO(001) and Fe3O4/NiO. The first unit cell of the Fe3O4(001) surface shows an excess of Fe3+ cations, likely related to a subsurface cation-vacancy reconstruction of the Fe3O4(001) surface, but the magnetic order of the different cation species appears to be not disturbed in this reconstructed layer. Beyond this layer, the magnetic order of all three iron cation species in Fe3O4/MgO(001) is stable for the entire film with no interlayer or magnetic dead layer at the interface. For Fe3O4/NiO films, we unexpectedly observe a magnetooptical absorption at the Ni L3 edge in the NiO film corresponding to a ferromagnetic order throughout the entire NiO film, which is antiferromagnetic in the bulk. Additionally, the magnetooptical profiles indicate a single intermixed layer containing both Fe2+ and Ni2+ cations.