Tuning the structural and magnetic properties of Sr 2 FeReO 6 by substituting Fe and Re with valence invariant metals

In the course of this work the effect of metal substitution on the structural and magnetic properties of the double perovskites Sr2MM’O6 (M = Fe, substituted by Cr, Zn and Ga; M’ = Re, substituted by Sb) was explored by means of X-ray diffraction, magnetic measurements, band structure calculations, Mößbauer spectroscopy and conductivity measurements. The focus of this study was the determination of (i) the kind and structural boundary conditions of the magnetic interaction between the M and M’ cations and (ii) the conditions for the principal application of double perovskites as spintronic materials by means of the band model approach. Strong correlations between the electronic, structural and magnetic properties have been found during the study of the double perovskites Sr2Fe1-xMxReO6 (0 < x < 1, M = Zn, Cr). The interplay between van Hove-singularity and Fermi level plays a crucial role for the magnetic properties. Substitution of Fe by Cr in Sr2FeReO6 leads to a non-monotonic behaviour of the saturation magnetization (MS) and an enhancement for substitution levels up to 10 %. The Curie temperatures (TC) monotonically increase from 401 to 616 K. In contrast, Zn substitution leads to a continuous decrease of MS and TC. The diamagnetic dilution of the Fe-sublattice by Zn leads to a transition from an itinerant ferrimagnetic to a localized ferromagnetic material. Thus, Zn substitution inhibits the long-range ferromagnetic interaction within the Fe-sublattice and preserves the long-range ferromagnetic interaction within the Re-sublattice. Superimposed on the electronic effects is the structural influence which can be explained by size effects modelled by the tolerance factor t. In the case of Cr substitution, a tetragonal – cubic transformation for x > 0.4 is observed. For Zn substituted samples the tetragonal distortion linearly increases with increasing Zn content. In order to elucidate the nature of the magnetic interaction between the M and M’ cations, Fe and Re were substituted by the valence invariant main group metals Ga and Sb, respectively. X-ray diffraction reveals Sr2FeRe1-xSbxO6 (0 < x < 0.9) to crystallize without antisite disorder in the tetragonal distorted perovskite structure (space group I4/mmm). The ferrimagnetic behaviour of the parent compound Sr2FeReO6 changes to antiferromagnetic upon Sb substitution as determined by magnetic susceptibility measurements. Samples up to a doping level of 0.3 are ferrimagnetic, while Sb contents higher than 0.6 result in an overall antiferromagnetic behaviour. 57Fe Mößbauer results show a coexistence of ferri- and antiferromagnetic clusters within the same perovskite-type crystal structure in the Sb substitution range 0.3 < x < 0.8, whereas Sr2FeReO6 and Sr2FeRe0.9Sb0.1O6 are “purely” ferrimagnetic and Sr2FeRe0.1Sb0.9O6 contains antiferromagnetically ordered Fe sites only. Consequently, a replacement of the Re atoms by a nonmagnetic main group element such as Sb blocks the double exchange pathways Fe–O–Re(Sb)–O–Fe along the crystallographic axis of the perovskite unit cell and destroys the itinerant magnetism of the parent compound. The structural and magnetic characterization of Sr2Fe1-xGaxReO6 (0 < x < 0.7) exhibit a Ga/Re antisite disorder which is unexpected because the parent compound Sr2FeReO6 shows no Fe/Re antisite disorder. This antisite disorder strongly depends on the Ga content of the sample. Although the X-ray data do not hint at a phase separation, sample inhomogeneities caused by a demixing are observed by a combination of magnetic characterization and Mößbauer spectroscopy. The 57Fe Mößbauer data suggest the formation of two types of clusters, ferrimagnetic Fe- and paramagnetic Ga-based ones. Below 20 % Ga content, Ga statistically dilutes the Fe–O–Re–O–Fe double exchange pathways. Cluster formation begins at x = 0.2, for 0.2 < x < 0.4 the paramagnetic Ga-based clusters do not contain any Fe. Fe containing Ga-based clusters which can be detected by Mößbauer spectroscopy firstly appear for x = 0.4.

Spin polarized transport in manganese oxide double-perovskite thin films

Gegenstand dieser Arbeit war die Untersuchung von metallischen gemischtvalenten Manganaten und magnetischen Doppelperowskiten. Aufgrund ihres großen negativen Magnetowiderstandes (MW) sind diese halbmetallischen Oxide interessant für mögliche technische Anwendungen, z.B. als Leseköpfe in Festplatten. Es wurden die kristallographischen, elektronischen und magnetischen Eigenschaften von epitaktischen Dünnschichten und polykristallinen Pulverproben bestimmt.Epitaktische Dünnschichten der Verbindungen La_0.67Ca_0.33MnO₃ und La_0.67Sr_0.33MnO₃ wurdenmit Kaltkathodenzerstäubung und Laserablation auf einkristallinen Substraten wie SrTiO₃abgeschieden. Mit Hall-Effekt Messungen wurde ein Zusammenbruch der Ladungsträgerdichte bei der Curie-Temperatur T_C beobachtet.Mit dem Wechsel des Dotierungsatoms A von Ca (T_C=232 K) zu Sr (T_C=345 K)in La_0.67A_0.33MnO₃ konnte die Feldsensitivität des Widerstandes bei Raumtemperatur gesteigert werden. Um die Sensitivität weiter zu erhöhen wurde die hohe Spinpolarisation von nahezu 100% in Tunnelexperimenten ausgenutzt. Dazu wurden biepitaktische La_0.67Ca_0.33MnO₃ Schichten auf SrTiO₃ Bikristallsubstraten hergestellt. Die Abhängigkeit des Tunnelmagnetowiderstandes (TMW) vom magnetischen Feld, Temperatur und Strum war ein Schwerpunkt der Untersuchung. Mittels spinpolarisierten Tunnelns durch die künstliche Korngrenze konnte ein hysteretischer TMW von 70% bei 4 K in kleinen Magnetfeldern von 120 Oe gemessen werden. Eine weitere magnetische Oxidverbindung, der Doppelperowskit Sr₂FeMoO₆ miteine Curie-Temperatur oberhalb 400 K und einem großen MW wurde mittels Laserablation hergestellt. Die Proben zeigten erstmals das Sättigunsmoment, welches von einer idealen ferrimagnetischen Anordnung der Fe und Mo Ionen erwartet wird. Mit Hilfe von Magnetotransportmessungen und Röntgendiffraktometrie konnte eine Abhängigkeit zwischen Kristallstruktur (Ordnung oder Unordnung im Fe, Mo Untergitter) und elektronischem Transport (metallisch oder halbleitend) aufgedeckt werden.Eine zweiter Doppelperowskit Ca₂FeReO₆ wurde im Detail als Pulverprobe untersucht. Diese Verbindung besitzt die höchste Curie-Temperatur von 540 K, die bis jetzt in magnetischen Perowskiten gefunden wurde. Mit Neutronenstreuung wurde eine verzerrte monoklinische Struktur und eine Phasenseparation aufgedeckt.

Neue Materialien für die Magnetoelektronik: Heusler- und Halb-Heusler-Phasen

Heusler- und Halb-Heusler-Phasen konnten als Verbindungsklasse identifiziert werden, neue Materialien für die Magnetoelektronik bereitzustellen. Auf Basis eines theoretischen Modells konnte das Auftreten eines hohen MR-Effekts auf bestimmte Valenzelektronenzahlen (VEK) präzisiert werden. Dazu muß ein dreiteiliger 'Fingerabdruck' in der Bandstruktur (Sattelpunkt, Spindichtewelle, lokales magnetisches Moment) vorliegen. Es existieren eine Vielzahl von halbmetallischen Ferromagneten in dieser Verbindungsklasse. Die variable Valenzelektronenkonzentrationen, die sich auch aus den hochsymmetrischen Strukturen ergeben, erlauben eine gute Dotierbarkeit der Phasen. Dadurch ist die Möglichkeit gegeben, die Phase exakt mit der geforderten VEK zu synthetisieren. Curietemperaturen > 500 K sind in Hinblick auf die technische Anwendbarkeit notwendig. PdMnTe hat nicht die Voraussetzungen für einen PMR-Effekt in der Bandstrukturrechnung, doch die Nähe zu einer halbmetallischen Zustandsdichte resultiert in einen negativen CMR-Effekt unterhalb des magnetischen Übergangs von MR0 = 18 % bei 4 K. Die Zusammenhänge von Probenpräparation zum magnetischen Sättigungsmoment konnten an Co2CrAl aufgedeckt werden. Die unter Anwendung des vorgestellten Modells synthetisierte Heusler-Phase Co2Cr0.6Fe0.4Al (VEK = 27.8) weisen den erwarteten MR-Effekt auf. Der gemessene PMR-Effekt ist größer als bei den GMR-Systemen (bei geringerer Feldempfindlichkeit) und anderen granularen Materialien wie CrO2 bei 295 K. Co2Cr0.6Fe0.4Al zeigt bei 295 K einen hohen negativen Magnetowiderstand von 30 % bei einem Sättigungsfeld von 0.2 Tesla. Durch die Beimischung von Oxiden und Polymeren sind Komposit-Materialien entwickelt worden, die MR0-Effekte von bis zu 88% mit einer verbesserten Feldempfindlichkeit von 0.1 Tesla bei Al2O3 und 0.05 Tesla bei den Oberflächenbeschichtungen zeigen.

Photochemie von ungesättigten Sternverbindungen

Photochemie von ungesättigten Sternverbindungen.Wirt-Gast-Systeme bei stilbenoiden Dendrimeren. Diese Arbeit beschäftigt sich mit der Synthese und denphotochemischen Eigenschaften stilbenoider und chalkonoiderSternverbindungen.Die Synthese der stilbenoiden Dendrimere gelingt über einekonvergente in einzelnen Generationen gekoppelteSynthesestrategie durch Wittig-Horner-Olefinierung inKombination mit einer Schutzgruppentechnik.Experimente mit den stibenoiden Dendrimeren 1. Generationhaben gezeigt, dass geänderte Belichtungsbedingungen(monochromatisches Licht in Gegenwart einesTriplett-Sensibilisators) die photochemische[2+2]Cycloaddition bzw. CC-Verknüpfung unterdrücken. Dabeiverläuft selektiv eine cis/trans-Isomerisierung, die füroptische Schaltung genutzt werden könnte.Mit Triplett-Sensibilisatoren wie Diacetyl oder Acetonkonnten auch Wirt-Gast-Systeme mit stilbenoiden Dendrimerengebildet werden. Das zeigt die Möglichkeit der Einlagerungvon Gastmolekülen in freie Kavitäten der Dendrimere.Die Synthese der chalkonoiden Sternverbindungen gelingt übereine dreifache Aldolkondensation des 1,3,5-Triacetylbenzolsmit unsubstituierten oder 3,4,5-trialkoxysubstituiertenBenzaldehyden. Mit einer geeigneten Verzweigungseinheitwurden auch Armbauteile zur Generationenerweiterungsynthetisiert.Die photochemischen Eigenschaften der chalkonoidenSternverbindungen in Lösung und im Festzustand wurdenstudiert und die entstandenen Produkte charakterisiert. BeiBelichtung im Festzustand läuft bei topochemischer Kontrolleeine Photodimerisierung unter Bildung eines Cyclobutanringsdurch Cycloaddition olefinischer Doppelbindungen ab, wobeiein Kopf-Schwanz-anti-Dimer erhalten wird. BeiPhotodimerisierung in Lösung entsteht einKopf-Kopf-anti-Dimer als Hauptprodukt. Das kann zur Syntheseder sonst schwer zugänglichen [4.4.4](1,3,5)Cyclophanegenutzt werden.

Thiete und Bisthiete in der Heterocyclensynthese

Die vorliegende Arbeit beschäftigt sich mit der Synthese arenoanellierter Naphthothiete und Benzobisthiete, sowie mit der Umsetzung der aus diesen Thieten thermisch generierbaren Valenzisomeren (Thiochinonmethide). Diese Thiochinonmethide sind hochreaktive Diensysteme, die mit zahlreichen Dienophilen (homo- und hetero-Doppel- und Dreifachbindungssysteme) nach Diels-Alder abreagieren, die dabei entstehenden S-Heterocyclen können im Sechsring noch weitere Heteroatome (N, P, O, S) enthalten. Daraus resultiert ein großes Potential der Arenothiete zur Synthese neuer Thioheterocyclen. Durch die erstmals gelungene Synthese der beiden Benzobisthiete 2H,3H-Benzo[1,2-b:4,3-b']bisthiet und 1H,4H-Benzo[2,1-b:3,4-b']bisthiet mit gewinkelter Anellierungsgeometrie hat das synthetische Spektrum der aus Arenothieten darstellbaren Thioheterocyclen nochmal eine deutliche Erweiterung erfahren.

Die Darstellung der Arenothiete erfolgt in einer mehrstufigen Synthese, in deren finalem Schritt sie mittels Blitz-Vakuum-Pyrolyse aus Arylhydroxymethylthiolen gebildet werden, dabei wird das Edukt mittels molekularer Strömung in den "Reaktor" eingebracht. Da die Arylhydroxymethylthiole in der Regel nur eine sehr geringe Flüchtigkeit haben, waren die Arenothiete meist nur in geringen Mengen darstellbar. Daher wurde in dieser Arbeit sowohl die Synthese neuer Arenothiete (gewinkelte Benzobisthiete) als auch eine Optimierung der bisherigen Synthesemethode angestrebt; diese erfolgt bevorzugt durch Variation der Pyrolyseedukte in Richtung zu potentiell höherflüchtigen Verbindungen.

Im Rahmen dieser Versuche war die Darstellung zweier Arenothiete ausgehend von cyclischen O,S-Acetalen als alternative Pyrolysevorstufen erfolgreich.

Ein besonderes Interesse speziell an Benzobisthieten begründet sich in ihrer generellen Fähigkeit zum Aufbau von bandartigen Strukturen durch Oligo- und Poly-Diels-Alder-Reaktionen. Durch die Synthese einiger Modellverbindungen konnte ihre prinzipielle Eignung zum Aufbau von Bandstrukturen auch für die beiden Benzobisthiete belegt werden.

Erzeugung höchster 3 He-Kernspinpolarisation durch metastabiles optisches Pumpen

In dieser Arbeit wird zum Erreichen hoher Kernspinpolarisationen die Methode des metastabilen optischen Pumpens benutzt. Das Verfahren beruht auf dem "Ubertrag des Drehimpulses absorbierter Photonen auf das hierbei angeregte Valenzelektron, welches durch Hyperfeinkopplung den Drehimpuls weiter auf den $^3$He-Kern transferiert. Da der Polarisationsprozess nur bei Dr"ucken von ca. 1~mbar effizient funktioniert, f"ur die meisten Anwendungen aber polarisiertes $^3$He bei einem Druck von $geq 1$~bar ben"otigt wird, muss das Gas nach der Aufpolarisation komprimiert werden. In unserer Arbeitsgruppe steht eine Maschine ("`Polarisator"') zur Verf"ugung, die das Gas polarisiert und anschlie"send komprimiert. Ziel dieser Dissertation ist, einerseits die Leistungsf"ahigkeit des Polarisators bez"uglich Maximalpolarisation und Gasfluss zu verbessern und andererseits den metastabilen Pumpprozess selbst genauer zu untersuchen.\ noindent Durch die Verwendung neuer Laser auf Basis der Fasertechnologie sowie einer systematischen Optimierung der optischen Komponenten konnten in abgeschlossenen Pumpzellen Rekord-Polarisationsgrade von $91pm 2$% erzielt werden.\ noindent Mit der Implementierung neuartiger Optiken und Laser am Mainzer Polarisator konnte die Leistungscharakteristik entscheidend verbessert werden. So wurde die erreichbare Polarisation bei identischer Produktionsrate um 20 Prozentpunkte gesteigert. Zurzeit sind maximale Polarisationsgrade von mehr als 75% im optischen Pumpvolumen erreichbar. Eine am Mainzer Triga-Reaktor durchgef"uhrte Polarisationsbestimmung ergab einen Wert von $72.7pm 0.7$%. Dies veranschaulicht die geringen Polarisationsverluste infolge der Gaskompression, des Transports und einer Lagerung "uber mehrere Stunden.\ noindent Zur Dynamik der geschwindigkeitsver"andernden St"o"se sowie zur Bestimmung der mittleren Photonen-Absorptionsrate wurde ein Modell entwickelt, welches auch experimentell best"atigt wurde. Damit konnte erstmalig das gemessene Absorptionsverhalten einer spektral schmalbandigen Laserdiode korrekt beschrieben werden.\ noindent Zudem stimmen die an so genannten abgeschlossenen Pumpzellen gemessenen extrem hohen Polarisationswerte mit theoretischen Vorhersagen "uberein, sofern der Druck im optischen Pumpvolumen geringer als 1~mbar ist und das $^3$He nicht durch Fremdgase verunreinigt ist. Bei derartigen Pumpzellen ist die gemessene Abh"angigkeit der Polarisation von Laserleistung, Metastabilendichte und falscher Zirkularkomponente mit der Theorie kompatibel.\

Synthesis and characterization of novel poly(imino ketone)s via palladium-catalyzed aryl amination

The challenge of the present work was to synthesize and to characterize new classes of N-containing polymers via palladium-catalyzed aryl amination. This work was inspired by a desire to combine the properties of high-performance polymers such as PEKs with those of N-containing conductive polymers such as polyaniline (PANI), poly(aromatic amides) (PAAs), and the ready synthesis of N-containing simple aromatic compound by the Buchwald-Hartwig reaction. Careful investigation of a model reaction was carried out to provide insights into the formation of side products which will have a negative effect upon the molecular weight or upon the materials properties of the desired polymers in the polycondensation reaction. In this thesis, five new different polymer classes namely, poly(imino ketone)s (PIKs), poly(imino acridine)s (PIAcs), poly(imino azobenzene)s (PIAzos), poly(imino fluorenone)s (PIFOs), and poly(imino carbazole)s (PICs) were synthesized and fully characterized by means of 1H-NMR, elemental analysis, UV, FT-IR, X-ray, GPC, TGA, DSC, DMA, and dielectric spectroscopy. To optimize the polycondensation process, the influence of the concentration, temperature, ligands and the reactivity of the halogen containing monomers were investigated. A temperature of 100-165 °C and a concentration of 30-36 % were found to be optimal for the palladium-catalyzed polycondensation to produce polymer with high molecular weight (Mn = 85 900, Mw = 474 500, DP = 126). Four different ligands were used successfully in the Pd-catalyzed process, of which the Pd/BINAP system was found to be the most effective catalyst, producing the highest yield and highest molecular weight polymers. It was found that the reactivity decreases strongly with increasing electronegativity of the halogen atoms, for example better yields, and higher molecular weights were obtained by using dibromo compounds than dichloro compounds while difluoro compounds were totally unreactive. Polymer analogous transformations, such as the protonation reaction of the ring nitrogens in PIAcs, or of the azobenzene groups of PIAzos, the photo and thermal cis-trans-isomerization of PIAzos, and of poly(imino alcohol)s were also studied. The values of the dielectric constants of PIKs at 1 MHz were in the range 2.71-3.08. These low values of the dielectric constant are lower than that of "H Film", a polyimide Kapton film which is one of the most preferred high-performance dielectrics in microelectronic applications having a dielectric constant of 3.5. In addition to the low values of the dielectric constants, PIKs have lower and glass transition temperatures (Tgs) than arimides such as Kapton which may make them more easily processable. Cyclic voltammetry showed that PICs exhibited low oxidation and reduction potentials and their values were shifted to low values with increasing degree of polymerization i.e. with increasing of the carbazole content in backbone of PICs (PIC-7, 0.44, 0.33 V, DP= 37, PIC-5, 0.63, 0.46, DP= 16, respectively).

Design, synthesis and photochemical studies of stilbenoid dendrimers

Stilbenoid dendrimers with stilbene in the periphery and stilbene in periphery as well as core were synthesized by convergent approach except 2nd generation dendrimer with stilbene in the periphery as well as in core (D-5). All dendrimers were characterized by standard techniques such as 1H NMR, 13C NMR, MS and IR spectroscopy. The MALDI-TOF technique proved to be very helpful in the identification of the 2nd generation dendrimer (D-5) with a mass of 3231 a.m.u. The dendrimers were designed in such a way that an intramolecular photochemical CC bond formation was favored. As two stilbene units of the same molecule were close enough so they preferred an intramolecular cyclic process except for zero generation dendrimers. Apart from the cycloaddition, some E/Z isomerization and oligomer formation was also observed on irradiation. These processes were observed by 1H NMR and MALDI-TOF MS. The photochemical behavior was also studied by UV absorption spectroscopy. Irradiating by monochromatic light led to an initial E/Z isomerization and by prolonged irradiation, an irreversible cyclic structure was formed. The choice of the wavelength of incident light is very important as irradiation at 320 nm leads to a reversible E/Z isomerization and a non-reversible cyclobutane formation, but irradiation at 340 nm favors the one-way process E Z. The [2+2] cycloaddition of molecule Tm2De was also studied by irradiating thin films on a quartz surface. An AFM image was taken before irradiation, after 3 sec irradiation and after long irradiation (1 hour). AFM studies show that a short irradiation leads to a cyclic structure as formation of hills of about 20-30 nm on the surface. A prolonged irradiation leads to a CC cross linking which can be monitored on AFM images as disappearance of hills. The roughness goes back to an almost smooth surface. These results prove a very complex material transport, which accompanies the reaction in the surface region.

Synthesis and surface modification of semiconductor nanocrystals

The last decade has witnessed an exponential growth of activities in the field of nanoscience and nanotechnology worldwide, driven both by the excitement of understanding new science and by the potential hope for applications and economic impacts. The largest activity in this field up to date has been in the synthesis and characterization of new materials consisting of particles with dimensions in the order of a few nanometers, so-called nanocrystalline materials. [1-8] Semiconductor nanomaterials such as III/V or II/VI compound semiconductors exhibit strong quantum confinement behavior in the size range from 1 to 10 nm. Therefore, preparation of high quality semiconductor nanocrystals has been a challenge for synthetic chemists, leading to the recent rapid progress in delivering a wide variety of semiconducting nanomaterials. Semiconductor nanocrystals, also called quantum dots, possess physical properties distinctly different from those of the bulk material. Typically, in the size range from 1 to 10 nm, when the particle size is changed, the band gap between the valence and the conduction band will change, too. In a simple approximation a particle in a box model has been used to describe the phenomenon[9]: at nanoscale dimensions the degenerate energy states of a semiconductor separate into discrete states and the system behaves like one big molecule. The size-dependent transformation of the energy levels of the particles is called “quantum size-effect”. Quantum confinement of both the electron and hole in all three dimensions leads to an increase in the effective bandgap of the material with decreasing crystallite size. Consequently, both the optical absorption and emission of semiconductor nanaocrystals shift to the blue (higher energies) as the size of the particles gets smaller. This color tuning is well documented for CdSe nanocrystals whose absorption and emission covers almost the whole visible spectral range. As particle sizes become smaller the ratio of surface atoms to those in the interior increases, which has a strong impact on particle properties, too. Prominent examples are the low melting point [8] and size/shape dependent pressure resistance [10] of semiconductor nanocrystals. Given the size dependence of particle properties, chemists and material scientists now have the unique opportunity to change the electronic and chemical properties of a material by simply controlling the particle size. In particular, CdSe nanocrystals have been widely investigated. Mainly due to their size-dependent optoelectronic properties [11, 12] and flexible chemical processibility [13], they have played a distinguished role for a number of seminal studies [11, 12, 14, 15]. Potential technical applications have been discussed, too. [8, 16-27] Improvement of the optoelectronic properties of semiconductor nanocrystals is still a prominent research topic. One of the most important approaches is fabricating composite type-I core-shell structures which exhibit improved properties, making them attractive from both a fundamental and a practical point of view. Overcoating of nanocrystallites with higher band gap inorganic materials has been shown to increase the photoluminescence quantum yields by eliminating surface nonradiative recombination sites. [28] Particles passivated with inorganic shells are more robust than nanocrystals covered by organic ligands only and have greater tolerance to processing conditions necessary for incorporation into solid state structures or for other applications. Some examples of core-shell nanocrystals reported earlier include CdS on CdSe [29], CdSe on CdS, [30], ZnS on CdS, [31] ZnS on CdSe[28, 32], ZnSe on CdSe [33] and CdS/HgS/CdS [34]. The characterization and preparation of a new core-shell structure, CdSe nanocrystals overcoated by different shells (CdS, ZnS), is presented in chapter 4. Type-I core-shell structures as mentioned above greatly improve the photoluminescence quantum yield and chemical and photochemical stability of nanocrystals. The emission wavelengths of type-I core/shell nanocrystals typically only shows a small red-shift when compared to the plain core nanocrystals. [30, 31, 35] In contrast to type-I core-shell nanocrystals, only few studies have been conducted on colloidal type-II core/shell structures [36-38] which are characterized by a staggered alignment of conduction and valence bands giving rise to a broad tunability of absorption and emission wavelengths, as was shown for CdTe/CdSe core-shell nanocrystals. [36] The emission of type-II core/shell nanocrystals mainly originates from the radiative recombination of electron-hole pairs across the core-shell interface leading to a long photoluminescence lifetime. Type-II core/shell nanocrystals are promising with respect to photoconduction or photovoltaic applications as has been discussed in the literature.[39] Novel type-II core-shell structures with ZnTe cores are reported in chapter 5. The recent progress in the shape control of semiconductor nanocrystals opens new fields of applications. For instance, rod shaped CdSe nanocrystals can enhance the photo-electro conversion efficiency of photovoltaic cells, [40, 41] and also allow for polarized emission in light emitting diodes. [42, 43] Shape control of anisotropic nanocrystals can be achieved by the use of surfactants, [44, 45] regular or inverse micelles as regulating agents, [46, 47] electrochemical processes, [48] template-assisted [49, 50] and solution-liquid-solution (SLS) growth mechnism. [51-53] Recently, formation of various CdSe nanocrystal shapes has been reported by the groups of Alivisatos [54] and Peng, [55] respectively. Furthermore, it has been reported by the group of Prasad [56] that noble metal nanoparticles can induce anisotropic growth of CdSe nanocrystals at lower temperatures than typically used in other methods for preparing anisotropic CdSe structures. Although several approaches for anisotropic crystal growth have been reported by now, developing new synthetic methods for the shape control of colloidal semiconductor nanocrystals remains an important goal. Accordingly, we have attempted to utilize a crystal phase control approach for the controllable synthesis of colloidal ZnE/CdSe (E = S, Se, Te) heterostructures in a variety of morphologies. The complex heterostructures obtained are presented in chapter 6. The unique optical properties of nanocrystals make them appealing as in vivo and in vitro fluorophores in a variety of biological and chemical investigations, in which traditional fluorescence labels based on organic molecules fall short of providing long-term stability and simultaneous detection of multiple emission colours [References]. The ability to prepare water soluble nanocrystals with high stability and quantum yield has led to promising applications in cellular labeling, [57, 58] deep-tissue imaging, [59, 60] and assay labeling [61, 62]. Furthermore, appropriately solubilized nanocrystals have been used as donors in fluorescence resonance energy transfer (FRET) couples. [63-65] Despite recent progress, much work still needs to be done to achieve reproducible and robust surface functionalization and develop flexible (bio-) conjugation techniques. Based on multi-shell CdSe nanocrystals, several new solubilization and ligand exchange protocols have been developed which are presented in chapter 7. The organization of this thesis is as follows: A short overview describing synthesis and properties of CdSe nanocrystals is given in chapter 2. Chapter 3 is the experimental part providing some background information about the optical and analytical methods used in this thesis. The following chapters report the results of this work: synthesis and characterization of type-I multi-shell and type-II core/shell nanocrystals are described in chapter 4 and chapter 5, respectively. In chapter 6, a high–yield synthesis of various CdSe architectures by crystal phase control is reported. Experiments about surface modification of nanocrystals are described in chapter 7. At last, a short summary of the results is given in chapter 8.

Computational studies on the structure and stabilities of magnetic inter-metallic compounds

The purpose of this thesis is to further the understanding of the structural, electronic and magnetic properties of ternary inter-metallic compounds using density functional theory (DFT). Four main problems are addressed. First, a detailed analysis on the ternary Heusler compounds is made. It has long been known that many Heusler compounds ($X_2YZ$; $X$ and $Y$ transition elements, $Z$ main group element) exhibit interesting half-metallic and ferromagnetic properties. In order to understand these, the dependence of magnetic and electronic properties on the structural parameters, the type of exchange-correlation functional and electron-electron correlation was examined. It was found that almost all Co$_2YZ$ Heusler compounds exhibit half-metallic ferromagnetism. It is also observed that $X$ and $Y$ atoms mainly contribute to the total magnetic moment. The magnitude of the total magnetic moment is determined only indirectly by the nature of $Z$ atoms, and shows a trend consistent with Slater-Pauling behaviour in several classes of these compounds. In contrast to experiments, calculations give a non-integer value of the magnetic moment in certain Co$_2$-based Heusler compounds. To explain deviations of the calculated magnetic moment, the LDA+$U$ scheme was applied and it was found that the inclusion of electron-electron correlation beyond the LSDA and GGA is necessary to obtain theoretical description of some Heusler compounds that are half-metallic ferromagnets. The electronic structure and magnetic properties of substitutional series of the quaternary Heusler compound Co$_2$Mn$_{1-x}$Fe$_x$Si were investigated under LDA+$U$. The calculated band structure suggest that the most stable compound in a half-metallic state will occur at an intermediate Fe concentration. These calculated findings are qualitatively confirmed by experimental studies. Second, the effect of antisite disordering in the Co$_2$TiSn system was investigated theoretically as well as experimentally. Preservation of half-metallicity for Co$_2$TiSn was observed with moderate antisite disordering and experimental findings suggest that the Co and Ti antisites disorder amounts to approximately 10~% in the compound. Third, a systematic examination was carried out for band gaps and the nature (covalent or ionic) of bonding in semiconducting 8- and 18-electron or half-metallic ferromagnet half-Heusler compounds. It was found that the most appropriate description of these compounds from the viewpoint of electronic structures is one of a $YZ$ zinc blende lattice stuffed by the $X$ ion. Simple valence rules are obeyed for bonding in the 8- and 18-electron compounds. Fourth, hexagonal analogues of half-Heusler compounds have been searched. Three series of compounds were investigated: GdPdSb, GdAutextit{X} (textit{X} = Mn, Cd and In) and EuNiP. GdPdSb is suggested as a possible half-metallic weak ferromagnet at low temperature. GdAutextit{X} (textit{X} = Mn, Cd and In) and EuNiP were investigated because they exhibit interesting bonding, structural and magnetic properties. The results qualitatively confirm experimental studies on magnetic and structural behaviour in GdPdSb, GdAutextit{X} (textit{X} = Mn, Cd and In) and EuNiP compounds. ~

Structure and properties of intermetallic ternary rare earth compounds

The so called material science is an always growing field in modern research. For the development of new materials not only the experimental characterization but also theoretical calculation of the electronic structure plays an important role. A class of compounds that has attracted a great deal of attention in recent years is known as REME compounds. These compounds are often referred to with RE designating rare earth, actinide or an element from group 1 - 4, M representing a late transition metal from groups 8 - 12, and E belonging to groups 13 - 15. There are more than 2000 compounds with 1:1:1 stoichiometry belonging to this class of compounds and they offer a broad variety of different structure types. Although many REME compounds are know to exist, mainly only structure and magnetism has been determined for these compounds. In particular, in the field of electronic and transport properties relatively few efforts have been made. The main focus in this study is on compounds crystallizing in MgAgAs and LiGaGe structure. Both structures can only be found among 18 valence electron compounds. The f electrons are localized and therefor not count as valence electrons. A special focus here was also on the magnetoresistance effects and spintronic properties found among the REME compounds. An examination of the following compounds was made: GdAuE (E = In, Cd, Mg), GdPdSb, GdNiSb, REAuSn (RE = Gd, Er, Tm) and RENiBi (RE = Pr, Sm, Gd - Tm, Lu). The experimental results were compared with theoretic band structure calculations. The first half metallic ferromagnet with LiGaGe structure (GdPdSb) was found. All semiconducting REME compounds with MgAgAs structure show giant magnetoresistance (GMR) at low temperatures. The GMR is related to a metal-insulator transition, and the value of the GMR depends on the value of the spin-orbit coupling. Inhomogeneous DyNiBi samples show a small positive MR at low temperature that depends on the amount of metallic impurities. At higher fields the samples show a negative GMR. Inhomogeneous nonmagnetic LuNiBi samples show no negative GMR, but a large positive MR of 27.5% at room temperature, which is interesting for application.

Photovernetzbare flüssigkristalline Polymere unterschiedlicher Kettentopologien

„Photovernetzbare flüssigkristalline Polymere unterschiedlicher Kettentopologien“, Patrick Beyer, Mainz 2007 Zusammenfassung In der vorliegenden Arbeit wurde die Synthese und Charakterisierung flüssigkristalliner Elastomere unterschiedlicher Polymertopologien vorgestellt. Dabei wurden Systeme synthetisiert, bei denen die mesogenen Einheiten entweder als Seitengruppen an ein Polymerrückgrat angebunden (Seitenkettenelastomere) oder direkt in die Polymerkette integriert (Hauptkettenelastomere) sind (siehe Abbildung). Bezüglich der Seitenkettensysteme konnten erstmals photovernetzbare smektische Seitenkettenpolymere, in denen aufgrund der Anknüpfung eines photoisomerisierbaren Azobenzols eine Photo- modulation der ferroelektrischen Eigenschaften möglich ist, dargestellt werden. Homöotrop orientierte freistehende Filme dieser Materialien konnten durch Spincoaten dargestellt und unter Ausnutzung des Dichroismus der Azobenzole durch geeignete Wahl der Bestrahlungsgeometrie photovernetzt werden. Aufbauend auf diesen Untersuchungen wurde anhand eines nicht vernetzbaren Modellsystems im Detail der Einfluss der trans-cis Isomerisierung des Azobenzols auf die ferroelektrischen Parameter untersucht. Durch zeitaufgelöste Messungen der Absorption der Azobenzole, der spontanen Polarisation und des Direktorneigungswinkels und Auswertung der kinetischen Prozesse konnte eine lineare Abhängigkeit der ferroelektrischen Eigenschaften vom Grad der Isomerisierungsreaktion festgestellt werden. Durch Vergleich dieser in der flüssigkristallinen Phase erhaltenen Ergebnisse mit der Kinetik der thermischen Reisomerisierung in Lösung (Toluol) konnte ferner eine deutliche Reduzierung der Relaxationszeiten in der anisotropen flüssigkristallinen Umgebung festgestellt und auf eine Absenkung der Aktivierungsenergie zurückgeführt werden. Makroskopische Formänderungen der Seitenkettenelastomere am Phasenübergang von der flüssigkristallinen in die isotrope Phase konnten jedoch nicht festgestellt werden. Aus diesem Grund wurden neue Synthesestrategien für die Darstellung von Hauptkettenelastomeren entwickelt, die sich aufgrund der direkten Kopplung von flüssigkristallinem Ordnungsgrad und Polymerkettenkonformation besser für die Herstellung thermischer Aktuatoren eignen. Auf Basis flüssigkristalliner Polymalonate konnten dabei lateral funktionalisierte smektische Hauptkettenpolymere synthetisiert werden, welche erstmals die Darstellung von LC-Hauptkettenelastomeren durch Photovernetzung in der flüssigkristallinen Phase erlauben. Durch laterale Bromierung konnte in diesen Systemen die Kristallisationstendenz der verwendeten Biphenyleinheiten unterdrückt werden. Bezüglich der Photovernetzung konnten zwei neue Synthesemethoden entwickelt werden, bei denen der Vernetzungsschritt entweder durch radikalische Polymerisation lateral angebundener Acrylatgruppen oder durch photoaktive Benzophenongruppen erfolgte. Basierend auf den Benzophenon funktionalisierten Systemen konnte ein neuartiges Verfahren zur Darstellung makroskopisch orientierter Hauptkettenelastomere durch Photovernetzung entwickelt werden. Die Elastomerproben, deren Ordnungsgrad durch Röntgenuntersuchungen ermittelt werden konnte, zeigen am Phasenübergang von der flüssigkristallinen in die isotrope Phase eine reversible Formänderung von 40%. Im Gegensatz zu anderen bekannten smektischen Systemen konnten die in dieser Arbeit vorgestellten Elastomere ohne Zerstörung der Phase bis zu 60% entlang der smektischen Schichtnormalen gestreckt werden, was im Kontext einer geringen Korrelation der smektischen Schichten in Hauptkettenelastomeren diskutiert wurde.

Unconventional correlated systems

This work comprises three different types of unconventional correlated systems.rnChapters 3-5 of this work are about the open shell compounds Rb4O6 and Cs4O6. These mixed valent compounds contain oxygen in two different modifications: the closed-shell peroxide anion is nonmagnetic, whereas the hyperoxide anion contains an unpaired electrons in an antibonding pi*-orbital. Due to this electron magnetic ordering is rendered possible. In contrast to theoretical predictions, which suggested half-metallic ferromagnetism for Rb4O6,rndominating antiferromagnetic interactions were found in the experiment. Besidesrna symmetry reduction due to the mixed valency, strong electronic correlations of this highly molecular system determine its properties; it is a magnetically frustrated insulator. The corresponding Cs4O6 was found to show similar properties.rnChapters 6-9 of this work are about intermetallic Heusler superconductors. rnAll of these superconductors were rationally designed using the van Hove scenario as a working recipe. A saddle point in the energy dispersion curve of a solid leads to a van Hove singularity in the density of states. In the Ni-based and Pd-based Heusler superconductors presented in this work this sort of a valence instability occurs at the high-symmetry L point and coincides or nearly coincides with the Fermi level. The compounds escape the high density of states at the Fermi energy through a transition into the correlated superconducting state.rnChapter 10 of this work is about the tetragonally distorted ferrimagnetic DO22 phase of Mn3Ga. This hard-magnetic modification is technologically useful for spin torque transfer applications. The phase exhibits two different crystallographic sites that are occupied by Mn atoms and can thus be written as Mn2MnGa. The competition between the mainly itinerant moments of the Mn atoms at the Wyckoff position 4d and the localized moments of the Mn atoms at the Wyckoff position 2b leads to magnetic correlations. The antiferromagnetic orientation of these moments determines the compound to exhibit a resulting magnetic moment of approximately 1 µB per formula unit in a partially compensated ferrimagnetic configuration.

Heusler compounds as thermoelectric materials

Heusler compounds as thermoelectric materialsrnrnThis work reports on Heusler and Half Heusler compounds and their thermoelectric properties. Several compounds were synthesized and their resistivity, Seebeck coefficient, thermal conductivity, and the figure of merit were determined. The results are presented in the following chapters.rnrnIn chapter 3 Co was substituted with Ni and Fe in the series TiCo1-x(Fe0.5Ni0.5)xSb. The substitution lead to a reduced loss of Sb during the synthesis. Further the Seebeck coefficient was increased and the thermal conductivity was reduced. These observations can be used to significantly improve the quality of TiCoSb based compounds in thermoelectric applications. rnrnIn chapter 4 the series TiCo1-xNixSnxSb1-x was investigated. Ni was substituted with Co and Sn with Sb. Especially for high Ni concentrations the figure of merit was enhanced compared to unsubstituted TiCoSb. This enhancement is based on the strong reduction of the thermal conductivity. The found values are among the lowest that have been determined up to date for Heusler compounds. rnrnIn chapter 5 Li containing Heusler compounds were theoretically and experimentally investigated. Li containing Heusler compounds are of special interest because the Li atoms scatter phonons efficiently. Therefore the thermal conductivity is decreased. The thermoelectric properties and especially the thermal conductivity are investigated in this chapter.rnrnIn chapter 6 several substitutions of TiCoSb were investigated. In the series TiCo1+xSb additional Co was introduced into the vacancies of the compound and the effect on the thermoelectric properties was measured. In the series TiCo1-xCuxSb Co was substituted with Cu. No significant enhancement of the ZT value were observed. In the series TiCoSb1-xBix Sb was substituted by Bi. The thermoelectric properties were significantly enhanced for small Bi concentrations. The Seebeck coefficient was increased and the resistivity was reduced at the same time. This unusual phenomenon is explained by band structure calculations.rnrnIn chapter 7 the material class of half metallic ferromagnets was investigated as a new materialclass for thermoelectric applications. The 26 valence electron compounds Co2TiSi, Co2TiGe, and Co2TiSn were used as model systems. The transport properties were determined theoretically. Then the properties were measured and compared to the calculated ones. The calculated values are in good agreement with the experimentally determined ones. The observed Seebeck coefficient has a big value and is nearly constant above the Curie temperature. This makes the materials appealing for the use as materials in thermocouples.rn

Electrostatically self-assembled nanoparticles based on biomolecules

In this work, two different systems were investigated to develop fundamental understanding of the self-assembly behavior of polyelectrolytes and small organic counterions with a certain geometry. Complexes formed were characterized by light scattering in solution, as well as UV-Vis spectroscopy, analytical ultracentrifugation, gel electrophoresis, zeta potential and IR spectroscopy. The morphologies of the aggregates were observed by AFM in dried state on surface. The charge ratio, the valence and the structure of the counterion were shown to represent key parameters in the complexation. The influence of polyelectrolyte type and molecular weights was also determined for the structure formed.rnrnOne system was mainly focused on the association of double-strand DNA with non-intercalating divalent and tetravalent organic counterions. The other model system involved linear NaPSS and oligolysines. In addition, various influences on the morphology of the charged self-assembly complexes in AFM studies were discussed. It was shown that electrostatic self-assembly of DNA and non-intercalating counterions as well as of a linear synthetic polyelectrolyte with oligolysine counterions that can build mutual hydrogen bonds can yield supramolecular aggregates of a defined size. Various morphologies (flower-like, rod-like, toroidal and spherical) of the assemblies were obtained for different combinations of polyelectrolyte and counterions. Results presented in this work are of importance for the fundamental understanding of the association behavior of various polyelectrolytes and organic counterions. The selection of biopolymers for the study may give an opportunity to transfer the basic research results into biological applications, such as gene therapy or drug delivery.rn