The function of titanium- and nickel-silicides is to lower the series resistance and contact resistivity in gate, source and drain contacts of an integrated circuit transistor. With decreasing dimensions, the low resistivity C54 TiSi2 is not formed and stays in its high resistivity phase C49. It was found that a layer of niobium interposed between titanium and silicon, which is supposed to promote the C54 phase, led to the formation of the high resistivity C40 (Ti,Nb)Si2 in both small and large contacts. Increased interest in Si1-xGex layers led to the inclusion of the Ni-Si-Ge system in this project. The interaction between nickel and poly-Si0.42Ge0.58 was found to be different from nickel and poly-silicon in the meaning of the phases formed during high temperature annealing. High-resistivity NiSi2 was formed at 750°C, but nickel and Si0.42Ge0.58 formed no disilicide. A massive out-diffusion of germanium from the NiSi1-uGeu resulted in agglomeration at lower temperatures than for NiSi. This was ascribed to the larger enthalpy of formation for nickel reacting with silicon than with germanium. Ternary phase diagrams, with and without the disilicide phase, were calculated. According to the tie lines, NiSi1-uGeu will be in thermodynamic equilibrium with Si1-xGex when u is smaller than x. This was confirmed experimentally, where a balanced germanium concentration in NiSi1-uGeu and Si1-xGex, stabilized the germanosilicide. When nickel interacted with strained and relaxed silicon-germanium it was established that a strained substrate led to a morphologically unstable NiSi1-uGeu. The germanosilicide was highly textured on both (001) and (111) substrates. The texturing was explained by the absence of Ni(SiGe)2 which forced NiSiGe to reorient so as not to resemble a digermanosilicide at the film/substrate interface. NiSi0.82Ge0.18 formed on p+-Si0.82Ge0.18 in CBKs grew laterally under the SiO2, defining the contact hole. The contact resistivity extracted by 3D modelling was 5×10-8 Ωcm2.

Black liquors are presently combusted in recovery boilers where the inorganic cooking chemicals are recovered and the energy in the organic material is converted to steam and electricity. A new technology, developed by Chemrec AB, is black liquor gasification (BLG). BLG has more to offer compared to the recovery boiler process, in terms of on-site generation of electric power, liquid fuel and process chemicals. A prerequisite for both optimization of existing processes and the commercialization of BLG is better understanding of the physical and chemical processes involved including interactions with the refractory lining. The chemistry in the BLG process is very complex and to minimize extensive and expensive time-consuming studies otherwise required accurate and reliable model descriptions are needed for a full understanding of most chemical and physical processes as well as for up-scaling of the new BLG processes. However, by using these calculated model results in practice, the errors in the state of the art thermochemical data have to be considered. An extensive literature review was therefore performed to update the data needed for unary, binary and higher order systems. The results from the review reviled that there is a significant range of uncertainty for several condensed phases and a few gas species. This resulted in experimental re-determinations of the binary phase diagrams sodium carbonate-sodium sulfide (Na2CO3-Na2S) and sodium sulfate-sodium sulfide (Na2SO4-Na2S) using High Temperature Microscopy (HTM), High Temperature X-ray Diffraction (HT-XRD) and Differential Thermal Analysis (DTA). For the Na2CO3-Na2S system, measurements were carried out in dry inert atmosphere at temperatures from 25 to 1200 °C. To examine the influence of pure CO2 atmosphere on the melting behavior, HTM experiments in the same temperature interval were made. The results include re-determination of liquidus curves, in the Na2CO3 rich area, melting points of the pure components as well as determination of the extent of the solid solution, Na2CO3(ss), area. The thermal stability of Na2SO3 was studied and the binary phase diagram Na2SO4-Na2S was re-determined. The results indicate that Na2SO3 can exist for a short time up to 750 °C, before it melts. It was also proved that a solid/solid transformation, not reported earlier, occurs at 675 ± 10 °C. At around 700 °C, Na2SO3 gradually breaks down within a few hours, to finally form the solid phases Na2SO4 and Na2S. From HTM measurements a metastable phase diagram including Na2SO3, as well as an equilibrium phase diagram have been constructed for the binary system Na2SO4-Na2S. Improved data on Na2S was experimentally obtained by using solid-state EMF measurements. The equilibrium constant for Na2S(s) was determined to be log Kf(Na2S(s)) (± 0.05) = 216.28 – 4750(T/K)–1 – 28.28878 ln (T/K). Gibbs energy of formation for Na2S(s) was obtained as ΔfG°(Na2S(s))/(kJ mol–1) (± 1.0) = 90.9 – 4.1407(T/K) + 0.5415849(T/K) ln (T/K). The standard enthalpy of formation of Na2S(s) was evaluated to be ΔfH°(Na2S(s), 298.15 K)/(kJ mol–1) (± 1.0) = – 369.0. The standard entropy was evaluated to be S°(Na2S(s), 298.15 K)/(J mol–1 K–1) (± 2.0) = 97.0. Analyses of used refractory material from the Chemrec gasifier were also performed in order to elucidate the stability of the refractory lining. Scanning electron microscopy (SEM) analysis revealed that the chemical attack was limited to 250-300 μm, of the surface directly exposed to the gasification atmosphere and the smelt. From XRD analysis it was found that the phases in this surface layer of the refractory were dominated by sodiumaluminosilicates, mainly Na1.55Al1.55Si0.45O4.

This research addresses and illuminates a little understood region of miscible polymer mixtures and demonstrates a new means of separating wax from such blends. The method, termed Deformation Induced Phase Segregation potentially eliminates need of toxic processing solvents for wax removal or recovery in these types of blends. Previous theories of polymer combinations address them exclusively as solutions or as blends, two independent classes having very different behaviors. This study provides bridge connecting these two classes by identifying crossover points between them and the behaviors exhibited therein. The blends of this form were found to be semi-miscible, forming a homogenous phase in the melt but a two-phase system in the solid, with the rheological behavior influenced by the polymer's molecular weight and architecture. It also demonstrates practical promise of this regime by introducing a mechanical compression process to separate the wax phase from such a type of blend. This process potentially permits production of ultra-high molecular weight polyethylene (UHMwPE) films and fibers by melt processing, thereby obviating need of otherwise essential but expensive and environmentally unfriendly toxic solvents.

The complete and accurate thermodynamic and kinetic description of any systemis crucialfor understanding and predicting its properties. A particular interest is in systemsthat are used for some practical applications and have to be constantly improved usingmodification of their composition and structure. This task can be quite accuratelysolved at a fundamental level by density functional theory methods. Thesemethods areapplied to two practically important systems Fe-Cr and TiC-ZrC.The elastic properties of pure iron and substitutionally disordered Fe-Cr alloy are investigatedas a function of temperature and concentration using first-principles electronicstructurecalculations by the exact muffin-tin orbitals method. The temperature effectson the elastic properties are included via the electronic, magnetic, and lattice expansioncontributions. It is shown that the degree of magnetic order in both pure iron andFe90Cr10 alloy mainly determines the dramatic change of the elastic anisotropy of thesematerials at elevated temperatures. A peculiarity in the concentration dependence ofthe elastic constants in Fe-rich alloys is demonstrated and related to a change in theFermi surface topology.A thermodynamic model for the magnetic alloys is developed from first principles andapplied to the calculation of bcc Fe-Cr phase diagram. Various contributions to the freeenergy (magnetic, electronic, and phonon) are estimated and included in the model. Inparticular, it is found that magnetic short range order effects are important just abovethe Curie temperature. The model is applied for calculating phase equilibria in disorderedbcc Fe-Cr alloys. Model calculations reproduce a feature known as a Nishizawahorn for the Fe-rich high-temperature part of the phase diagram.The investigation of the TiC-ZrC system includes a detailed study of the defect formationenergies and migration barriers of point defects and defect complexes involvedin the diffusion process. It is found, using ab initio atomistic simulations of vacancymediateddiffusion processes in TiC and ZrC, that a special self-diffusion mechanism isoperative for metal atom diffusion in sub-stoichiometric carbides. It involves a noveltype of a stable point defect, a metal vacancy ”dressed” in a shell of carbon vacancies.It is shown that this vacancy cluster is strongly bound and can propagate through thelattice without dissociating. / <p>QC 20120604</p> / HERO-M

The availability of high quality thermodynamic data on solid solutions and compounds present in multicomponent systems assists in optimizing processing parameters for synthesis, and in evaluating stability domains and materials compatibility under different conditions. Several oxide systems of technological interest, for which thermodynamic data was either not available or is inconsistent were selected for study. Thermodynamic properties of phases present in the binary systems Nb-O and Ta-O were measured in the temperature range from 1000 to 1300 K using solid state electrochemical cells based on (Y2O3) ThO2 as the electrolyte. Based on these measurements and more recent data on heat capacity and phase transitions reported in the literature, Gibbs energy of formation for NbO, NbO2, NbO2.422, Nb2O5-x and Ta2O5 were reassessed. Significant improvements in the data for NbO2, Nb2O5 and Ta2O5 are suggested. The pseudo binary system MoO2-TiO2 was investigated because of the inconsistency between the phase diagram and thermodynamic properties of the solid solution reported in the literature. Based on new electrochemical measurements, a new improved phase diagram for the system MoO2-TiO2, incorporating recently discovered monoclinic to tetragonal phase transition in MoO2 at 1533 K, is presented. Isothermal section of the phase diagram for the ternary systems Cr-Rh-O and Ta-Rh-O and thermodynamic properties of ternary oxides CrRhO3 and TaRhO4 were measured for the first time in the temperature range from 900 to 1300 K. Phase relations for these systems have been computed as a function of oxygen potential at fixed temperature and as a function of temperature at selected oxygen partial pressures. Metal-spinel-corundum three-phase equilibrium in the Ni-Al-Cr-O system at 1373 K has been explored because of its relevance to high temperature corrosion of super alloys. The Gibbs energy of mixing of spinel solid solution was derived from the tie-line data and is compared with the values calculated from cation distribution models. An oxygen potential diagram is developed for the decomposition of spinel solid solution to nickel and corundum solid solution at 1373 K under reducing conditions. The high temperature thermodynamic properties of the phases present in quaternary systems Ca-Co-Al-O and Ca-Cu-Ti-O have been measured by solid state electrochemical cells based on stabilized zirconia. Gibbs energies of formation of the quaternary oxides Ca3CoAl4O10 in the temperature range from 1150 to1500 K and CaCu3Ti4O12 in the range from 900 to 1350 K are presented. Chemical potential diagrams have been computed for the system Al2O3-CaO-CoO at 1500 K. The oxygen potential corresponding to the decomposition of the complex perovskite CaCu3Ti4O12 (CCTO) has been calculated as a function of temperature from the emf of the cell. The effect of the oxygen partial pressure on the phase relations in the pseudo-ternary system CaO-(CuO/Cu2O)-TiO2 at 1273 K has been evaluated. The phase diagrams are useful for the control of the secondary phases that form during synthesis of CCTO, a material exhibiting colossal dielectric response.

Silicium wird während des Ätzvorgangs von Solar-Wafern mit HF-HNO3-Mischungen hauptsächlich zu Hexafluorosilicat (SiF62-) umgewandelt, welches sich negativ auf den Ätzabtrag, die Reaktivität der Ätzlösung und die Oberflächeneigenschaften der Wafer auswirkt. Möglichkeiten, das Silicium als SiF62- abzutrennen, sollten in dieser Arbeit untersucht werden. Voraussetzung für Abtrennungsuntersuchungen war eine quantitative Bestimmung des SiF62- in Ätzlösungen mittels Ramanspektrometrie. Als Abreicherungs-möglichkeiten des Siliciums in Form von Hexafluorosilicat wurden einerseits das Ausfrieren als Hydrat der Hexafluorokieselsäure (H2SiF6•nH2O) und andererseits die Fällung als K2SiF6 untersucht. Die experimentellen Ergebnisse wurden jeweils gestützt durch thermodynamische Modellierungen: die Tieftemperaturphasendiagramme wurden durch eine modifizierte BET-Modellierung bestätigt, die Löslichkeiten durch Nutzung des SIT-Ansatzes. Demnach erwies sich die Ausfällung als K2SiF6 als ökonomisch günstigste Variante.

In part to search for a possible critical point (CP) in the phase diagram of hot nuclear matter, a beam energy scan was performed at the Relativistic Heavy-Ion Collider at Brookhaven National Laboratory. The Solenoidal Tracker at RHIC (STAR) collected Au+Au data sets at beam energies, √sNN , of 7.7, 11.5, 19.6, 27, 39, 62.4, and 200 GeV. Such a scan produces hot nuclear matter at different locations in the phase diagram. Lattice and phenomenological calculations suggest that the presence of a CP might result in divergences of the thermodynamic susceptibilities and correlation lengths. The statistical moments of the identified-particle multiplicity distributions directly depend on both the thermodynamic susceptibilities and correlation lengths, possibly making the shapes of these multiplicity distributions sensitive tools for the search for the critical point. The statistical moments of the multiplicity distributions of a number of different groups of identified particle species were analyzed. Care was taken to remove a number of experimental artifacts that can modify the shapes of the multiplicity distributions. The observables studied include the lowest four statistical moments (mean, variance, skewness, kurtosis) and some products of these moments. These observables were compared to the predictions from several approaches lacking critical behavior, such as the Hadron Resonance Gas model, mixed events, (negative) binomial, and Poisson statistics. In addition, the data were analyzed after gating on the event-by-event antiproton-to-proton ratio, which is expected to more tightly constrain the event trajectories on the phase diagram.

The phase diagram of the Mg-Pd system was redetermined in the range from 50 at. % Mg to 100 at. % Mg. It contains several intermediate phases with some of them being complex metallic alloy phases (CMAs), i.e., characterized by (i) giant unit cells with more than hundred atoms, (ii) inherent disorder, (iii) the presence of a cluster substructure. Phase fields and heterogeneous equilibria of the intermediate phases β- Mg6Pd, γ-Mg57Pd13, δ-Mg56.4Pd13.6, ε-Mg306Pd77, ζ-Mg64Pd17, η-Mg3Pd, θ-Mg5Pd2, ι- Mg2Pd and κ-MgPd were determined. The first five phases are CMAs with Mackay clusters as fundamental structural units. The crystal structure of the most magnesium-rich compound β-Mg6Pd was redetermined. It was found to be more complicated than previously thought due to correlated disorder of only two atom sites in the cubic unit cell. The γ-, ε- and ζ-phases form in a small window of temperature (50 oC) and composition (3 at. %) close to 80 at. % Mg. A new structure type was assigned to Mg3Pd (Cu3P, P63cm). The single phase field of the θ-phase is caused by constitutional vacancies. The new ι-phase crystallizes with NiTi2 structure-type. / Das Phasendiagramm des Systems Mg–Pd wurde im Bereich von 50 bis 100 At.-% Mg neu bestimmt. In diesem Phasendiagramm finden sich mehrere intermediäre Phasen, darunter auch komplexe intermetallische Verbindungen (engl.: complex intermetallic alloys, CMAs). CMAs sind charakterisiert durch (i) große Elementarzellen mit mehr als einhundert Atomen, (ii) intrinsischer Fehlordnung und (iii) dem Vorhandensein einer Cluster- Substruktur. Die Phasenfelder und heterogenen Gleichgewichte der intermediären Phasen β-Mg6Pd, γ- Mg57Pd13, δ-Mg56.4Pd13.6, ε-Mg306Pd77, ζ-Mg64Pd17, η-Mg3Pd, θ-Mg5Pd2, ι-Mg2Pd und κ- MgPd wurden bestimmt. Die ersten fünf der eben genannten Phasen sind CMAs mit Mackay Clustern als fundamentales strukturelles Einheit. Alle übrigen Phasen besitzen einen einfacheren kristallografischen Aufbau. Die Kristallstruktur der Mg-reichsten Verbindung β-Mg6Pd wurde neu bestimmt und ist weitaus sich als komplizierter als bisher angenommen. Die Ausdehnung des Einphasenfeldes von β-Mg6Pd lässt sich jedoch sehr einfach mit korrelierter Fehlordnung von lediglich zwei Atomen in der kubischen Elementarzelle verstehen. Die γ-, ε-, und ζ-Phasen bilden sich in einem schmalen Temperatur- (50 °C) und Zusammensetzungsbereich (3 at. %) nahe 80 at. % Mg. Der Verbindung Mg3Pd (Cu3P, P63cm) wurde ein neuer Strukturtyp zugewiesen. Die Ausdehnung des Einphasenfeldes der θ-Phase lässt sich mit dem Einbau konstitutioneller Leerstellen erklären. Die neue ι-Phase kristallisiert im NiTi2 Strukturtyp.

Im Mittelpunkt dieser Arbeit standen die Darstellung und Charakterisierung ternärer Bismutsubchloride unter Einbau von Übergangsmetallen der 8., 9. und 10. Gruppe. Durch Vorlage eines hohen Chloranteils in der Synthese wurde die &amp;quot;chemische Schere&amp;quot; der Oxidation so stark wirksam, dass in den Verbindungen die gewünschten voneinander isolierten Cluster aus Metallatomen vorlagen. Die Verbindungen Bi12PtCl12, Bi12-xRhCl13-x, Bi12-xIrCl13-x (x &amp;lt; 1) und Bi6,67PtCl12 wurden als Pulver und als Kristalle durch Festkörperreaktionen bei 1273 K in Quarzglasampullen hergestellt. Die schwarz glänzenden, würfelförmigen Kristalle sind luftstabil, in verdünnten Mineralsäuren und in organischen Lösungsmitteln beständig. Die Zusammensetzungen wurden mit EDX-Analysen und Röntgenbeugung am Einkristall bestimmt. Zur weiteren Charakterisierung wurden quantenchemische Rechnungen, ramanspektroskopische Untersuchungen, Messungen der magnetischen Suszeptibilität und der elektrischen Leitfähigkeit durchgeführt. Kristalle der Verbindung Bi12PtCl12 täuschen ein rhomboedrisches Kristallsystem vor, die Struktur konnte in der Raumgruppe P 1 als nahezu perfekter Inversionszwilling eines Achsendrillings gelöst werden. Auf den Eckplätzen der pseudorhomboedrischen Elementarzelle befinden sich [PtBi6Cl12]2- -Cluster und in der Mitte ein (Bi6)2+ -Polykation. Dieses (Bi6)2+ -Polykation in Form eines geöffneten Oktaeders bestätigt experimentell Vorhersagen von Kuznetsov et al. Nach den Regeln von Wade ist das Polykation mit 2 x 6 + 4 = 16 Gerüstelektronen als nido-Cluster zu verstehen. Die Schwerpunkte der Anionen und Kationen fügen sich zu einer dem CsCl-Typ analogen Anordnung zusammen. Mit einer vollständigen Besetzung aller Bismutlagen in der Mitte der Elementarzelle kann Bi12PtCl12 eine Schlüsselrolle zugeordnet werden, die sozusagen den Prototyp für diesen Strukturtyp darstellt. Die weiteren Verbindungen stellen unterbesetzte Varianten dar und können von Bi12PtCl12 abgeleitet werden. Im Verlauf der Untersuchungen zu den ternären Subchloriden in den Systemen wurden wenige Kristalle der binären Verbindung Bi7Cl10 erhalten. Die Tatsache, dass es sich um eine neue binäre Phase im recht stark untersuchten Gebiet Bismut-Chlor handelte führte zu einer neuerlichen, systematischen Überprüfung des Systems Bi/Cl. Mittels thermischer Analysen wurde das Zustandsdiagramm Bi/BiCl3 präzisiert. Bi7Cl10 zersetzt sich bereits bei 190 °C peritektoid in Bi6Cl7 und BiCl3 Bi7Cl10(s) = Bi6Cl7(s) + BiCl3(g). Das Zustandsbarogramm des binären Systems wurde über Gesamtdruckmessungen im Membran-Nullmanometer erstmalig bestimmt. Aus den Druckfunktionen der Bismutchloride sowie aus Messungen der Molwärme von Bi6Cl7 wurden die thermodynamischen Standarddaten abgeleitet. Unter Verwendung dieser Daten wurden thermodynamische Modellierungen der Festkörper-Gasphasen-Gleichgewichte durchgeführt, mit deren Hilfe die Synthese von Bi7Cl10 optimiert werden konnte. Die phasenreine Gasphasenabscheidung von Bi7Cl10 ist aufgrund der Kondensation der dominierenden Gasphasenspezies BiCl und BiCl3 im Existenzbereich der Verbindung oberhalb des Zersetzungspunktes (190 °C) nicht möglich. Im Existenzgebiet von Bi7Cl10 kommt der Transport dann wegen der resultierenden Partialdrücke unmittelbar zum Erliegen. Aus Röntgenbeugungsuntersuchungen an Einkristallen geht hervor, dass Bi7Cl10 bei Raumtemperatur in der tetragonalen Raumgruppe I 41/a c d mit a = 28,235(3) und c = 39,950(4) Å kristallisiert (Z = 64). Analog zu Bi6Cl7 = ((Bi9)5+)[(Bi3Cl14)5-] kann Bi7Cl10 unter Verdopplung der Summenformel als ((Bi9)5+)[(Bi5Cl20)5-] formuliert werden. In der Kristallstruktur sind Polykationen (Bi9)5+, welche die Gestalt zweifach überkappter trigonaler Prismen haben, in ein Chlorobismutat(III)-Raumnetzwerk [(Bi5Cl20)5-] eingebettet. Die Polykationen und das Anionennetzwerk sind deutlich voneinander separiert.

Die Dissertation beschreibt Untersuchungen der intermetallischen Verbindungen TbxY1-xNi2B2C bzw. TbxEr1-xNi2B2C, Tb2PdSi3 sowie Dy2PdSi3, die sich auszeichnen durch physikalische Erscheinungen, die durch die Wechselwirkung der magnetischen Momente der Seltenerd (SE)-Ionen mit den Leitungselektronen hervorgerufen werden. Sie umfasst Beiträge zur Konstitution der Legierungssysteme, methodische Untersuchungen zur Einkristallzüchtung, zur Charakterisierung der Homogenität und Perfektion der Kristalle und zu physikalischen Eigenschaften (Supraleitung, Magnetismus). Die für das Erstarrungs- und Schmelzverhalten der intermetallischen Phasen relevanten quasi-binären Schnitte der Tb-(Y, Er)-Ni-B-C bzw. Tb(Dy)-Pd-Si-Phasendiagramme, die bisher noch nicht bekannt waren, konnten bestimmt werden. Damit wurden die Prozessparameter der Einkristallzüchtung durch tiegelfreies Zonenschmelzen optimiert. Die unterschiedlichen Erstarrungstypen, peritektische Erstarrung (SENi2B2C) bzw. kongruentes Erstarren (SE2PdSi3), wurden durch unterschiedliche Ziehgeschwindigkeiten bei der Einkristallzüchtung berücksichtigt. An den massiven Einkristallen wurden Homogenitätsuntersuchungen hinsichtlich Elementkonzentration und physikalischer Eigenschaften (Tc, Tn, RRR) als Funktion der Längskoordinate durchgeführt, die geringe Eigenschaftsunterschiede der einkristallinen Proben nachweisen. Aus der Zusammensetzungsänderung über die Kristalllänge konnte in Verbindung mit in-situ Messungen der Zonentemperatur ein einfaches Prozessmodell des Zonenschmelzens der untersuchten Verbindungen entwickelt werden. Die Korrelation von magnetischen und supraleitenden Eigenschaften der Borokarbidmischreihen werden primär vom Verhältnis der Seltenen Erden bestimmt aber auch durch die Konzentration der weiteren Elemente. An Einkristallen konnte eine Anisotropie des oberen kritischen Feldes der Supraleitung von TbxY1-xNi2B2C gezeigt werden, die durch die magnetischen Tb-Ionen bestimmt wird. Die Untersuchungen der Tb2PdSi3- und Dy2PdSi3-Einkristalle ergaben eine Anisotropie der magnetoelektrischen Eigenschaften. / In this thesis investigations of the intermetallic compounds TbxY1-xNi2B2C, TbxEr1-xNi2B2C, Tb2PdSi3 and Dy2PdSi3 are presented. These compounds exhibit interesting physical phenomena caused by the interaction of the rare earth (RE) magnetic moments on the conduction electrons. Moreover, contributions on the constitution of the alloy systems, basic investigations of crystal growth process, homogeneity, microstructure and physical properties (superconductivity, magnetism) of the crystals are given. The quasi-binary sections of the Tb-(Y, Er)-Ni-B-C and Tb(Dy)-Pd-Si-phase diagrams which are relevant for the crystallisation of the different intermetallic phases have been determined for the first time. They were utilised for optimisation of the process parameters of single crystal growth by floating-zone melting. Because of the different solidification modes of RENi2B2C (peritectic solidification) and RE2PdSi3 (congruent solidification) different growth velocities have been employed in crystal growth. The composition and the physical properties (Tc, Tn, RRR) have been investigated as function of the crystal axis co-ordinate. As these properties show only a slight shift over the crystal length samples are representative for the whole crystal. From the slight composition shift over the crystal length a process model of the floating zone growth has been developed utilising the in-situ measurements of the zone-temperature. The correlation of magnetic and superconducting properties of the borocarbide solid solution compounds are mainly governed by the RE-fraction but they are also influenced by the concentration of the other elements. For TbxY1-xNi2B2C single crystals an anisotropic upper critical field of superconductivity has been detected which is induced by the magnetic Tb-ions. The investigations of Tb2PdSi3 and Dy2PdSi3 revealed an anisotropy of the magnetoresistive properties.