Violation of Kohler's rule by the magnetoresistance of a quasi-two-dimensional organic metal

The interlayer magnetoresistance of the quasi-two-dimensional metal alpha-(BEDT-TTF)(2)KHg(SCN)(4) is considered. In the temperature range from 0.5 to 10 K and for fields up to 10 T the magnetoresistance has a stronger temperature dependence than the zero-field resistance. Consequently Kohler's rule is not obeyed for any range of temperatures or fields. This means that the magnetoresistance cannot be described in terms of semiclassical transport on a single Fermi surface with a single scattering time. Possible explanations for the violations of Kohler's rule are considered, both within the framework of semiclassical transport theory and involving incoherent interlayer transport. The issues considered are similar to those raised by the magnetotransport of the cuprate superconductors. [S0163-1829(98)13219-8].

Incoherent interlayer transport and angular-dependent magnetoresistance oscillations in layered metals

The effect of incoherent interlayer transport on the interlayer resistance of a layered metal is considered. We find that for both quasi-one-dimensional and quasi-two-dimensional Fermi liquids the angular dependence of the magnetoresistance is essentially the same for coherent and incoherent transport. Consequently, the existence of a three-dimensional Fermi surface is not necessary to explain the oscillations in the magnetoresistance that are seen in many organic conductors as the field direction is varied. [S0031-9007(98)07660-1].

Comparison of coherent and weakly incoherent transport models for the interlayer magnetoresistance of layered Fermi liquids

The interlayer magnetoresistance of layered metals in a tilted magnetic field is calculated for two distinct models for the interlayer transport. The first model involves coherent interlayer transport, and makes use of results of semiclassical or Bloch-Boltzmann transport theory. The second model involves weakly incoherent interlayer transport where the electron is scattered many times within a layer before tunneling into the next layer. The results are relevant to the interpretation of experiments on angular-dependent magnetoresistance oscillations (AMRO) in quasi-one- and quasi-two-dimensional organic metals. We find that the dependence of the magnetoresistance on the direction of the magnetic field is identical for both models except when the field is almost parallel to the layers. An important implication of this result is that a three-dimensional Fermi surface is not necessary for the observation of the Yamaji and Danner oscillations seen in quasi-two- and quasi-one-dimensional metals, respectively. A universal expression is given for the dependence of the resistance at AMRO maxima and minima on the magnetic field and scattering time (and thus the temperature). We point out three distinctive features of coherent interlayer transport: (i) a beat frequency in the magnetic oscillations of quasi-two-dimensional systems, (ii) a peak in the angular-dependent magnetoresistance when the field is sufficiently large and parallel to the layers, and (iii) a crossover from a linear to a quadratic field dependence for the magnetoresistance when the field is parallel to the layers. Properties (i) and (ii) are compared with published experimental data for a range of quasi-two-dimensional organic metals. [S0163-1829(99)02236-5].

A nanometre-scale non-periodic structural variation in high temperature superconducting ceramics and the implications for properties

Non-periodic structural variation has been found in the high T-c cuprates, YBa2Cu3O7-x and Hg0.67Pb0.33Ba2Ca2Cu3O8+delta, by image analysis of high resolution transmission electron microscope (HRTEM) images. We use two methods for analysis of the HRTEM images. The first method is a means for measuring the bending of lattice fringes at twin planes. The second method is a low-pass filter technique which enhances information contained by diffuse-scattered electrons and reveals what appears to be an interference effect between domains of differing lattice parameter in the top and bottom of the thin foil. We believe that these methods of image analysis could be usefully applied to the many thousands of HRTEM images that have been collected by other workers in the high temperature superconductor field. This work provides direct structural evidence for phase separation in high T-c cuprates, and gives support to recent stripes models that have been proposed to explain various angle resolved photoelectron spectroscopy and nuclear magnetic resonance data. We believe that the structural variation is a response to an opening of an electronic solubility gap where holes are not uniformly distributed in the material but are confined to metallic stripes. Optimum doping may occur as a consequence of the diffuse boundaries between stripes which arise from spinodal decomposition. Theoretical ideas about the high T-c cuprates which treat the cuprates as homogeneous may need to be modified in order to take account of this type of structural variation.

Electric-field-induced Mott insulating states in organic field-effect transistors

We consider the possibility that the electrons injected into organic field-effect transistors are strongly correlated. A single layer of acenes can be modeled by a Hubbard Hamiltonian similar to that used for the κ-(BEDT-TTF)2X family of organic superconductors. The injected electrons do not necessarily undergo a transition to a Mott insulator state as they would in bulk crystals when the system is half-filled. We calculate the fillings needed for obtaining insulating states in the framework of the slave-boson theory and in the limit of large Hubbard repulsion U. We also suggest that these Mott states are unstable above some critical interlayer coupling or long-range Coulomb interaction.

Current density mapping approach for design of clinical magnetic resonance imaging magnets

Novel current density mapping (CDM) schemes are developed for the design of new actively shielded, clinical magnetic resonance imaging (MRI) magnets. This is an extended inverse method in which the entire potential solution space for the superconductors has been considered, rather than single current density layers. The solution provides an insight into the required superconducting coil pattern for a desired magnet configuration. This information is then used as an initial set of parameters for the magnet structure, and a previously developed hybrid numerical optimization technique is used to obtain the final geometry of the magnet. The CDM scheme is applied to the design of compact symmetric, asymmetric, and open architecture 1.0-1.5 T MRI magnet systems of novel geometry and utility. A new symmetric 1.0-T system that is just I m in length with a full 50-cm diameter of the active, or sensitive, volume (DSV) is detailed, as well as an asymmetric system in which a 50-cm DSV begins just 14 cm from the end of the coil structure. Finally a 1.0-T open magnet system with a full 50-cm DSV is presented. These new designs provide clinically useful homogeneous regions and have appropriately restricted stray fields but, in some of the designs, the DSV is much closer to the end of the magnet system than in conventional designs. These new designs have the potential to reduce patient claustrophobia and improve physician access to patients undergoing scans. (C) 2002 Wiley Periodicals, Inc.

Investigations of growth processes in Y-Ba-Cu-O materials by microstructural examination of quenched samples

Y-Ba-Cu-O samples with additions of Y2O3 and CeO2 were quenched during seeded isothermal melt processing and examined by optical microscopy and scanning electron microscopy. Large YBa2Cu3O7-y (Y123) particles in the starting powder were found to form a distinct type of melt during heating, which was unaffected by the Y2O3 or CeO2 additives. This type of melt later formed regions with a low concentration of Y2BaCuO5 (Y211) particles in the Y123 matrix. The maximum growth rate of Y123 that could be sustained in the sample was found to be lower in the melt formed from large Y123 particles, and this may lead to growth accidents and subgrains in some samples.

Simulation of the Magnetic Induction Vector of a Magnetic Core to be Used in FFC NMR Relaxometry

This paper is a contribution for the assessment and comparison of magnet properties based on magnetic field characteristics particularly concerning the magnetic induction uniformity in the air gaps. For this aim, a solver was developed and implemented to determine the magnetic field of a magnetic core to be used in Fast Field Cycling (FFC) Nuclear Magnetic Resonance (NMR) relaxometry. The electromagnetic field computation is based on a 2D finite-element method (FEM) using both the scalar and the vector potential formulation. Results for the magnetic field lines and the magnetic induction vector in the air gap are presented. The target magnetic induction is 0.2 T, which is a typical requirement of the FFC NMR technique, which can be achieved with a magnetic core based on permanent magnets or coils. In addition, this application requires high magnetic induction uniformity. To achieve this goal, a solution including superconducting pieces is analyzed. Results are compared with a different FEM program.

Simulation of the magnetic induction vector of a magnetic core to be used in FFC NMR relaxometry

This paper is a contribution for the assessment and comparison of magnet properties based on magnetic field characteristics particularly concerning the magnetic induction uniformity in the air gaps. For this aim, a solver was developed and implemented to determine the magnetic field of a magnetic core to be used in Fast Field Cycling (FFC) Nuclear Magnetic Resonance (NMR) relaxometry. The electromagnetic field computation is based on a 2D finite-element method (FEM) using both the scalar and the vector potential formulation. Results for the magnetic field lines and the magnetic induction vector in the air gap are presented. The target magnetic induction is 0.2 T, which is a typical requirement of the FFC NMR technique, which can be achieved with a magnetic core based on permanent magnets or coils. In addition, this application requires high magnetic induction uniformity. To achieve this goal, a solution including superconducting pieces is analyzed. Results are compared with a different FEM program.

Magnetic flux density distribution in the air gap of a ferromagnetic core with superconducting blocks: three-dimensional analysis and experimental NMR results

The design of magnetic cores can be carried out by taking into account the optimization of different parameters in accordance with the application requirements. Considering the specifications of the fast field cycling nuclear magnetic resonance (FFC-NMR) technique, the magnetic flux density distribution, at the sample insertion volume, is one of the core parameters that needs to be evaluated. Recently, it has been shown that the FFC-NMR magnets can be built on the basis of solenoid coils with ferromagnetic cores. Since this type of apparatus requires magnets with high magnetic flux density uniformity, a new type of magnet using a ferromagnetic core, copper coils, and superconducting blocks was designed with improved magnetic flux density distribution. In this paper, the designing aspects of the magnet are described and discussed with emphasis on the improvement of the magnetic flux density homogeneity (Delta B/B-0) in the air gap. The magnetic flux density distribution is analyzed based on 3-D simulations and NMR experimental results.

Manuel Cardona i Castro

Biografia del físic Manuel Cardona i Castro, autoritat mundial en l’estudi dels semiconductors i dels superconductors i gran promotor de la física a l’Amèrica Llatina.

Deposició de capes superconductores de YBa2Cu3O7 amb textura bidimensional a partir de solucions metal·lorgàniques

L’objectiu d’aquest projecte és l'obtenció de capes primes superconductores de YBa2Cu3O7 mitjançant el procés de descomposició metal·lorgànica, a partir de la combinació de sals precursores amb un contingut en fluor inferior a l’estàndard utilitzat pel grup de superconductivitat de l’ICMAB, així com l’estudi i caracterització d’aquestes capes mitjançant les tècniques utilitzades pel mateix grup. Per tal de poder analitzar els resultats, es realitzarà una comparació entre aquesta capa obtinguda a partir de la nova solució i una altra desenvolupada pel mètode estàndard. Sobre aquestes dues mostres es realitzaran tots els assaigs necessaris per tal d’obtenir les seves propietats físiques i químiques per tal d’analitzar la qualitat de la capa i avaluar la viabilitat de la nova solució.

Estudio de cerámicas nanoestructuradas mediante difracción de rayos X y microscopía electrónica de alta resolución

Este proyecto trata sobre la determinación de las relaciones epitaxiales que se dan entre una capa de NGO (Oxido de Neodimio-Galio) y una capa depositada de CGO (Óxido de Cerio dopado con Gadolinio). Con ello buscamos estudiar indirectamente como podemos producir las dislocaciones antes citadas mediante la tensión superficial que se crea al dar lugar un crecimiento heteroepitaxial auto-ensamblado de nanohilos sobre un substrato. Para utilizar en el futuro esta cerámica nanoestructurada como plantillas de superconductores. Abordaremos este objetivo mediante dos vertientes distintas. Por un lado, mediante el estudio de una muestra mediante difracción de rayos X en dos dimensiones (DRX2). Y paralelamente mediante su visualización usando Microscopía Electrónica de Transmisión (MET).

Mètodes de visualització i dinàmica de gasos relacionats amb l'escalat de cintes superconductores en planta prepilot

Ara ja fa un segle del descobriment de la superconductivitat. Aquest fenomen quàntic macroscòpic té aplicacions en el camp de la diagnosi mèdica per MRI (Magnetic Resonance Imaging), que permet obtenir imatges internes detallades del cos humà o en aplicacions científiques com el SQUID (Superconducting Quantum Interference Device), amb el que es poden mesurar camps magnètics molt dèbils, amb límits de detecció fins a 10-15 T. Però les aplicacions dels superconductors no es limiten ni molt menys a aquests camps ja que s‟estan fent grans esforços per poder processar cintes superconductores a gran escala per tal de poder aplicar aquest fenomen a cables de conducció elèctrica, motors, generadors, transformadors, etc. Amb això s‟aconseguiria un increment notable de l‟eficiència energètica amb la consegüent disminució de l‟emissió de gasos d‟efecte hivernacle. En aquest projecte, realitzat al grup de Superconductivitat i Nanoestructuració a Gran Escala de l„ICMAB, s‟han fet diversos muntatges experimentals per tal de poder observar i entendre millor el procés de piròlisi d‟una solució precursora de YBCO en forma de capes primes a sobre de diferents substrats. Aquesta etapa és determinant per obtenir en el procés de creixement una capa texturada i d‟ alta densitat de corrent crítica (Jc). Per això s‟ha fet ús d‟un sistema que permet realitzar la piròlisi de forma relativament ràpida mentre s‟enregistra en vídeo l‟evolució de la capa. En totes les mostres pirolitzades s‟ha estudiat la qualitat, textura i morfologia superficial. També s‟ha intentat veure de forma qualitativa el comportament dinàmic dels gasos a dins d‟una cavitat cilíndrica, que és la geometria utilitzada fins ara per créixer cintes superconductores. Finalment s‟han dissenyat diferents tipus de bufadors per tal d‟introduir els gasos de forma transversal i no longitudinal dins del forn tubular durant el tractament tèrmic, fet que dóna lloc a un increment de la superfície superconductora homogènia. El projecte es distribueix en diferents parts. Inicialment es fa una introducció als superconductors d‟alta temperatura així com els mètodes de fabricació actuals de les cintes superconductores. Seguidament s‟expliquen els objectius que pretenem assolir. En un apartat posterior descrivim les tècniques experimentals utilitzades. Seguidament detallem tots els resultats obtinguts junt amb les seves caracteritzacions. Finalment estudiem el impacte ambiental que ha tingut la realització d‟aquest projecte. Detallem el cost del mateix en un pressupost. En tres annexes ampliem alguns subapartats que per manca d‟espai en el text principal no hem pogut desenvolupar.

Síntesis de nanopartículas de ferritas tipo MFe2O4 (M=Fe, Co, Cu) para su aplicación en superconductores

La tecnología actual ha permitido que en los últimos años la nanociencia y la nanotecnología sean puntos críticos en el desarrollo del conocimiento. En estos momentos se desarrollan sistemas de dimensiones nanométricas que son interesantes debido a sus potenciales aplicaciones en diferentes ámbitos como en química, física, biología, materiales, medicina, cosmética... Dentro de estos sistemas nanoscópicos se encuentran las nanopartículas, estructuras con un tamaño inferior a los 100nm de longitud. En esta clasificación existen a su vez diferentes categorías, como las nanopartículas metálicas, semiconductoras, magnéticas, etc. y es exactamente en esta última tipoogía donde se centra este estudio. Este proyecto de investigación desarrolla la síntesis de magnetita (Fe3O4), ferrita de cobalto (CoFe2O4) y ferrita de cobre (CuFe2O4) con la finalidad de utilizarlas como dopante en superconductores. El método sintético utilizado es del tipo solvotérmico y se lleva a cabo en trietilenglicol, el cual actúa a la vez como disolvente y como estabilizante de las nanopartículas. Las partículas así obtenidas son dispersables en medios polares como el etanol absoluto. Los precursores de este método sintético son los respectivos acetilacetonatos metálicos debido a que el ligando orgánico descompone en productos volátiles. Existen diferentes factores que afectan a la síntesis, tales como la velocidad de ascenso de la temperatura, la agitación, la presencia de agua, la temperatura de descomposición de los precursores, etc. Algunos de estos factores han sido estudiados con detalle y aplicados con tal de optimizar el método experimental. Las nanopartículas sintetizadas han sido analizadas mediante diversas técnicas físicas con tal de establecer diferentes parámetros, tales como su composición fnal, su pureza, su estructura, sus propiedades magnéticas, etc. Estas técnicas son diversas: desde la espectroscopia infrarroja hasta medidas mediante SQUID, pasando por rayos X, microscopía electrónica y termogravimetría. Los resultados han sido favorables en la síntesis de la magnetita y también en la ferrita de cobalto, ya que las nanopartículas obtenidas son homogéneas, fácilmente dispersables en algoholes, estables por largos períodos de teimpo, rápidas de sintetizar, etc. El único problema observado ha sido la síntesis de ferrita de cobre la cual se ha de optimizar, ya que el producto final ha resultado ser una mezcla de tres compuesto diferentes.