Anomalous temperature behavior of the resistivity in lightly doped manganites around a metal-insulator phase transition; Ausloos, Marcel ; Bougrine, Hassan et alin JETP Letters (1999), 70(7), 481-487 An unusual temperature and concentration behavior of the resistivity ρ(T,x) in La0.7Ca0.3Mn1-xCuxO3 is observed at slight Cu doping (0 ≤x≤ 0.05). Namely, the introduction of copper results in a splitting ... [more ▼] An unusual temperature and concentration behavior of the resistivity ρ(T,x) in La0.7Ca0.3Mn1-xCuxO3 is observed at slight Cu doping (0 ≤x≤ 0.05). Namely, the introduction of copper results in a splitting of the resistivity maximum around the metal-insulator transition temperature T0(x) into two differently evolving peaks. Unlike the original Cufree maximum, which steadily increases with doping, the second (satellite) peak remains virtually unchanged for x<xc, increases for x≥xc, and finally disappears at xm ≃ 2xc, with xc ≃ 0.03. The observed phenomenon is thought to arise from a competition between substitution-induced strengthening of the potential barriers (which hinder the charge hopping between neighboring Mn sites) and weakening of the kinetic energy of the carriers. The data are well fitted by assuming a nonthermal tunneling conductivity theory with randomly distributed hopping sites. © 1999 American Institute of Physics. [less ▲] Detailed reference viewed: 3 (0 ULg) Anomalous temperature behavior of the resistivity in lightly doped manganites around a metal-insulator phase transition; Ausloos, Marcel ; Bougrine, Hassan et alin JETP Letters (1999), 70(7), 481-487 An unusual temperature and concentration behavior of the resistivity ρ(T,x) in La0.7Ca0.3Mn1-xCuxO3 is observed at slight Cu doping (0 ≤x≤ 0.05). Namely, the introduction of copper results in a splitting ... [more ▼] An unusual temperature and concentration behavior of the resistivity ρ(T,x) in La0.7Ca0.3Mn1-xCuxO3 is observed at slight Cu doping (0 ≤x≤ 0.05). Namely, the introduction of copper results in a splitting of the resistivity maximum around the metal-insulator transition temperature T0(x) into two differently evolving peaks. Unlike the original Cufree maximum, which steadily increases with doping, the second (satellite) peak remains virtually unchanged for x<xc, increases for x≥xc, and finally disappears at xm ≃ 2xc, with xc ≃ 0.03. The observed phenomenon is thought to arise from a competition between substitution-induced strengthening of the potential barriers (which hinder the charge hopping between neighboring Mn sites) and weakening of the kinetic energy of the carriers. The data are well fitted by assuming a nonthermal tunneling conductivity theory with randomly distributed hopping sites. © 1999 American Institute of Physics. [less ▲] Detailed reference viewed: 2 (0 ULg) A new fast and non-destructive method for evaluating the superconducting properties of bulk materialsVanderbemden, Philippe ; ; Cloots, Rudi et alin Obradors, X.; Sandiumenge, F.; Fontcuberta, J. (Eds.) Applied Superconductivity 1999. Volume 1 : Large Scale Applications (1999) This paper aims at reporting a new, simple and low-cost experimental technique designed for investigating the electrical properties of disk-shaped superconducting samples. The principle is similar to that ... [more ▼] This paper aims at reporting a new, simple and low-cost experimental technique designed for investigating the electrical properties of disk-shaped superconducting samples. The principle is similar to that of an induction motor. Two neighbouring and 90° out-of-phase AC magnetic fields are applied perpendicularly to the disk to be measured. As a result, the material experiences an electromagnetic torque which depends on its electrical properties. In this paper the experimental system is briefly described and illustrative measurements on different HTS are reported and discussed. [less ▲] Detailed reference viewed: 23 (2 ULg) Intragranular and intergranular superconducting properties of bulk melt-textured YBCOVanderbemden, Philippe ; Cloots, Rudi ; Ausloos, Marcel et alin IEEE Transactions on Applied Superconductivity (1999), 9(2), 2308-2311 We have investigated the superconducting properties of bulk melt-processed YBCO using different experimental techniques. First, single domain materials (i.e. containing no grain boundaries) have been ... [more ▼] We have investigated the superconducting properties of bulk melt-processed YBCO using different experimental techniques. First, single domain materials (i.e. containing no grain boundaries) have been studied. Electrical resistivity, current-voltage characteristics, M-H loops, and A,C. susceptibility. have been measured for different field and current directions. The intragranular properties are characteristic of high-quality melt-processed YBCO material,,vith a critical current density J(c)(T=77K, B=1T//c) > 10(4) A/cm(2). The anisotropy ratio J(c)(ab)/ J(c)(c) is found to be close to 3. Both magnetic and transport measurements show that defects in the microstructure do not significantly impede the current flow inside the single domain. These results were compared to those measured on samples containing one "natural" single grain boundary which sometimes appears during the grain growth process. The intergranular properties show a much stronger current and magnetic field dependence than that measured within the grain and these differences are discussed. [less ▲] Detailed reference viewed: 11 (2 ULg) A sharp decrease of resistivity in La0.7Ca0.3Mn0.96Cu0.04O3: Evidence for Cu-assisted coherent tunneling of spin polarons; Bougrine, Hassan ; Ausloos, Marcel et alin JETP Letters (1999), 69(11), 858-862 Nearly a 50% decrease of the resistivity rho(T,x) is observed upon just 4% Cu doping at the Mn site of La2/3Ca1/3Mn1-xCuxO3. When the observed phenomenon is attributed to a decrease of the spin-polaron ... [more ▼] Nearly a 50% decrease of the resistivity rho(T,x) is observed upon just 4% Cu doping at the Mn site of La2/3Ca1/3Mn1-xCuxO3. When the observed phenomenon is attributed to a decrease of the spin-polaron energy E-sigma(x) below T-C(x), all of the data are found to be well fitted by the nonthermal coherent tunneling expression rho(T,x)=rho(0)e(-gamma M2(T,x)), assuming that the magnetization in the ferromagnetic state is given by the expression M(T,x)=M-R(x)+M-0(x)tanh{T-[root(C)(x)/T](2)-1}. The best fits through all the data points suggest M-0(x)similar or equal to root 1-xM(0)(0), M-R(x)similar or equal to x root M-0(0), and E-sigma(x)similar or equal to E-sigma(0)(1-x)(4) for the explicit x dependence of the Cu-induced modifications of the Mn-spin-dominated zero-temperature spontaneous magnetization, residual paramagnetic contribution, and spin-polaron tunneling energy, respectively, with E-sigma(0)=0.12 eV. (C) 1999 American Institute of Physics. [S0021-3640(99)00811-7]. [less ▲] Detailed reference viewed: 18 (1 ULg) Effect of synthesis process and substrate on electrical and thermal transport properties of Bi-2212Dorbolo, Stéphane ; Ausloos, Marcel ; Bougrine, Hassan et alin Journal of Superconductivity (1999), 12(5), 623-629 Resistivity, thermoelectric power, and thermal conductivity have been measured for a Bi-2212 system synthesized from a glassy precursor, either with a commercially Al2O3 substrate or with a homemade ... [more ▼] Resistivity, thermoelectric power, and thermal conductivity have been measured for a Bi-2212 system synthesized from a glassy precursor, either with a commercially Al2O3 substrate or with a homemade BaZrO3 substrate. Those measurements show that the BaZrO3 substrate gives better superconducting properties to the Bi-2212 than the Al2O3 substrate. The effect of (1.0 T) weak magnetic field has been searched for. The thermal magnetoconductivity and the contributions of the magnetic field to the thermoelectrical power are studied and compared through fine measurements. An electronic contribution seems to appear already well above the critical temperature and to exist up to 200 degrees K. The onset temperature is thus deduced. [less ▲] Detailed reference viewed: 23 (2 ULg) Foam-like evolution in polycrystalline systems following successive 'melt and growth' cyclesVandewalle, Nicolas ; ; Ausloos, Marcel et alin Philosophical Magazine B-Physics of condensed matter statistical mechanics electronic optical and magnetic properties (1998), 78(4), 397-408 A stochastic model of multigrain growth which allows for successive melting-growth cycles is investigated on a square lattice. Two fundamental constraints are introduced: (i) the melted mass amplitude and ... [more ▼] A stochastic model of multigrain growth which allows for successive melting-growth cycles is investigated on a square lattice. Two fundamental constraints are introduced: (i) the melted mass amplitude and (ii) the number of cycles guide the process. The evolution of the microstructure is found to be quite similar to foam systems, i.e. topological rearrangements are observed together with the increase of the-mean grain area. A drastic crossover between two types of growth regimes is found as a function of the amplitude of the melting-growth cycles. This allows one to envisage the existence of optimal conditions for polycrystal processing. [less ▲] Detailed reference viewed: 8 (0 ULg) Branched Eden clusters in the dynamic epidemic modelVandewalle, Nicolas ; Ausloos, Marcel ; Cloots, Rudi ![]() in Physical Review. E : Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics (1998), 58(1), 1152-1154 The dynamic epidemic model [J. Phys. A 29, 309 (1996)] considers a simple Eden growth history in a medium containing a fraction x of mobile hindrances ("particles"). These particles an supposed to be ... [more ▼] The dynamic epidemic model [J. Phys. A 29, 309 (1996)] considers a simple Eden growth history in a medium containing a fraction x of mobile hindrances ("particles"). These particles an supposed to be pushed by the front of the growing cluster. We have investigated how the medium becomes organized after n successive Eden growth cycles. Applications to various fields are underlined. Unexpectedly, the mobile hindrances aggregate such that the Eden cluster becomes branched after a finite number of growth cycles. [less ▲] Detailed reference viewed: 10 (0 ULg) Effect of BaZrO3 additions on the microstructure and physical properties of melt-textured Y-123 superconducting materialsCloots, Rudi ; ; et alin Materials Science & Engineering : B (1998), 53(1-2), 154-158 The effect of BaZrO3 additions on the microstructure and physical properties of melt-textured Y-123 have been investigated. The distribution of the 211 particles is strongly modified by the presence of ... [more ▼] The effect of BaZrO3 additions on the microstructure and physical properties of melt-textured Y-123 have been investigated. The distribution of the 211 particles is strongly modified by the presence of such an additive. In fact, BaZrO3 is effective in reducing the size of the 211 particles. As a consequence, a strong interaction in terms of repulsion takes place between the 123 growth front and the 211 particles which are partially dissolved in the reactive liquid phase. New types of patterns are also reported in the microstructure of such materials and are related to the presence of BaZrO3 in the melt. [less ▲] Detailed reference viewed: 8 (1 ULg) The non-trivial dispersion of Y2BaCuO5 particles trapped in the YBa2Cu3O7-x crystal matrixVandewalle, Nicolas ; ; Cloots, Rudi et alin Philosophical Magazine Letters (1998), 77(5), 301-306 Micrographs of melt-textured YBa2Cu3O7-x/Y2BaCuO5 (123/211) have been digitized. Through image analysis, we point out that the dispersion of the 211 particles is highly inhomogeneous in the melt and in ... [more ▼] Micrographs of melt-textured YBa2Cu3O7-x/Y2BaCuO5 (123/211) have been digitized. Through image analysis, we point out that the dispersion of the 211 particles is highly inhomogeneous in the melt and in the 123 crystal matrix. Indeed, free 211 particle regions and 211 aggregates are observed. The distribution laws are given. Moreover, the dispersions of 211 particles in the melt and those trapped in the crystal matrix are quite different. We point out that this difference cannot be explained solely by the partial dissolution of the 211 particles during the growth process. [less ▲] Detailed reference viewed: 11 (0 ULg) The Nd-123 superconducting system: From single crystal to top-seeded large grain. Physical and chemical parameters influence; Vandewalle, Nicolas ; Ausloos, Marcel et alin Applied Superconductivity (1998), 6(2-5), 77-85 Nd-123 signle crystals have been produced via the Aux method in alumina crucibles by controlling the chemical composition of the flux. For so doing, quenched materials have been prepared and analyzed in ... [more ▼] Nd-123 signle crystals have been produced via the Aux method in alumina crucibles by controlling the chemical composition of the flux. For so doing, quenched materials have been prepared and analyzed in order to get information about the optimum barium: copper ratio for an unchanged neodymium concentration. Non corrosive fluxes with a low viscosity have been put into evidence and can thus be used for single crystal production. Experiments have been performed with three different chemical compositions of the Aux and by considering various amounts of neodymium oxide for each system. The single crystals have been analyzed by energy dispersive X-ray microanalysis and used for the synthesis of large Dy-123 single-domains? [less ▲] Detailed reference viewed: 38 (1 ULg) High field behavior of artificially engineered boundaries in melt-processed YBa2Cu3O7-delta; ; et al in Applied Physics Letters (1998), 73(1), 117-119 Artificial bulk "zero-angle" boundaries parallel to the c axis have been engineered between large melt-processed YBa2CU3O7-delta (YBCO) grains and observed to carry a transport supercurrent at fields up ... [more ▼] Artificial bulk "zero-angle" boundaries parallel to the c axis have been engineered between large melt-processed YBa2CU3O7-delta (YBCO) grains and observed to carry a transport supercurrent at fields up to at least 5 T at 77 K. The temperature and angular dependencies of the boundary resistance have exactly the same form as those of the grains, which is evidence that the grains are intimately coupled. The limiting mechanism for current transfer across these boundaries is, therefore, not a simple weak link or Josephson effect. This joining technique is extremely promising for production of macroscopic engineering artifacts. (C) 1998 American Institute of Physics. [less ▲] Detailed reference viewed: 79 (1 ULg) AC susceptibility data on Dy2O3 seeded randomly oriented Dy-123 mono domains melt-textured superconductorVanderbemden, Philippe ; Bougrine, Hassan ; Ausloos, Marcel et alin Materials Science & Engineering : B (1998), 53(1-2), 198-202 Dy-123 superconducting ceramics have been grows using small Dy2O3 single-crystals as seeds. Randomly oriented large mono-domains have been observed in the vicinity of the seeding single crystal. These ... [more ▼] Dy-123 superconducting ceramics have been grows using small Dy2O3 single-crystals as seeds. Randomly oriented large mono-domains have been observed in the vicinity of the seeding single crystal. These domains are one order of magnitude greater in volume than the seed. The AC susceptibility versus temperature curves have been measured in a polycrystalline cubic sample for different orientations of the magnetic field with respect to the sample and for amplitudes up to 20 G. Three measuring coils, each parallel to one side of the sample, were used to investigate the anisotropy of the properties. Electrical resistance versus temperature and flux profiles at 77 K were also explored. The results show good grain connectivity. A non negligible part of the magnetic shielding is due to currents flowing inside the grains. (C) 1998 Elsevier Science S.A. All rights reserved. [less ▲] Detailed reference viewed: 44 (3 ULg) Magnetic flux penetration and creep in BSSCO-2223 composite ceramicsVanderbemden, Philippe ; ; Cloots, Rudi et alin Superconductor Science and Technology (1998), 11(1), 94-100 We have experimentally investigated the magnetic flux penetration through a Bi-2223 polycrystalline superconductor synthesized by a classical solid-state reaction method. Electrical resistance, AC ... [more ▼] We have experimentally investigated the magnetic flux penetration through a Bi-2223 polycrystalline superconductor synthesized by a classical solid-state reaction method. Electrical resistance, AC susceptibility, the Campbell method and magnetic flux waveform recordings have been analysed and compared in order to separate clearly intergrain and intragrain contributions. The AC susceptibility frequency dependence has been also examined at T = 77 K in a broad field range (0.01 G < B-AC < 100 G) The activation energy as a function of AC applied magnetic field is found to present a pronounced minimum for an induction (8 G) corresponding to full magnetic flux penetration through the intergranular matrix. [less ▲] Detailed reference viewed: 26 (1 ULg) Distribution of vortex lattice melting temperatures in mixed state diagram of Bi2212 tapes; Bougrine, Hassan ; et alin Physica C (1998), 303(3-4), 169-176 The electrical resistivity in the mixed state of Bi2212 tape superconductors can be accurately reconstructed for values below approximately a half of the normal state value of resistivity, assuming a ... [more ▼] The electrical resistivity in the mixed state of Bi2212 tape superconductors can be accurately reconstructed for values below approximately a half of the normal state value of resistivity, assuming a Gaussian distribution for the vortex lattice melting temperatures. The magnetic field dependences of the distribution width and of the dB(c2)/dT parameter were calculated. Moreover the vortex liquid viscosity coefficient was determined between the vortex lattice melting temperature and T-c at various magnetic fields. It is pointed out that the vortex lattice melting transition should not be confused with the irreversibility line of magnetic studies nor with the percolation temperature line for electrical resistivity. (C) 1998 Elsevier Science B,V. All rights reserved. [less ▲] Detailed reference viewed: 17 (7 ULg) Transport properties of HgBaCaCuO(1223) polycrystalline superconductorsBougrine, Hassan ; ; Cloots, Rudi et alin Superconductor Science & Technology (1998), 11(1), 128-132 We report on the temperature (20-300 K) dependence of the resistivity, thermopower and thermal conductivity measurements of HgBaCaCuO(1223) polycrystalline superconductors with nominal composition Hg1 ... [more ▼] We report on the temperature (20-300 K) dependence of the resistivity, thermopower and thermal conductivity measurements of HgBaCaCuO(1223) polycrystalline superconductors with nominal composition Hg1.4Ba2Ca2CU3O8+delta. We present some discussion of the precision and the originality of the measurement methods which are especially used to measure the electrical resistivity and simultaneously the thermopower and the thermal conductivity as a function of temperature. The superconductivity fluctuation contributions to the transport properties of the materials are calculated and compared. The results are related to the 2D anisotropy of the crystallographic structure. [less ▲] Detailed reference viewed: 11 (0 ULg) The effect of BaZrO3 addition on transport properties of Dy-based 123-211 composite materials: electrical resistivity, thermal conductivity and thermoelectric powerBougrine, Hassan ; Ausloos, Marcel ; et alin Superconductor Science & Technology (1998), 11(8), 803-809 Composite samples made of 123-211 DyBaCuO-based systems with 1, 4, 10 and 15% in weight BaZrO3 additions have been synthesized. Their electrical resistivity, thermal conductivity and thermoelectric power ... [more ▼] Composite samples made of 123-211 DyBaCuO-based systems with 1, 4, 10 and 15% in weight BaZrO3 additions have been synthesized. Their electrical resistivity, thermal conductivity and thermoelectric power have been measured. The electrical resistivity has also been measured in a magnetic field less than 1 T. The data show that BaZrO3 addition has a non-trivial effect: beside mildly reducing the critical temperature of the superconductor, it increases the scattering at small concentration, and effectively reduces weak link features in the electrical property, but increases the thermal conductivity. The field influence on T-c is shown to be T-c(O)- T-c(B) approximate to B-1/2. [less ▲] Detailed reference viewed: 20 (0 ULg) Directional solidification by appropriate chemically active single crystal seed: An alternative way of generating large superconducting 123 single domainCloots, Rudi ; ; Rulmont, André et alin Journal of Materials Research (1997), 12(12), 3199-3202 A Dy2O3 single crystal has been used as a seed for the growth of isothermally melt-textured DY-123 material. The nucleation-controlled step has been observed to be related to the heterogeneous nucleation ... [more ▼] A Dy2O3 single crystal has been used as a seed for the growth of isothermally melt-textured DY-123 material. The nucleation-controlled step has been observed to be related to the heterogeneous nucleation of 211 particles at the surface of the dysprosium oxide single crystal. The subsequent growth mode seems to be controlled by a high concentration gradient of dysprosium in the liquid phase. This leads to a directional solidification process of the 123 phase. The size of the 211 particles seems to decrease as the distance from the dysprosium oxide single crystal increases. [less ▲] Detailed reference viewed: 26 (3 ULg) Formation of nick instabilities due to particle clustering along crystal interfacesVandewalle, Nicolas ; Ausloos, Marcel ; Cloots, Rudi ![]() in Physical Review. E : Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics (1997), 56(4), 4042-4047 The kinetic growth of crystal grains is simulated on a square lattice in the presence of mobile particles. The model is based on the Eden and the dynamic epidemic models. Trapping of the particles by the ... [more ▼] The kinetic growth of crystal grains is simulated on a square lattice in the presence of mobile particles. The model is based on the Eden and the dynamic epidemic models. Trapping of the particles by the advancing front and a short-range repulsion of the particles by the front are both allowed. The grain boundary morphology is studied through the kink density concept and the spatial distribution of particles is discussed. Indeed, the clustering of particles along the crystal edges is found to induce the formation of so-called nick instabilities at the liquid-solid interface. The particles, when trapped near such instabilities, occur as oblique filamentary structures in the crystal matrix, just like river networks. These findings agree with recent experimental observations. The numerical laws are also explained by theoretical arguments based on different characteristic lengths. [less ▲] Detailed reference viewed: 8 (0 ULg) Physicochemical causes for the microstructure of melt-textured YBa2Cu3O7-delta/Y2BaCuO5 compositesVandewalle, Nicolas ; Cloots, Rudi ; Ausloos, Marcel ![]() in Superconductor Science and Technology (1997), 10(3), 123-133 We report semiquantitative results for a physicochemical model intended to describe the multigrain growth of YBa2Cu3O7-deltaN2BaCuO5 (123/211) composites under isothermal undercooling. This model takes ... [more ▼] We report semiquantitative results for a physicochemical model intended to describe the multigrain growth of YBa2Cu3O7-deltaN2BaCuO5 (123/211) composites under isothermal undercooling. This model takes into account various ingredients supposed to be controlling the growth of such superconducting compounds, i.e. the presence of secondary phases. Moreover, a possible dynamical interaction between the growing 123 grains and the 211 solid particles is also included. The numerical investigations were performed for a model bivariate-like 211 particle distribution. The complete chemical dissolution of the small particles is allowed but the large ones are only partially dissolved in the first step which can be followed when chemically possible by a complete dissolution. The model is restricted to a two-dimensional square lattice. Various microstructural morphologies are obtained as a function of the initial composition of the melt and the initial size distributions of the 211 particles. Results are in quite good agreement with experimental observations. The quantity of 123 phase is predicted depending on the initial conditions. The optimal situation when a minimum fraction of liquid phase segregates at the gain boundaries is found to occur for 20 % excess of 211 phase in the initial melt. [less ▲] Detailed reference viewed: 3 (0 ULg) |
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