14 research outputs found
Study of effect of Sn doping of EuBa2Cu3-xO7-δ compound on superconducting properties by contactless methods
Effect of Sn addition on structural and superconducting properties in EuBa2Cu3O7-δ (Eu-123) compound was studied using XRD and SQUID magnetometric measurements. Transition process from normal to superconducting state was analyzed by the measurement of temperature change of the magnetic moment of the combined ZFC and the remanence technique beside the usual ZFC and FC ones. Samples of the nominal composition EuBa2Cu3-xSnxO7-δ with x ranging from 0.0 to 0.2 were prepared by the solid state reaction technique from Eu2O3, BaCO3, CuO and SnO2 precursors. The increasing Sn-content deteriorates the superconducting properties of the Sn doped samples
Experimental Liver Iron Measurement with the SQUID Gradiometer System
An experimental system for noninvasive measurement of the iron stores in the liver of living human organism has been designed and realized. This system enables to test the presence and to determine the iron concentration in this organ. The principle of operation is based on measurement of small response (magnetic moment) of the paramagnetic protein ferritin to the applied magnetic field on the complex diamagnetic background of other body organs. The experiment was performed by modified SQUID system with the 2nd order gradiometer. At present, the sensitivity of the system is 1 mg Fe per gram of the wet liver, which from the point of view of clinical diagnostics, enables to indicate the state of the liver iron overload, e.g., in hemochromatosis and hemosiderosis
Identification of single-domain structures in the system YBa 2 Cu 3 O 7-δ -Ag by magnetization measurements
Abstract The magnetization methods were used in study of effect of Ag doping on the structural and superconducting parameters in two series of melted and highly textured samples of the system (YBa 2 Cu 3 O 7−δ ) 1-x (Ag 2 O) x . The x concentration level of the first series ranged from 0 to 10 wt % and the second one from 0 to 3.6 wt % Ag 2 O. By means of the SQUID magnetization measurements the optimum Ag 2 O doping level ranged from 1.6 to 2.8 wt %. These methods led to optimization of conditions in preparation of single-domain samples. From the secondary precipitated CuO phase and from the appearance of Ag component the solubility limit of Ag in solid solution YBa 2 Cu 3−y Ag y O 7−y/2−δ was found
Magnetometric Measurements of Low Concentration of Coated Nanoparticles
A modified RF SQUID system with the order gradiometer has been tested for the purposes of detecting the magnetic nanoparticles as potential carriers of biological medicament. The paper presents basic information about the sensitivity of the system and its use for quantification of low concentration of coated magnetic nanoparticles. Model measurements provided information that enabled us to define the parameter influencing the experimental results. The volume of the biological object and its distance from the antenna appear to have the significant influence on the measurement accuracy
Effects of Gd/Ba Nonstoichiometry in on Superconducting and Magnetic Properties
Effects of slight nonstoichiometry in compounds on superconducting and magnetic properties were studied. The series of single-phase samples of with composition deviation x from the stoichiometric value of 0 to 0.1 and to -0.1 were synthesized by the solid-state reaction method from , and CuO precursors, sintered at the temperature of ~ 1000°C in flowing oxygen and annealed at 450°C for 24 h
Magnetic Properties of YBaCuO Melt Textured Samples Prepared by Powder Melting Process and Quench and Melt Growth Techniques
The microstructure and magnetic properties of the melt textured YBaCuO samples prepared by the powder melting process, in which YCuO and BaCuO were used as precursors, and those prepared by the quench and melt growth method are described and compared. The lattice parameters and T values for the samples prepared by the both techniques were similar. The penetration and the spatial distribution of the magnetic flux in the superconducting samples was imaged by means of a field-mapping device using a Hall probe. In the range of low magnetic fields up to 820Am no significant differences in penetration of magnetic flux between the samples prepared by the powder melting process and the quench and melt growth were observed. The mapping could not resolve any grain boundaries, single grains and structural defects. By the ac and virgin volume magnetisation characteristics, which were measured in the zero-field cooled condition by a 2nd order SQUID gradiometer, no weak links were identified. Better magnetic properties of the quench and melt growth samples in high magnetic fields can be explained by the differences in microstructure and/or by the risen content of the finely dispersed 211 and Pt containing phases. The increase factor in magnetisation is about 2.5. Some aspects of the Bean model for textured YBaCuO samples are discussed
Magnetic Properties of Nanooxide Prepared Mechanochemically With and Without Salt Matrix
We present a new technological route of synthesis of nanocrystals based on mechanochemical reduction of with as a reductant, followed by low temperature vacuum annealing. The structural and magnetic properties of the nanocrystals were studied
Magnetic Properties of Synthetic Gehlenite Glass Microspheres
In the paper, gehlenite amorphous microspheres were prepared by the flame synthesis of a powder precursor. In the first step, the precursor was prepared from a stoichiometric mixture of CaCO₃, Al₂O₃ and SiO₂ by a standard solid-state reaction method. Next, the precursor was sprayed into a CH₄-O₂ flame with the temperature of around 2200°C and molten droplets of synthetic gehlenite were rapidly cooled by distilled water. Structural and detailed magnetic properties were studied by the optical microscopy, X-ray diffraction and QD SQUID magnetometer. The gehlenite microspheres show a complex magnetic behaviour that is a function of the temperature and the magnetic field, e.g. diamagnetism and paramagnetism at 300 K and 2 K, respectively