T. Porjesz
Eötvös Loránd University
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Featured researches published by T. Porjesz.
Journal of Crystal Growth | 1988
I. Halász; V. Fulop; I. Kirschner; T. Porjesz
Abstract Thermogravimetric (TG) measurements and differential thermoanalysis (DTA) were carried out connected with X-ray powder diffraction investigations of Ba 2 Cu 3 O 5+ d samples prepared at different temperatures. A low temperature tetragonal phase with higher oxygen content and a high temperature tetragonal phase could be distinguished with lattice constants a = 16.19 A and 12.96 A, and c = 12.38 A and 9.16 A, respectively. A possible mechanism for selective preparation of superconductors from high temperature phase has also been proposed assuming a structure with space group P4 2 /mcm.
Physics Letters A | 1988
I. Kirschner; I. Halász; Cs. Sükösd; T. Porjesz; J. Kürti; Gy. Kovács; L. Korecz; T. Kármán; N.S. Rozlosnik; G. Zsolt; T. Träger
Abstract A TlBaCaCuO 4.5+ x compound has been investigated from the point of view of superconductivity. Depending on the heat treatment, one part of the samples exhibits superconductivity with an onset of 121 K and a zero resistivity of 106 K, while the other part of them shows only a sharp drop in resistivity at 130 K which hints at the existence of superconducting domains. This picture was confirmed by magnetic and ESR measurements giving possibility for estimation of the critical magnetic fields.
Cryogenics | 1977
G. Reményi; I. Kirschner; T. Porjesz
Abstract A method was developed to calculate the magnetic field of superconducting magnets with a computer, type ODRA 1304. This programme calculates the magnetic field of every individual layer of the coil at any point in space, and sums them. By this process it is possible to build magnets with better homogeneity, than 10 −6 cm −1 . It guarantees two kinds of methods for realizing high homogeneity by overwinding the ends of the solenoid: both discreet coils of corrections and corrections of different continuous shape. The numerical results for the three experimentally examined magnets (cylindrical solenoid, Helmholtzs coil and corrected solenoid) are in close agreement with the theory.
European Physical Journal B | 1988
I. Kirschner; I. Halász; T. Träger; J. Tóth; Gy. Kovács; T. Porjesz; G. Zsolt; T. Kármán
Different heat treatment procedures were applied during sample preparation, which resulted in different superconducting properties in samples of the same nominal composition, TlCaBa2Cu3O7.5±d. This manifests itself in different critical temperatures: 104 K, 107 K and 93 K. The highestTc belongs to the best-crystallized samples in which the tetragonal Tl2Ca1Ba2Cu2O8±d phase is responsible for the superconductivity. The effect of heat treatments is reflected in the structural and magnetic properties as well.
Physica C-superconductivity and Its Applications | 1990
A.C. Bódi; J. Csikai; R. Pepelnik; I. Halász; I. Kirschner; Gy. Kovács; T. Porjesz; T. Träger
Abstract Irradiation effects of low-dose (10 14 n/cm 2 ) neutrons on the resistance and AC susceptibility of multiphase YBa 2 Cu 3 O 7 and Tl 2 Ca 1 Ba 2 Cu 2 O 8 have been studied. Experimental results show that dispersed local superconducting regions in the samples may be unified to form a continuous percolating network using neutron irradiation. If the concentration of oxygen vacancies and interstitials is below or above an optimum value, the irradiation increases or decreases, respectively, the superconductive volume fraction and - via Cu-O bond length - the T c value.
Journal of The Less Common Metals | 1989
Gy. Kovács; I. Kirschner; I. Halász; R. Laiho; T. Porjesz; K. Tompa; T. Träger; T. Kármán; G. Zsolt
Abstract Starting materials, compositions and heat treatments were varied to study the influence of preparation conditions on the structure and superconductivity of Tl-Ca-Ba-Cu-O compounds. Twenty-four different groups of samples were synthesized, and their phases, structures, superconducting parameters and inter-relations were investigated. Most of the samples are superconducting above 100 K. The critical temperatures occupy a rather wide interval of 61–121 K. A few specimens have no superconductivity down to liquid helium temperatures. The number, type, quantity and proportion of phases produced strongly depend on the chemical quality and mixture of the starting materials and on the heat treatment. We searched for all known phases which may be responsible for superconductivity. It has been observed that better superconductivity generally occurs for the more highly crystalline structures. In our experiments, the presence of non-reacted barium cuprates in the samples does not obstruct the establishment of superconductivity, but Tl2O3, CaO, BaO, CuO and other impurities disturb and limit the quality of superconductivity. The superconducting parameters are also affected by the oxygen stoichiometry. The resistivity-temperature curves of some samples indicate the presence of a two-phase system. A change with time of the microstructure of some samples was observed, and was reflected in macroscopic change of the superconducting parameters. This is supported by NMR investigations. Scanning tunneling microscopy indicates an oriented surface structure of the samples.
Physica C-superconductivity and Its Applications | 2000
István Vajda; T. Porjesz; Attila Györe; András Szalay; W. Gawalek
Abstract An experimental flywheel based on high temperature superconductors was constructed. The aim of the study is to investigate the possible use of this technology to improve electric power quality against voltage disturbances. Some preliminary results on the flywheel performance are reported.
Cryogenics | 1989
I. Kirschner; J. Matrai; G. Szentgyörgyi; T. Porjesz; M. Lamm; I. Molnár; Gy. Kovács; T. Träger; P. Lukács; T. Kármán; J. György; M. Takács; G. Zsolt
Abstract High T c superconducting magnets have been constructed and built of individual ceramic rings. For the elimination of problems of power dissipation on the resistance of electrical contacts, energy was supplied by a contactless magnetic induction method. The magnetic fields produced by two systems of rings were 16.1 and 20.7 mT. Other types of high T c magnets have been built based on superconducting ceramic spirals supplied by d.c. current, which produces a magnetic field of 0.15 and 3.2 mT.
Acta Physica Academiae Scientiarum Hungaricae | 1980
T. Porjesz; I. Kirschner; M. F. Kotkata; M. S. Zaghloul; Gy. Kovács; P. Debreceni
Investigation of galvanomagnetic effects was carried out in the temperature range of 1.5–350 K. The samples were made ofn- andp-type PhS, cut off in different orientations and rotated in the magnetic field.The reproductibility of the measurement and the stability of the temperature was better than 0.1%.The results show in the entire temperature range that the magnetoresistance contrary to accepted assumptions cannot be expressed in terms of only even powers of the magnetic field strength and a negative change appears as well.Calculating the electron effective mass more precisely considering the electron motion in thek-space the experimental results could be explained in a simple way in the whole temperature range.
Cryogenics | 1991
I. Kirschner; S. Leppävuori; R. Laiho; A.D. Caplin; I. Halász; T. Porjesz; A. Uusimāki; G. Zsolt; E. Lähderanta; T. Kármán; J.R. Laverty; Gy. Kovács
Abstract Using different batches of starting materials (samples I, TINO 3 , CaO, Ba 2 Cu 3 O 5 ; II, TINO 3 , CaO, BaO, CuO; III, TINO 3 , CaO, Ba(NO 3 ) 2 , CuO; IV, TINO 3 , CaO, BaCuO 2 ; V, TINO 3 , CaO, Ba(NO 3 ) 2 , CuO, O 2 ) and the same heat treatment process, high T c superconducting systems of nominal composition TICaBaCuO 4.5 were prepared. Different superconducting phases were formed depending on the starting compounds used. Specimens I and IV had a single-phase (2,1,2,2) character. In samples II and III the dominant (2,1,2,2) phase was accompanied by (2,0,2,1) and by (1,2,2,3) and (2,2,2,3) phases in small quantity, respectively, while specimens V can be characterized by the existence of CuO and Cu 2 O beside the chief (2,1,2,2) phase. The superconducting properties were affected by starting materials, which manifests itself in the difference in onset and critical temperatures, lower and upper critical magnetic fields, paramagnetic limits, coherence length, penetration depth and Ginzburg - Landau parameter of specimens of different kinds. Due to the weak coupling created by interstitial material, different intergrain, intragrain and direct transport critical currents were determined, depending on the type of samples. The main aim of this work was to compare the experimental data with the corresponding theories to draw conclusions on the role of the starting compounds.