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1.
Anisotropy and Hall effect measurements have been performed in calcium-doped, i.e., overdoped YBa2Cu3Oy ((Y1−xCax)Ba2Cu3Oy) thin films witha andc axis orientations. In highly overdoped films (x=0.4), the anisotropy of the normal resistivity decreases and a drastic change in Hall conductivity in the mixed state is observed. The change in Hall conductivity in the overdoped region is consistent with recent experimental results for La2−xSrxCuO4 films and seems to be common in highT c superconductors.  相似文献   

2.
The temperature dependences of the resistivity and of the Seebeck coefficient S is studied in three series of Y1−x CaxBa2Cu3−x CoxOy samples (x=0–0.3) differing in oxygen content. It was found that the critical temperature decreases for y≈7.0, and S(T=300 K) increases with doping, whereas oxygen deficiency results in a nonmonotonic variation of these quantities with increasing x. The band structure parameters have been determined from an analysis of the S(T) relations using a phenomenological theory of electron transport. It was found that an increase in x results in a gradual increase in band asymmetry, which is caused by calcium-induced creation of additional states in the band responsible for conduction in the normal phase. An analysis has shown that high impurity concentrations in oxygen-deficient Y1−x CaxBa2Cu3−x CoxOy samples bring about an additional ordering of the structure, which may be caused by formation of a cobalt superlattice. It has also been shown that, in the case of Ca and Co codoping, the dependence of critical temperature on effective conduction-band width coincides with the universal correlation relation observed in the YBa2Cu3Oy system with single substitutions in various lattice sites. Fiz. Tverd. Tela (St. Petersburg) 41, 1363–1371 (August 1999)  相似文献   

3.
The temperature dependences of the thermopower coefficient for two systems of doped yttrium high-temperature superconductors Y1 − x Pr x Ba2Cu3O y (x = 0.1−0.6) and Y1 − x Ca x Ba1.5La0.5Cu3O y (x = 0.05–0.30) have been analyzed using three models of electron transport, i.e., the Xin two-band model, the two-band model with an additional term linear in temperature, and the narrow-band model. For parameters of different models with a similar physical meaning, identical tendencies have been revealed in their variation with an increase in the dopant content. The mechanisms of influence of the dopants under investigation on the parameters of the band spectrum and the systems of charge carriers have been examined. It has been demonstrated that the revealed features of the dynamics of the Fermi level in the Y1 − x Ca x Ba1.5La0.5Cu3O y system are explained by the formation of an additional peak in the density of states upon doping with calcium, and the energy position of this peak is estimated.  相似文献   

4.
The thermopower in the YBa2−x LaxCu3Oy system (x=0–0.5) has been studied. An analysis made in terms of the narrow-band model revealed trends in the variation of the main band parameters with increasing lanthanum concentration. The dependence of the conduction band width on lanthanum concentration was found to pass through a weak minimum at x=0.05–0.1, which correlates in position with the maximum in the concentration dependences of the critical temperature and degree of sample orthorhombicity. The results obtained and their comparison with Fe, Co→Cu substitution data permit a conclusion that the main factor affecting the properties of the YBa2Cu3Oy system under nonisovalent substitution of various cations is the increasing disorder in the chain-oxygen subsystem caused by increasing impurity content. Fiz. Tverd. Tela (St. Petersburg) 40, 17–22 (January 1998)  相似文献   

5.
A new series of mixed oxide superconductors with the stoichiometric composition La2−x Dy x Ca y Ba2Cu4+y O z (x=0.0 − 0.5, y=2x) has been studied for structural and superconductiong properties. Our earlier studies on La2−x (Y/Er) x Ca y Ba2Cu4+y O z series, show a strong dependence of T c on hole concentration (p sh). In the present work, the results of the analysis of the neutron diffraction measurements at room temprerature on x=0.3 and 0.5 samples are reported. It is interesting to know that Ca substitutes for both La and Ba site with concomitant displacement of La onto Ba site. Superconductivity studies show that maximum T c is obtained for x=0.5, y=1.0 sample (T c ∼ 75 K), for La1.5Dy0.5Ca1Ba2Cu5O z (La-2125).  相似文献   

6.
The temperature dependence of the thermoelectric power in samples of Y1−x PrxBa2Cu3Oy (x=0−0.6) is investigated. The principal parameters of the system of charge carriers are determined on the basis of an analysis of this dependence within a narrow-conduction-band model, and their variation with increasing praseodymium content is analyzed. It is found that an increase in x leads to a very weak increase in the electron filling and considerable broadening of the conduction band accompanied by strong localization of the charge carriers. It is concluded on the basis of a comparative analysis of the results obtained and data for the YBa2Cu3Oy system in the case of aliovalent substitutions in the barium and copper sites that the valence of praseodymium in Y1−x PrxBa2Cu3Oy is very close to 3+. It is shown that there is a universal correlation between the effective width of the conduction band and the critical temperature following various cation substitutions in the Y-Ba-Cu-O system. It is concluded that the main reason for suppression of the superconducting properties of Y1−x PrxBa2Cu3Oy is the strong modification of the band spectrum caused by praseodymium. Fiz. Tverd. Tela (St. Petersburg) 39, 1520–1525 (September 1997)  相似文献   

7.
Incidence of doped holes in the CuO2 plane on the AF state was studied by Cu(1) nuclear quadrupole resonance (NQR) in slightly doped YBa2(Cu1 − z Li z )3O6 + x compounds. Inhomogeneous distribution of doped holes in the plane was detected in the low temperature measurements of transverse (1/T 2) and longitudinal (1/T 1) relaxation rates. We establish that at lower T the holes motion slows down and we estimate that the holes localize finally in restricted regions (∼3 lattice constants) in the Coulomb potential of the Li+ ions. Also we compared the hole behavior in slightly doped YBa2(Cu1 − z Li z )3O6 + x samples with that in slightly doped Y1 − y Ca y Ba2Cu3O6. A stronger trapping potential of the in-plane Li+ impurities was concluded as compared to slightly doped Y1 − y Ca y Ba2Cu3O6 compound with out-of-plane Ca2+ impurities.  相似文献   

8.
Superconductivity is found in tetragonal La3−x Ba3+x Cu6O14+δ and La, Ba)6−x Sr x Cu6O14+δ even though they do not possess Cu-O chains or the K2NiF4 structure. Resistivity measurements confirm the occurrence of a transformation from chain-superconductivity to sheet-superconductivity in YBa2Cu3O7−δ as δ is varied in the range 0.0–0.5. Contribution No. 481 from the Solid State and Structural Chemistry Unit  相似文献   

9.
The results of the experimental study of the specific features of changes in the temperature and concentration dependences of the thermopower coefficient and the critical temperature in the Y0.85 − x Ca0.15Pr x Ba2Cu3O y system as the praseodymium content increases are presented. The results obtained have been analyzed based on the narrow band model, the energy spectrum and charge carrier system parameters have been determined, and their behavior with an increase in the doping level has been analyzed. It has been found that both superconducting properties and parameters of the normal state of Y0.85 − x Ca0.15Pr x Ba2Cu3O y vary differently in various doping ranges. Based on a comparison of the results obtained with the available data for the case of single doping of YBa2Cu3O y with praseodymium, conclusions have been drawn regarding the mechanism of the energy spectrum modification in the studied compound. The Fermi-level pinning effect has been revealed in the region of a local peak of the density-of-states function, and the energy position of this peak has been determined. It has been shown that the consideration of the Fermi level dynamics caused by the specific features of the structure and transformation of the Y0.85 − x Ca0.15Pr x Ba2Cu3O y energy spectrum upon doping makes it possible to explain the observed dependence of the critical temperature on the praseodymium content.  相似文献   

10.
The modification of the temperature dependences of the thermopower coefficient for the Tl2Ba2Ca1 − x Y x Cu2 − y Co y O z system is investigated as a function of the dopant content. The model of an asymmetric narrow band is shown to be applicable to high-temperature superconductors in the thallium system. The parameters of the band spectrum and charge carrier system for samples of a close-to-optimum composition are determined by analyzing the temperature dependences of the thermopower coefficient within the narrow band model. The character and mechanism of their variation in the course of the transition to an underdoped regime are analyzed together with the dynamics of changes in the superconducting properties. The critical temperature T c is found to correlate with the effective conduction-band width W D . It was shown that the dependence T c (W D ) for Tl2Ba2Ca1 − x Y x Cu2 − y Co y O z has a close-to-universal character, but the suppression of T c upon the broadening of the band occurs faster than in the case of the yttrium system. Original Russian Text ? O.A. Martynova, V.é. Gasumyants, 2007, published in Fizika Tverdogo Tela, 2007, Vol. 49, No. 9, pp. 1537–1542.  相似文献   

11.
Samples of YBa2(Cu0.85Sn0.15)3O7–y (1-2-3), La2(Cu0.95Sn0.05)O44–x, and La1.85Ba0.15(Cu0.95Sn0.05)O4–x (2-1-4), with different oxygen stoichiometry, have been studied by Mössbauer spectroscopy. These measurements reveal the existence of two inequivalent sites for Sn in the (1-2-3) compounds. The (1-2-3) spectra display two quadrupole doublets which we associate with Sn in Cu(1) and Cu(2) sites, respectively. La compounds show a single quadrupole doublet.  相似文献   

12.
Measurements of the temperature dependences of the resistivity and Seebeck coefficient S, as well as of the Hall coefficient R H at T=300 K are reported for two series of ceramic Y1−x CaxBa2Cu3Oy samples with oxygen contents in the initial sample close to stoichiometric and then lowered by annealing. It has been found that an increase in calcium content in the first series results in a drop of the critical temperature T c , a weak variation of S (300 K), and an increase of R H (300 K), whereas in the second series T c increases, S (300 K) decreases, and R H (300 K) remains practically constant. The S (T) relations acquire additional features with increasing doping level, which are not typical of the YBa2Cu3Oy system for other types of substitution. An analysis of the data obtained made in terms of the phenomenological band model permits a conclusion that calcium is capable of introducing additional states in the conduction band. Based on this assumption, we have succeeded in providing a qualitative explanation for the unusual features in the behavior of the transport coefficients and critical temperature in Y1−x CaxBa2Cu3Oy. Fiz. Tverd. Tela (St. Petersburg) 40, 2145–2152 (December 1998)  相似文献   

13.
We update our muon spin relaxation studies of the magnetic field penetration depth which show the correlations betweenT c and the relaxation rate σ αn s/m * (carrier density/effective mass) of hole-doped high-T c cuprate superconductors (La2, Sr3)CuO4, YBa2Cu3O7 (Y1−xPrx)Ba2Cu3O7, and other double and triple layer systems. These studies are extended to the organic superconductor (BEDT-TTF)2Cu(NCS)2.  相似文献   

14.
The temperature dependence of the Nernst-Ettingshausen coefficient Q(T) in the normal phase of doped HTSCs of the yttrium system was studied. The main features characterizing the behavior of this coefficient were revealed, and the character and mechanism of the effect that various nonisovalent substituents exert on the Q(T) dependence were analyzed. It is shown that the narrow-band model permits one not only to describe all the specific features observed in the Q(T) curves but also to perform a simultaneous quantitative analysis of the temperature dependences of four kinetic coefficients (the electrical resistivity and the Seebeck, Hall, and Nernst-Ettingshausen coefficients) with the use of a common set of model parameters characterizing the band structure and carrier system in the normal phase of an HTSC. This approach was employed to determine the carrier mobilities and the asymmetry of the dispersion curve in the systems studied (YBa2Cu3Oy, y = 6.37–6.91; YBa2Cu3?xCoxOy, x = 0–0.3; Y1?xCaxBa2Cu3Oy, x = 0–0.25; Y1?xCaxBa2?xLaxCu3Oy, x = 0–0.5) and to analyze the effect of the substitutions involved on the variation of these parameters.  相似文献   

15.
New results on the Mossbauer spectroscopy of the YBa2(Cu1−xFex)3Oy system are reported and the availible reliable experimental data are briefly summarized.  相似文献   

16.
The temperature dependences of the thermopower, S(T) of Y1−xPrxBa2Cu3Oy (0≤x≤0.6) have been measured and analyzed within a phenomenological model of electron transport in the case of a narrow conductive band. The band spectrum parameters have been estimated by a quantitative comparison of the experimental and calculated S(T) curves. It was revealed that an increase of the Pr content results in remarkable broadening of the conductive band and a strong localization of the states. This can be considered as the main reason for Tc depression. The effect of Pr on the band filling is very slight that makes it possible to conclude a valence of Pr to be close to 3+. The Pr influence on superconducting properties of YBa2Cu3Oy cannot be described in the terms of hole-filling effect.  相似文献   

17.
The lattice parameters of a Nd 1111 Fe-pnictide superconductor, NdFeAsO0.89F0.11, were accurately measured using X-ray diffraction between 20 K and 280 K. A very small change in the lattice parameter could be detected in the superconducting phase. This change can be attributed to a spontaneous strain generated in the superconducting phase by the coupling between a superconducting order parameter and the strain. The present results are compared with the thermal expansion coefficients of Ba (Fe1−x Co x )2As2, in addition to the previous lattice parameter measurements of YBa2Cu3O6.5, MgB2, La1.85Sr0.15CuO4, and Ba0.6K0.4BiO3.  相似文献   

18.
Transverse and zero-field μSR measurements were made on YBa2(Cu1−xNix)3O7−y withx=0.1 and 0.2, and YBa2(Cu1−x Zn x )3O7−y withx=0.03, 0.06, 0.1, and 0.16, wherey≈0.1. Since doping may lead to magnetic ordering this was searched for with both zero and transverse field μSR, but no evidence was found over the temperature range studied: 10–100 K. However, depolarization rates as functions of temperature were obtained, and the low temperature values of these are σ=3.2 μs−1.1.6μs−1, and 1 μs−1 forx=0.01, and 0.2 Ni, respectively, and σ=0.8 μs−1, 0.75 μs−1, 0.65 μs−1, and 0.4 μs−1 forx=0.03, 0.06, 0.1, and 0.16 Zn, respectively. Estimates for the effect of decreasing electron concentration for Zn are made, but these alone do not account for the drop in σ. Estimates for the effect of scattering on λ and hence σ are made. The reduction in σ for Ni dopant is in surprisingly good agreement with these estimates. For Zn the order of magnitude is correct, but the relative lack of further change in σ after the effect of the first 0.03 addition seems to imply a saturation of the effect of scattering.  相似文献   

19.
Epitaxial La1−x Pb x MnO3 (LPMO) thin films, grown on (100) SrTiO3 substrates by laser ablation technique at different temperatures between 600 and 850°C, have been characterized for electrical and magnetic properties. The temperature dependence of resistivity showed that the metal-insulator transition temperature (T MI) decreases with increasing substrate temperature, which has been attributed to decrease in Pb content in the filsm. The YBa2Cu3O x /La1−x MnO3 heterostructures, exhibiting both superconductivity and ferromagnetism, have been fabricated.  相似文献   

20.
The negative muon spin rotation method (μ SR) has been applied to studies of electronic states at oxygen sites of oxide superconductors YBa2Cu3O7, Nd2−x Ce x CuO4−δ (x=0.15, oxygen reduced), LiTi2O4 and related oxide-insulators La2CuO4−δ, CuO, Cu2O. The paramagnetic shifts of μ trapped at oxygen nuclei in these polycrystalline powder samples have been measured at 300 K. All the measured shifts are positive. In copper-oxides the paramagnetic shifts are of the order 10−3, while in LiTi2O4 is very small (8.4±3.34×10−5). In YBa2Cu3O7, a fast μ spin relaxation timeT 2 * (∼ 200 ns) has been observed; the reason for this is unknown and further studies are now in progress.  相似文献   

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