Electrical Transport and Lowered Percolation Threshold in YBa2Cu3O7−δ-Nano-YBa2ZrO5.5 Composites

Rejith, Pullanhiyodan Puthiyaveedu; Vidya, Sukumariamma; Thomas, Jijimon Kumpukattu

doi:https://doi.org/10.1155/2014/768714

International Journal of Superconductivity

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Research Article | Open Access

Volume 2014 | Article ID 768714 | https://doi.org/10.1155/2014/768714

Electrical Transport and Lowered Percolation Threshold in YBa₂Cu₃O_7−δ-Nano-YBa₂ZrO_5.5 Composites

Pullanhiyodan Puthiyaveedu Rejith,¹Sukumariamma Vidya,¹and Jijimon Kumpukattu Thomas¹

Academic Editor: Dong Qian

Received10 May 2014

Accepted06 Aug 2014

Published25 Aug 2014

Abstract

We investigated the chemical reactivity and percolation characteristics of insulating nanocrystalline YBa₂ZrO_5.5 prepared by modified combustion route and the YBa₂Cu₃O_7−δ superconductor composite system. Structural analysis was done by using X-ray diffraction technique, surface morphology of the samples was studied using scanning electron microscopy, and electrical transport measurements like critical transition temperatures () and self-field transport critical current () were done by using standard four-probe technique. It is found that, in YBa₂Cu₃O_7−δ-nano-YBa₂ZrO_5.5 composite system, the superconductor and insulator materials coexist as separate phases without any noticeable chemical reaction even after sintering at high temperatures. Furthermore, percolation threshold and critical exponent are found to be , and . And the analysis of the current flow in the polycrystalline samples reveals weak link behavior in the majority of grain connections.

1. Introduction

High temperature superconductors with transition temperatures above 77 K in ceramic materials have received tremendous responsiveness because of their scientific and practical potential. The study of superconducting small aggregates, clusters, or particles is very important from both the fundamental and the technological standpoint [1–3]. It will be significant to study the percolation and superconductivity of composites involving superconductor inserted in an insulator medium. Granular nature along with short coherence length [4] and large penetration depth [5] of high temperature superconductors allows us to investigate the percolation behavior, fractal properties, quantum size effects, thermal fluctuations, and size effects on superconductivity. The percolation concept was first employed to describe superconductors by Davidson and Tinkham [6], who analysed resistivity data of composite Nb₃Sn/Cu wires. For the growth of high quality films, the choice of substrate is vital. A high superconductor-insulator system is very difficult to obtain without compromising the superconducting properties. The chemical nonreactivity of the substrate materials with superconductors indicates their potential as substrates for film deposition. The chemical compatibility of materials with the superconductor at the processing temperature is crucial. Also superconductor-insulator percolation studies are a medium to understand the fundamental mechanism behind high temperature superconductivity.

A percolation model can be regarded as a collection of points or occupied sites distributed in a space; certain pairs of them are randomly linked [7]. Its applications range from transport in amorphous and porous media and composites to the properties of branched polymers, gels, complex ionic conductors, and superconductors [8]. There is a path between two points and , if a sequence beginning with and ending with can be found, such that successive points in this sequence are linked. This path may allow the flow of charge between two points if we regard the occupied sites as pieces of conductor. The sites may be clustered such that pairs of points belonging to the same cluster are connected but there is no path between points belonging to different clusters. Cluster size (number of points in the cluster) increases with the number of linkages. Some cluster may become of infinite size at some critical density of occupied sites. Above this critical density, known as percolation threshold , the infinite cluster spans entire system and the system is in percolating state. For instance, in an ideal mixture of conducting and insulator particles the conductivity is zero outside the percolating region, whereas it takes a finite value inside this region.

It was reported that perovskites could be beneficial for incorporation into YBCO due to their similar crystal structures relative to the host YBCO phase [9]. Thereafter perovskite based additions have gained renewed interest as a class of materials that can be incorporated into REBCO superconductor for dramatic improvements in the pinning properties [10–13]. And a number of perovskites like Sr₂HoHfO_5.5 [14], GdBa₂NbO₆ [15], Ba₂ErZrO_5.5 [16], YBa₂ZrO_5.5 [17], and so forth were being considered as substrate materials for YBCO film deposition. However substrate selection presents particular challenges for the production of high-quality high-temperature superconducting (HTS) films suitable for applications [18]. In order to confirm their chemical compatibility with YBCO, it is important to study the electrical transport and percolation behavior in these superconductor-insulator composites. Transport properties and percolation behavior of high superconductor-metal composites have been reported extensively [19–24]. The general form of the double perovskites is , where for the present work , , and . Paulose et al. studied percolation properties of Ba₂YZrO₆ prepared by conventional solid state route and YBa₂Cu₃O_7−δ superconductor composite using temperature-resistivity measurement and reported that both superconducting and normal state percolation threshold values of the composite are around 35 vol.% of YBa₂Cu₃O₇ in the system [25]. In the present work, the percolation behavior and nonreactivity of nanoparticles of YBa₂ZrO_5.5 (YBZO) ceramic prepared through an autoigniting combustion technique mixed with bulk YBa₂Cu₃O_7−δ (YBCO) superconductors are studied. The variations in the microstructure, sintering behavior, sample density, electrical transport such as , and current carrying capacity are also studied.

2. Materials and Methods

Conventional technique of solid state route was used for the preparation of YBCO superconductor, by which high purity Y₂O₃, BaCO₃, and CuO were thoroughly mixed in the stoichiometric ratio of Y : Ba : Cu = 1 : 2 : 3. The mixture was then calcined at 930°C for 72 hours with two intermediate wet grindings. High quality nanoparticles of YBa₂ZrO_5.5 (YBZO) were synthesized through modified autoigniting combustion technique as reported by Jose et al. [26]. In a typical synthesis, aqueous solution containing ions of Y, Ba, and Zr was prepared by dissolving high purity Y₂O₃ in dilute HNO₃, Ba (NO₃)₂, and ZrOCl₂ (99%) in double distilled water in a glass beaker. Citric acid (99%) was then added to the solution containing Zr ions which serves as the complexing agent. Oxidant/fuel ratio of the system was adjusted by adding nitric acid and ammonium hydroxide and the ratio was kept at unity. The solution containing the precursor mixture at a pH of ~7.0 was heated using a hot plate at ~250°C in a ventilated fume hood. The combustion product was subsequently characterized as single phase nanocrystals of YBa₂ZrO_5.5. The YBCO and nano-YBZO were thoroughly mixed in different ratios and made into rectangular pellets of dimension 12 × 4 × 1 mm. These pellets were sintered at temperature ranges from 975°C to 1500°C for 12 hours with a heating rate of 3°C/minute depending on the volume percentage of YBHO in the composite material. The samples were then cooled to 550°C and kept 24 hours for oxygenation and then cooled to room temperature.

The structural characterization of YBCO-nanocrystalline YBZO composites was done by powder X-ray diffraction (XRD) technique using a Bruker D-8 X-ray diffractometer with Nickel filtered Cu radiation. The surface morphology of the sintered samples was studied using scanning electron microscopy (SEM) (JEOL JSM 6390 LV). The qualitative and quantitative elemental composition of the materials in the compounds was studied using energy dispersive X-ray spectroscopy (EDS) JEOL model JED-2300. The critical transition temperatures () of the samples were measured using standard four-probe technique. For the samples with higher vol.% of insulator, a two-probe method was used to measure their resistivity. For this experiment the entire data collection was run using a Lab VIEW 7.1 program on a PC. This was connected to Keithley source meter 2440 and nanovoltmeter 2182A along with lakeshore temperature controller equipped with PT-111 platinum sensor using a GPIB connection. The electrical contacts on the surface of the pellets were done by adhesive silver paste after making a narrow scratch on the sample surface. The self-field transport critical current () measurements were done at liquid nitrogen temperature using the standard 1 μV/cm criterion.

3. Results and Discussion

The powder morphology of the as-prepared YBa₂ZrO_5.5 nanopowder was done by using transmission electron microscopy (TEM) and is shown in Figure 1. The result suggested that the self-aligned nanoparticles of YBZO are of cuboidal shape with sharp grain boundaries and with size less than 20 nm. The selected area electron diffraction (SAED) pattern, shown inset to Figure 1, reveals that the YBa₂ZrO_5.5 nanoparticles were crystallized, with bright polycrystalline diffraction rings. SAED patterns were composed of a number of bright spots arranged in concentric rings. The electrons were reflected and diffracted from crystallographic planes of the unit cells of the sample to produce bright spots. The rings were diffuse and hollow, showing that the products were composed of nanocrystals with different orientations. This is indicative of the polycrystalline nature of the crystallites, but the spotty nature of the SAED pattern could be due to the fact that finer crystallites with related orientations were agglomerated together, resulting in a limited set of orientations.

The X-ray diffraction (XRD) patterns of composites for 0–100 vol.% of nano-YBZO in the YBCO system are shown in Figure 2. XRD patterns of composites show that all the peaks could be indexed for orthorhombic YBa₂Cu₃O_7−δ and cubic YBa₂ZrO_5.5 and there is no extra peak detectable. This implies that YBa₂ZrO_5.5 and YBa₂Cu₃O_7−δ remain as two different separate phases in the composite even after severe heat treatment up to 1020°C. For YBCO-YBZO composites with 80 vol.% YBZO, the sintering temperature was above the peritectic temperature of YBCO (~1030°C) and therefore the formation of a 211 phase with YBCO is expected, but in the present study the XRD patterns did not show the presence of a 211 phase in the system. Thus, the composites synthesized are suitable for the percolation studies.

The surface morphology of the composite samples was illustrated by scanning electron microscopy (SEM). Figure 3 shows the SEM images of different vol.% of nano-YBZO added YBCO composites. These indicate that the surface of the samples presents a crystalline character, which is typical of a polycrystalline ceramic material. The YBa₂Cu₃O_7−δ grains form groups which have appearance of clusters and there is no detectable interface interaction between the YBZO and YBCO grains. However, there are different grain sizes and a random orientation of grain boundaries, whereby the presence of different intergrain conductivities is expected.

(a)

(b)

(c)

(d)

(e)

(f)

The effect of YBa₂ZrO_5.5 on the superconducting transition temperature of YBa₂Cu₃O_7−δ was studied by four probe measurements for temperatures ranging from 77 to 300 K. Variation of normalized resistivity with temperature of the YBCO superconductor mixed with different vol.% of insulating nano-YBZO samples is shown in Figure 4. It is observed that the composite sample with less than 50 vol.% of YBCO showed a metallic behavior and gave zero resistivity superconducting transition temperature above liquid nitrogen temperature. However the YBCO-nano-YBZO composite with 80 vol.% of YBZO showed a conducting behavior; there is no superconducting transition up to 77 K. The resistivity of composites is dominated by YBZO for volume less than 50% of YBCO with a significant drop of occurring near these values of volume. The absence of a superconducting network through the composite sample or a low vol.% of YBCO may be the reason for this behavior. These results show that when YBCO is ~30 vol.% or above there are interconnected networks of superconducting grains for the super current to pass through the composite material, but for lower vol.% of YBCO, the continuous network of superconducting grains breaks away and the resistance becomes nearly equal to that of pure insulator. Hence the value of percolation threshold for the YBCO-nano-YBZO composite sample lies between 30 and 40 vol.% of YBCO in the composite.

The resistivity and temperature coefficient of resistivity, at room temperature, are shown in Figure 5 as a function of vol.% of YBCO () in the composite. In the normal state, YBCO behaves as a metallic conductor and shows resistivity ~10 μΩm. However the resistivity of composites is dominated by YBa₂ZrO_5.5 for lower vol.% of YBCO with a significant drop of occurring near 30–50 vol.%. The behavior of correlates with that of , which increases sharply towards that of YBCO starting from vol.%. So if we assumed that the electrical transport behavior in YBCO-nano-YBZO composites is percolative, the percolation threshold is between 0.3 and 0.4. Thus, the superconducting percolation threshold and normal state percolation threshold values of YBCO-nano-YBZO composites lie in the same range. The electrical properties of the superconductor-insulator system can be described in [27, 28] where and are constants, is the critical volume fraction of superconductor at which changes dramatically and is called the percolation threshold, is the vol.% of superconducting material in the composite, and and are the critical exponent describing the transport properties of the composite system. The values , , , and are found from the log-log plot of versus and versus with . The value of is adjusted so that the log-log plots of and give a straight line.

Log-log plot of versus , for , is shown in Figure 6 which gave the exponents and μΩ m. And Figure 7 shows the log-log plot of in function of for system which gave the values and μΩ m. Least square fits were performed to determine the slope of the plots which gave the values of exponents and . However for an idealized metal-insulator system and [29]. A great number of experiments on conducting-insulator systems show percolation thresholds in agreement with percolation theory [19–21]. However, there are few others which reported variation from the universal values [27, 30].

The values of critical current densities measured for different samples at zero applied magnetic field are shown in Table 1. The self-field is found to be decreasing on the addition of nanocrystalline YBZO in YBCO. A judicious explanation is the existence of larger defect density, since is more sensitive to the defect density. The analysis of the current flow in the composite samples reveals the weak link behavior in the majority of grain connections. But this does not necessarily mean that weak (Josephson) grain coupling is absent in these samples. However, the number of stronger grain connections must be significantly above the percolation threshold [28], which is defined as the minimum fraction for a continuous current path.

YBa₂Cu₃O_7−δ superconductor will start to melt and decompose when it is sintered at higher temperature. The values of , , and obtained for different systems of composites vary due to many factors. The critical exponents, and , are a measure of the order of interaction between normal metal and insulator. The value for ideal percolation threshold is around 17 vol.% of metal in the system for a perfect metal-insulator composite without any interaction or reaction between the two. The normal state and superconducting percolation threshold values of YBCO-nano-YBZO (0.3 vol.% of YBCO) composites are in closer ranges as expected for an idealized percolation system and are lower than those observed in conventionally prepared YBZO-YBCO (0.35 vol.% of YBCO) composite [25]. This may be due to the better chemical nonreactivity between YBCO and nano-YBZO. Furthermore, there is a negligible conductivity below percolation threshold while it is expected to be zero in ideal percolative systems. The nonreactivity of YBCO with nano-YBZO even at high processing temperature also points to the fact that nano-YBZO is a suitable substrate for YBCO superconductor and thus to develop devices based on high temperature superconductor films and junctions.

4. Conclusion

In this paper we have studied the chemical reactivity and percolation behavior using electric transport measurements in polycrystalline YBa₂Cu₃O_7−δ superconductor-nano-YBa₂ZrO_5.5 composite. From structural analysis it is observed that the mixture of materials YBa₂ZrO_5.5 insulator with YBa₂Cu₃O_7−δ superconductor is a system where the particles of superconductor and insulator materials are found to coexist in a composite with two well-defined separate phases. Resistivity measurements of the composites synthesized in this work show an apparent percolative behavior with percolation threshold and critical exponents values and . Compared to the conventionally prepared YBZO, nanocrystalline YBZO mixed superconductor-insulator system showed a better percolation behavior. Thus, as discussed earlier, YBZO is chemically stable with the YBCO superconductor and, at the same time, it did not have any deteriorating effect on the superconducting property characterized by the transition temperature.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgment

Sukumariamma Vidya acknowledges CSIR for financial assistance.

References

T. van Duzer, “Superconductor electronics,” Cryogenics, vol. 30, no. 12, pp. 980–995, 1990.
View at: Publisher Site | Google Scholar
T. van Duzer, “Superconductor electronics and power applications,” Proceedings of the IEEE, vol. 100, no. 11, pp. 2993–2995, 2012.
View at: Publisher Site | Google Scholar
N. McN Alford, T. W. Button, and J. D Birchall, “Processing, properties and devices in high-T_c superconductors,” Superconductor Science and Technology, vol. 3, no. 1, 1990.
View at: Publisher Site | Google Scholar
T. K. Worthington, W. J. Gallagher, and T. R. Dinger, “Anisotropic nature of high-temperature superconductivity in single-crystal Y₁Ba²Cu₃O_7-x,” Physical Review Letters, vol. 59, no. 10, pp. 1160–1163, 1987.
View at: Publisher Site | Google Scholar
D. R. Harshman, G. Aeppli, E. J. Ansaldo et al., “Temperature dependence of the magnetic penetration depth in the high-T_c superconductor Ba₂YCu₃O_9-φ: evidence for conventional s-wave pairing,” Physical Review B, vol. 36, no. 4, pp. 2386–2389, 1987.
View at: Publisher Site | Google Scholar
A. Davidson and M. Tinkham, “Phenomenological equations for the electrical conductivity of microscopically inhomogeneous materials,” Physical Review B, vol. 13, no. 8, pp. 3261–3267, 1976.
View at: Publisher Site | Google Scholar
J. W. Essam, “Percolation theory,” Reports on Progress in Physics, vol. 43, no. 7, pp. 833–912, 1980.
View at: Publisher Site | Google Scholar | MathSciNet
M. Sahimi, Application of Percolation Theory, Taylor & Francis, London, UK, 1994.
K. Osamura, N. Matsukura, Y. Kusumoto, S. Ochiai, B. Ni, and T. Matsushita, “Improvement of critical current density in YBa₂Cu₃O_6+x superconductor by Sn addition,” Japanese Journal of Applied Physics, vol. 29, no. 9, pp. L1621–L1623, 1990.
View at: Google Scholar
S. H. Wee, A. Goyal, Y. L. Zuev, C. Cantoni, V. Selvamanickam, and E. D. Specht, “Formation of self-assembled, double-perovskite, Ba₂YNbO₆ nanocolumns and their contribution to flux-pinning and J_c in Nb-doped $YB a_{2} C u_{3} O_{7 - δ}$ films,” Applied Physics Express, vol. 3, no. 2, Article ID 023101, 2010.
View at: Publisher Site | Google Scholar
M. Coll, S. Ye, V. Rouco et al., “Solution-derived YBa₂Cu₃O_7-δ nanocomposite films with a Ba₂YTaO₆ secondary phase for improved superconducting properties,” Superconductor Science and Technology, vol. 26, no. 1, Article ID 015001, 2012.
View at: Publisher Site | Google Scholar
P. P. Rejith, S. Vidya, S. Vipinlal Solomon, and J. K. Thomas, “Flux-pinning properties of nanocrystalline HfO₂ add YBa₂Cu₃O_7-δ superconductor,” Physica Status Solidi B, vol. 251, pp. 809–814, 2014.
View at: Google Scholar
S. A. Harrington, J. H. Durrell, B. Maiorov et al., “rare earth tantalate pyrochlore nanoparticles for superior flux in YBa₂Cu₃ $O_{7 - δ}$ films,” Superconductor Science and Technology, vol. 22, no. 2, Article ID 022001, 2009.
View at: Publisher Site | Google Scholar
Y. P. Yadava, E. Montarroyos, J. M. Ferreira, and J. Albino Aguiar, “Synthesis and study of the structural characteristics of a new complex perovskite oxide Sr₂HoHfO_5.5 for its use as a substrate for YBCO superconducting films,” Physica C: Superconductivity, vol. 354, no. 1–4, pp. 444–448, 2001.
View at: Publisher Site | Google Scholar
J. Koshy, J. K. Thomas, J. Kurian, Y. P. Yadava, and A. D. Damodaran, “Development and characterization of GdBa₂NbO₆, a new ceramic substrate for YBCO thick films,” Materials Letters, vol. 17, no. 6, pp. 393–397, 1993.
View at: Publisher Site | Google Scholar
R. Jose, A. M. John, J. K. Thomas et al., “Synthesis, crystal structure, dielectric properties, and potential use of nanocrystalline complex perovskite ceramic oxide Ba₂ErZrO_5.5,” Materials Research Bulletin, vol. 42, no. 12, pp. 1976–1985, 2007.
View at: Publisher Site | Google Scholar
K. V. Paulose, M. T. Sebastian, K. R. Nair, J. Koshy, and A. D. Damodaran, “Synthesis of Ba₂YZrO₆: a new phase in YBa₂Cu₃O₇ -ZrO₂ system and its suitability as a substrate material for YBCO films,” Solid State Communications, vol. 83, no. 12, pp. 985–988, 1992.
View at: Publisher Site | Google Scholar
J. M. Phillips, “Substrate selection for high-temperature superconducting thin films,” Journal of Applied Physics, vol. 79, no. 4, pp. 1829–1848, 1996.
View at: Publisher Site | Google Scholar
S. Vidya, K. C. Mathai, P. P. Rejith, S. Solomon, and J. K. Thomas, “SmBa₂NbO₆ nanopowders, an effective percolation network medium for YBCO superconductors,” Advances in Materials Science and Engineering, vol. 2013, Article ID 578434, 7 pages, 2013.
View at: Publisher Site | Google Scholar
J. Kurian, P. R. S. Wariar, P. K. Sajith, and J. Koshy, “Percolation behavior of the normal-state resistivity and superconductivity of the YBa₂Cu₃O_7-δ-Ba₂GdNbO₆ composite system,” Journal of Superconductivity and Novel Magnetism, vol. 11, no. 6, pp. 683–687, 1998.
View at: Google Scholar
P. R. S. Wariar, J. Koshy, J. Kurian, Y. P Yadava, and A. D Damodaran, “Percolation studies in SmBa₂SbO₆-YBa₂Cu₃O_7-δ composite system,” Modern Physics Letters B, vol. 9, no. 10, p. 585, 1995.
View at: Publisher Site | Google Scholar
H. Tovar, O. O. Díaz, D. A. L. Téllez, and J. Roa-Rojas, “Ba₂NdZrO_5.5 as a potential substrate material for YBa₂Cu₃O_7-δ superconducting films,” Physica Status Solidi C: Current Topics in Solid State Physics, vol. 4, no. 11, pp. 4294–4297, 2007.
View at: Publisher Site | Google Scholar
O. O. Diaz, L. D. López Carreño, J. Albino Aguiar, J. Roa-Rojas, and D. A. Landínez Téllez, “tructural ordering, chemical stability and percolative effect analysis in YSr₂SbO₆/YBa₂Cu₃O_7-δ complex perovskite composites,” Physica C, vol. 408–410, pp. 886–888, 2004.
View at: Google Scholar
Q. Madueño, D. A. Landínez Téllez, and J. Roa-Rojas, “Production and characterization of Ba₂NdSbO₆ complex perovskite as a substrate for YBa₂Cu₃O_7-δ superconducting films,” Modern Physics Letters B, vol. 20, p. 427, 2006.
View at: Publisher Site | Google Scholar
K. V. Paulose, M. K. Jayaraj, J. Koshy, and A. D. Damodaran, “Preparation and properties of Ba₂YZrO₆YBa₂Cu₃O₇ composites,” Solid State Communications, vol. 87, no. 2, pp. 147–150, 1993.
View at: Publisher Site | Google Scholar
R. Jose, J. James, A. M. John, D. Sundararaman, R. Divakar, and J. Koshy, “New combustion process for nanosized YBa₂ZrO_5.5 powders,” Nanostructured Materials, vol. 11, no. 5, pp. 623–629, 1999.
View at: Publisher Site | Google Scholar
J. J. Lin, W. Y. Lin, and R. F. Tsui, “Electrical transport and superconductivity in the Al₂O₃-Bi₂Sr_1.8Ca_1.2Cu₂Oy and MgO-Bi₂Sr_1.8Ca_1.2Cu₂O_y composites,” Physica C, vol. 210, no. 3-4, pp. 455–462, 1993.
View at: Google Scholar
M. Eisterer, J. Emhofer, S. Sorta, M. Zehetmayer, and H. W. Weber, “Connectivity and critical currents in polycrystalline MgB₂,” Superconductor Science and Technology, vol. 22, no. 3, Article ID 034016, 2009.
View at: Publisher Site | Google Scholar
D. Stauffer and A. Aharony, Introduction to Percolation Theory, Taylor and Francis, 1994.
J. Wu and D. S. McLachlan, “Percolation exponents and thresholds obtained from the nearly ideal continuum percolation system graphite-boron nitride,” Physical Review B, vol. 56, no. 3, pp. 1236–1248, 1997.
View at: Google Scholar

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Copyright © 2014 Pullanhiyodan Puthiyaveedu Rejith et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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