Structure and properties of BSCCO-whiskers grown from amorphous precursors with foreign dopants

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Abstract

The process of BSCCO whisker growth from varying Bi2Sr2Ca3Cu5AlxMyOz(M = Li, Mg,Pb, Y, Zr, V, Nb, Mo) compositions of amorphous precursor have been investigated. The Al2O3ZrO2 double oxide favours the whisker growth even if the glass precursor contains a crystalline portion. The whiskers grown from a 2235 plate and from 2235AlZr plate had a similar cation composition, but in the second case the Sr and Cu content in the crystal tends to be lower. The Al and Zr additives are distributed uniformly inside the plates with foreign framework fabrication. The variation of whisker structure parameters and superconducting properties have been investigated. The tunnelling characteristics for break junctions of whiskers are discussed and a model of BSCCO whisker growth is presented.

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Cited by (24)

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    One of the main concerns about YBCO whiskers employment for these kinds of investigation is their synthesis in useful quantities, with respect to the BSCCO counterpart. As a matter of fact, much information is given in the literature about BSCCO whiskers and what is favoring or allowing their growth [11]. In this case, alumina addition as a precursor dopant has been found to drastically enhance the formation of such whiskers [12–15].

  • Crystallization of glass-ceramic Bi<inf>3</inf>Sr<inf>2</inf>Ca <inf>2</inf>Cu<inf>3</inf>O<inf>y</inf> superconducting system

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    In order to achieve good superconducting properties, the crystallization mechanism and so kinetics must be carefully determined. Some models for the crystallization mechanism in the HTc materials have been developed by some research groups, such as vapor–liquid–solid (VLS) mechanism [6–8], vapor-phase-deposition on a screw dislocation mechanism [9], growth via ‘melt transport under a temperature gradient’ (MTTG) mechanism [10,11], ‘Microcrucible’ self supporting mechanism [12,13], generalized growth mechanism (GGM) [14], solid-state growth [15], growth induced by the inner stress from the substrates [16], self-flux growth mechanisms [17,18], seeded growth [19,20], models depending based on the ‘catalytic’ impurity [6]. However, there is no consensus among the models.

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    The Melt Transport under Temperature Gradient model is based on the fast transport of ions in the matrix. The driving force is the temperature gradient in the sample [15–17]. The Microcrucible model was suggested by Matsubara et al. [18].

  • Application of elevated magnetic fields during growth of BiSrCaCuO superconducting whiskers and studies of growth defects for better understanding of the growth mechanism

    2004, Journal of Crystal Growth
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    The role of the atmosphere (cation and oxygen) can be active, i.e. cations in the vapor state are supplied to the growth site of the whiskers generating a chemical gradient or of passive type, i.e. cation vapor environment ensures local equilibrium with liquid phase and prevention of cation evaporation and escape from the growth site. For the first case of active role, the driving force would be super-saturation of the liquid due to the continuous arrival of cation vapors at the growth site and for the situation of the passive role, the driving force of the self-growth of whiskers should be thermal gradients [21,22] or capillarity forces of the liquid [18] generating the necessary chemical gradient. On the other hand, analysis of the profile of the kinetics curves of growth are closer to the VLS model [7].

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Permanent address: Department of Physics, Bergische Universität Wuppertal, Gauss-Str. 20, D-42097 Wuppertal, Germany.

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