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Related Concept Videos

Types Of Superconductors01:28

Types Of Superconductors

A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...

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Submicrometer Superconducting YBa2Cu3O6+x Particles Made by a Low-Temperature Synthetic Route.

H S Horowitz, S J McLain, A W Sleight

    Science (New York, N.Y.)
    |January 6, 1989
    PubMed
    Summary

    Researchers developed a new method to synthesize superconducting orthorhombic YBa(2)Cu(3)O(6+x) (orthorhombic 123). This process involves creating tetragonal 123 first, then oxidizing it to achieve superconductivity at 87 K.

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    Area of Science:

    • Materials Science
    • Solid-State Chemistry
    • Superconductivity

    Background:

    • Superconducting orthorhombic YBa(2)Cu(3)O(6+x) (orthorhombic 123) is typically formed by oxidizing the oxygen-deficient tetragonal phase (tetragonal 123).
    • A reliable synthesis route for high-quality tetragonal 123 is crucial for producing superconducting orthorhombic 123.

    Purpose of the Study:

    • To establish a novel synthetic pathway for producing superconducting orthorhombic YBa(2)Cu(3)O(6+x).
    • To demonstrate the feasibility of using solution-derived, carbon-free precursors for this synthesis.

    Main Methods:

    • Decomposition of solution-derived, carbon-free precursors (hydrated oxides, hyponitrites) at 650–700°C in an inert atmosphere to yield tetragonal 123.
    • Subsequent oxidation of the synthesized tetragonal 123 phase at 400°C to produce orthorhombic 123.
    • Characterization of superconductivity using Meissner effect and specific-heat measurements.

    Main Results:

    • A reproducible synthetic route was developed to produce tetragonal YBa(2)Cu(3)O(6+x) from carbon-free precursors.
    • Oxidation of the tetragonal phase yielded submicrometer particles of orthorhombic YBa(2)Cu(3)O(6+x).
    • The resulting orthorhombic 123 material exhibited superconductivity with a T(c) onset of approximately 87 K.

    Conclusions:

    • The developed method provides an effective route to synthesize superconducting orthorhombic YBa(2)Cu(3)O(6+x) via an intermediate tetragonal phase.
    • The use of solution-derived precursors offers a controlled and potentially scalable approach for producing high-quality superconducting materials.
    • This work confirms the established relationship between the tetragonal and orthorhombic phases in YBa(2)Cu(3)O(6+x) and its superconducting properties.