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High critical current density and enhanced irreversibility field in superconducting MgB2 thin films

Abstract

The discovery of superconductivity at 39 K in magnesium diboride1 offers the possibility of a new class of low-cost, high-performance superconducting materials for magnets and electronic applications. This compound has twice the transition temperature of Nb3Sn and four times that of Nb-Ti alloy, and the vital prerequisite of strongly linked current flow has already been demonstrated2,3,4,5. One possible drawback, however, is that the magnetic field at which superconductivity is destroyed is modest. Furthermore, the field which limits the range of practical applications—the irreversibility field H*(T)—is approximately 7 T at liquid helium temperature (4.2 K), significantly lower than about 10 T for Nb-Ti (ref. 6) and 20 T for Nb3Sn (ref. 7). Here we show that MgB2 thin films that are alloyed with oxygen can exhibit a much steeper temperature dependence of H*(T) than is observed in bulk materials, yielding an H* value at 4.2 K greater than 14 T. In addition, very high critical current densities at 4.2 K are achieved: 1 MA cm-2 at 1 T and 105 A cm-2 at 10 T. These results demonstrate that MgB2 has potential for high-field superconducting applications.

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Acknowledgements

The work at the University of Wisconsin was supported by funding from the US Department of Energy, the Air Force Office of Scientific Research, the National Science Foundation through the Materials Research Science and Education Center for Nanostructured Materials and a David Lucile Packard Fellowship (C.B.E.). The work at Princeton University was supported by the National Science Foundation and the US Department of Energy.

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Correspondence to C. B. Eom.

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Further reading

Figure 1: X-ray diffraction θ–2θ scans of films 1 (black curve), 2 (red curve) and 3 (blue curve), showing both (002) MgB2 and (002) MgO peaks.
Figure 2: Resistivity as a function of temperature.
Figure 3: Magnetization measurements for films 1 (red curves), 2 (black curves), and 3 (blue curves).
Figure 4: Transmission electron microscopy.

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