Superconducting structure

Details Superconducting structure Superconducting structure

1998-09-14

2003-04-01

Dunn, Tom (Department: 1725)

Stock material or miscellaneous articles

Composite

Of inorganic material

C428S702000, C505S234000

Reexamination Certificate

active

06541136

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to superconducting structures and to a method of improving superconducting properties of selected (RE)Ba
2
Cu
3
O
7
films, where RE is a selected rare earth element.
BACKGROUND OF THE INVENTION
Since the discovery of high-temperature superconducting (HTS) materials (superconducting above the liquid nitrogen temperature of 77 K) there have been efforts to research and develop various technology and engineering applications using such HTS materials. In thin film superconductor devices, the most progress has been made with fabrication of Josephson junctions and microwave devices utilizing an oxide superconductor including yttrium, barium, copper and oxide in the well-known basic composition of YBa
2
Cu
3
O
7−x
(hereinafter referred to as Y123). At liquid nitrogen temperatures and in high magnetic fields, the J
c
of Y123 is superior to those of the bismuth, thallium and mercury based HTS materials. Thus, Y123 has generally been the preferred material for thin film and bulk applications.
Even though Y123 is the material of choice for HTS applications, it still has a few problems. One problem is that Y123 has one of the lowest T
c
's among (RE)Ba
2
Cu
3
O
7−x
materials (hereinafter referred to as RE123) which can limit J
c
at the liquid nitrogen temperature (since J
c
depends on T
c
; J
c
≈(1−T/T
c
)
3/2
). Another problem is that compared with SmBa
2
Cu
3
O
7
(Sm123) and NdBa
2
Cu
3
O
7
(Nd123) films, Y123 films have a much rougher surface morphology which is detrimental for any device application and imposes a materials challenge. Still another problem is that it has been known that Nd123 has a larger J
c
in high magnetic fields than Y123. Hence, it has been important to continue development of RE123 films for various HTS applications. Previously, there have been some efforts to fabricate high quality RE123 films. Sm123 and Nd123 films with good superconducting properties (T
c
>90 K and J
c
>10
6
Amperes per square centimeter (A/cm
2
)) and smooth surface morphology have been fabricated using Pulsed Laser Deposition (PLD), Molecular Beam Epitaxy (MBE), and Coevaporation techniques. However, the optimization of film properties has only been achieved by using barium-rich targets, post-annealing of the films, or changing the stoichiometry of the targets, and it has been difficult to reproducibly fabricate high quality films.
There have been several attempts to overcome these difficulties by using a buffer layer to produce RE123 films. For example, U.S. Pat. No. 5,232,900 describes the use of a non-superconducting buffer layer. U.S. Pat. No. 5,512,541 describes the deposition of superconducting films on a superconducting single crystal substrate. U.S. Pat. No. 5,629,268 describes the deposition of multilayers on a bottom superconductor without damaging its superconducting properties. Kwon et al., Appl. Phys. Lett., 62,1289-1291 (1993), describe a buffer layer of yttrium-doped Pr123 in order to improve the superconducting properties of ultra-thin Y123 films.
Despite these earlier efforts, the need to find additional buffer materials suitable for reproducible deposition of various RE123 films has remained. Thus, an object of the present invention is buffer materials suitable for reproducible deposition of various RE123 films.
Another object of the present invention is to simplify the process conditions needed to form various RE123 films.
SUMMARY OF THE INVENTION
To achieve the foregoing and other objects, and in accordance with the purposes of the present invention, as embodied and broadly described herein, the present invention provides a superconductive structure including a dielectric oxide substrate, a thin buffer layer of a superconducting material thereon; and, a layer of a rare earth-barium-copper oxide superconducting film thereon the thin layer of yttrium-barium-copper oxide, the rare earth selected from the group consisting of samarium, gadolinium, ytterbium, erbium, neodymium, dysprosium, holmium, lutetium, a combination of more than one element from the rare earth group and a combination of one or more elements from the rare earth group with yttrium, the buffer layer of superconducting material characterized as having chemical and structural compatibility with the dielectric oxide substrate and the rare earth-barium-copper oxide superconducting film. Preferably, the superconducting material characterized as having chemical and structural compatibility with the superconducting (rare-earth)-barium-copper oxide is yttrium-barium-copper oxide.
The present invention also provides a method of improving the superconducting properties of a superconducting (rare-earth)-barium-copper oxide structure by use of a thin layer of a superconducting material characterized as having chemical and structural compatibility with the superconducting (rare-earth)-barium-copper oxide as a buffer layer situated directly between a dielectric oxide substrate and the layer of superconducting (rare-earth)-barium-copper oxide. Preferably, the superconducting material characterized as having chemical and structural compatibility with the superconducting (rare-earth)-barium-copper oxide is yttrium-barium-copper oxide.


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Kwon et al., “High critical current densities in ultrathin YBa2Cu3O(7-beta) films sandwiched between (PrXY(1-X))Ba2Cu3O(7-beta) layers” Mar. 15, 1993, Applied Physics Letters 62(11), pp. 1289-1291.

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