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Ultrathin films and superlattices of high Tc superconductors controlled in the unit-cell scale using RHEED oscillations

Isolated ultrathin films of YBa 2Cu 3O 7−x (YBCO) on PrBa 2Cu 3O 7−x (PrBCO) and YBCO/PrBCO superlattices were epitaxially grown on SrTiO 3 by reactive coevaporation with measurement of reflection high energy electron diffraction (RHEED) specular intensity. X-ray diffraction profiles and cross secti...

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Bibliographic Details
Published in:Physica. C, Superconductivity Superconductivity, 1991-12, Vol.185, p.204-209
Main Authors: Bando, Yoshichika, Terashima, Takahito, Shimura, Kenichi, Sato, Toshifumi, Matsuda, Yuji, Komiyama, Susumu, Kamigaki, Kousel, Terauchi, Hikaru
Format: Article
Language:English
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Summary:Isolated ultrathin films of YBa 2Cu 3O 7−x (YBCO) on PrBa 2Cu 3O 7−x (PrBCO) and YBCO/PrBCO superlattices were epitaxially grown on SrTiO 3 by reactive coevaporation with measurement of reflection high energy electron diffraction (RHEED) specular intensity. X-ray diffraction profiles and cross sectional electron microscopic (TEM) observation reveal that the heterostructures are excellent crystallinity with no interface disorder and fit for the ptudy of superconductivity of the 1 unit-cell layer of YBCO. The 1 unit-cell layer of YBCO sandwiched between PrBCO layers exhibits a superconducting transition with the onset temperature at 70K and the zero resistance at 30K. A reduction of the onset temperature is found to be mainly due to a decrease of the hole carriers but not due to the absence of interlayer coupling. It was demonstrated that the 1 unit-cell layer of YBCO needed the overlayer of PrBCO to give rise to superconductivity. The overlayer of PrBCO may have the role of supply of carriers for the underlying YBCO layer. The resistive transition for the ultrathin YBCO layer below 4 unit-cells thick was independent of the magnetic field up to 10T applied parallel to the CuO 2 layer.
ISSN:0921-4534
1873-2143
DOI:10.1016/0921-4534(91)91973-8