Uniform deposition of YBa sub 2 Cu sub 3 O sub 7 minus. delta. films over large areas using ion-beam sputtering

Uniform films of YBaCuO have been deposited over 4-in.- (100-mm) diam, unheated Si wafers using ion-beam sputtering of a stoichiometric YBa{sub 2}Cu{sub 3}O{sub 7{minus}{delta}} target. Rutherford backscattering spectrometry reveals that within a 3-in. diam, the thickness variation is {plus minus}2....

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Veröffentlicht in:Journal of applied physics 1991-12, Vol.70:11
Hauptverfasser: Lichtenwalner, D.J., Soble, C.N. II, Woolcott, R.R. Jr, Auciello, O., Kingon, A.I.
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Sprache:eng
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Zusammenfassung:Uniform films of YBaCuO have been deposited over 4-in.- (100-mm) diam, unheated Si wafers using ion-beam sputtering of a stoichiometric YBa{sub 2}Cu{sub 3}O{sub 7{minus}{delta}} target. Rutherford backscattering spectrometry reveals that within a 3-in. diam, the thickness variation is {plus minus}2.9%, and the compositional uniformity of Y, Ba, and Cu is {plus minus}0.9%, {plus minus}5.2%, and {plus minus}3.4%, respectively. The average film composition is Y{sub 1.03}Ba{sub 1.88}Cu{sub 3.09}O{sub 7{minus}{delta}}. Deposition onto unheated substrates virtually eliminates the problem of the low sticking coefficients of Ba and Cu, and is much simpler for film synthesis and processing. The observed difference from the 1:2:3 target composition is attributed mainly to angular differences in the sputtered-flux distribution of each element. These effects should be minimized by substrate rotation. In order to obtain useful superconducting films, a post-deposition anneal on a suitable substrate or buffer layer is required. Using a relatively low temperature ({similar to}810 {degree}C), low O{sub 2} pressure (1.2 Torr) post-anneal, we show that oriented, superconducting films can be obtained on single-crystal MgO and SrTiO{sub 3} substrates. Films annealed under these conditions on MgO are predominantly {ital c}-axis oriented, whereas those on SrTiO{sub 3} are predominantly {ital a}-axis oriented.
ISSN:0021-8979
1089-7550
DOI:10.1063/1.349822