EPITAXIAL Y1BA2CU3O7-DELTA THIN-FILMS WITH (103) (110)-ORIENTATION AND (100)/(010)-ORIENTATION ON NDGAO3 AND SRTIO3 SUBSTRATES GROWN BY ION-BEAM SPUTTER-DEPOSITION/
Jp. Krumme et al., EPITAXIAL Y1BA2CU3O7-DELTA THIN-FILMS WITH (103) (110)-ORIENTATION AND (100)/(010)-ORIENTATION ON NDGAO3 AND SRTIO3 SUBSTRATES GROWN BY ION-BEAM SPUTTER-DEPOSITION/, Journal of materials research, 9(12), 1994, pp. 3032-3049
A fully oxygen-compatible ion-beam sputter deposition process (IBS) ha
s been implemented for investigation of four film/substrate couples: (
103)/(110) YBCO on (110)SrTiO3 (STO) and on (100)NdGaO3 (NGO), and (10
0)/(010)YBCO on (110)NGO and on (100)STO. For comparison, some (103)/(
110)YBCO films have also been prepared by off-axis rf-magnetron sputte
ring. Below about 600-degrees-C semiconducting, sub-nm flat, and perfe
ctly single-crystalline YBCO films crystallize on these substrates wit
h a crystallographic unit cell of about 1/3 of the Cu-O subcell of YBC
O and perfect registration with the Ti4+ -O and Ga3+ -O sublattice of
STO and NGO, respectively. At higher temperature superconducting YBCO
films grow coherently epitaxially in the first approximately 100 nm th
ickness; in thicker films the lattice-misfit strain relaxes to the ''f
ree'' lattice constants. Above approximately 680-degrees-C a faceted (
103)YBCO orientation grows on (110)STO and (100)NGO substrates with un
iform in-plane orientation of the [010]YBCO direction parallel to [001
]STO and [001]NGO. Along [010]YBCO the (103)YBCO films exhibit high cr
ystalline perfection and intrinsic superconducting properties approach
ing those of (001)YBCO films in the plane; i.e., T(c,0) > 88 K, DELTAT
(c,0) < 0.6 K, R300/R100 > 2.9, rho100 > 250 muOMEGAcm, and j(c) (77 K
) greater-than-or-equal-to 10(6) A/cm2. Practical use of (103)YBCO fil
ms is hampered by the large surface roughness. Above approximately 680
-degrees-C a mixed (100)/(010)YBCO orientation grows on (110)NGO subst
rates, exhibiting a very smooth surface but less attractive supercondu
cting properties; typically, T(c,0) less-than-or-equal-to 80 K, DELTAT
(c,0) approximately 1 K, R300/R100 approximately 1.2, rho100 > 3 mOMEG
Acm, and j(c) (77 K) less-than-or-equal-to 10(5) A/cm2. On (100)STO su
bstrates the YBCO film orientation varies from pure (100)YBCO between
approximately 580 and approximately 630-degrees-C and mixed (100)/(010
)YBCO below approximately 660-degrees-C to pure (001) YBCO above appro
ximately 670-degrees-C. With rising temperature the surface roughness
increases from <2 to approximately 6 nm-rms, while the other parameter
s continuously improve to state-of-the-art values for c perpendicular-
to-oriented films. Specifically, mixed (100)/(010)YBCO films reach T(c
,0) > 86 K, DELTAT(c,0) approximately 1 K, R300/R100 > 2.8, rho100 < 3
mOMEGAcm, and j(c) (77 K) > 10(5) A/cm2. (100)/(010)YBCO films on (10
0)STO are a promising candidate for sandwich-type SIS-JJ.