Single crystals of Sr2RuO4 were grown by the floating zone melting technique. The crystals have the K2NiF4 structure and display a metallic resistivity behavior in the a‐b‐plane between 300 and 4.2 K (ρab≂10−4 Ω cm at 300 K). The in‐plane lattice mismatch between YBa2Cu3O7−δ (001) and Sr2RuO4 (001) is smaller than 1.3%, better than that to SrTiO3 {100}. Epitaxial films of YBa2Cu3O7−δ with Tc(R=0) as high as 86 K have been grown on Sr2RuO4 crystals. The epitaxial growth of YBa2Cu3O7−δ on Sr2RuO4 was revealed by four‐circle x‐ray diffraction as well as by transmission electron microscopy.
REFERENCES
1.
A.
Callaghan
, C. W.
Moeller
, and R.
Ward
, Inorg. Chem.
5
, 1572
(1966
).2.
3.
J. A.
Wilson
, F. J.
Di Salvo
, and S.
Mahajan
, Adv. Phys.
24
, 117
(1975
).4.
5.
Chemistry and Physics of Carbon (Marcel Dekker, New York, 1973), Vol. 11, pp. 114–115.
6.
J.
Geerk
, X. X.
Xi
, H. C.
Li
, W. Y.
Guan
, P.
Kus
, M.
Höbel
, G.
Linker
, O.
Meyer
, F.
Ratzel
, C.
Schultheiss
, R.
Smithey
, B.
Strehlau
, and F.
Weschenfelder
, Int. J. Mod. Phys. B
3
, 923
(1989
).7.
A.
Catana
, R. F.
Broom
, J. G.
Bednorz
, J.
Mannhart
, and D. G.
Schlom
, Appl. Phys. Lett.
60
, 1016
(1992
).
This content is only available via PDF.
© 1992 American Institute of Physics.
1992
American Institute of Physics
You do not currently have access to this content.