We have fabricated Cu‐Ni superlattices with exclusive [100] modulating orientation by using a dc magnetron sputtering system. The layer thicknesses of both Cu and Ni range from 5 to 125 Å. The high quality of the samples is confirmed by the intense satellite peaks in the x‐ray diffraction. The spontaneous magnetization at 5 K, which is found to be inversely proportional to the Ni layer thickness, vanishes at two Ni atomic planes. A very large difference in magnetic surface anisotropy has been found between [100] and [111] textured Cu‐Ni superlattices, displaying the important role of modulating orientation on the magnetic properties of superlattice.

1.
See reviews in Synthetic Modulated Structures, edited by L. L. Chang and B. C. Giessen (Academic, New York, 1985).
2.
E. M.
Gyorgy
,
J. F.
Dillon
, Jr.
,
D. B.
McWhan
,
L. W.
Rupp
, Jr.
,
L. R.
Testardi
, and
P. J.
Flanders
,
Phys. Rev. Lett.
45
,
57
(
1980
).
3.
E. M.
Gyorgy
,
D. B.
MeWhan
,
J. F.
Dillon
, Jr.
,
L. R.
Walker
, and
J. V.
Waszczak
,
Phys. Rev. B
25
,
6739
(
1982
).
4.
J. Q.
Zheng
,
J. B.
Ketterson
,
Charles M.
Falco
, and
Ivan K.
Schuller
,
J. Appl. Phys.
53
,
3150
(
1982
).
5.
T.
Jarlborg
and
A. J.
Freeman
,
Phys. Rev. Lett.
45
,
653
(
1980
).
6.
J.
Tersoff
and
L. M.
Falicov
,
Phys. Rev. B
26
,
459
(
1982
).
7.
Ding‐sheng
Wang
,
A. J.
Freeman
, and
H.
Krakauer
,
Phys. Rev. B
26
,
1340
(
1982
).
8.
L.
Néel
,
J. Phys. Radium
15
,
225
(
1954
).
9.
In Ref. 2, the K5 value of [111] Cu‐Ni superlattices was indicated to be 0.3 erg/cm2. The correct K5 value is 0.12 erg/cm2 according to relation (2) in the text.
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