Stock material or miscellaneous articles – All metal or with adjacent metals – Having magnetic properties – or preformed fiber orientation...
Reexamination Certificate
2002-02-21
2004-03-23
Nakarani, D. S. (Department: 1773)
Stock material or miscellaneous articles
All metal or with adjacent metals
Having magnetic properties, or preformed fiber orientation...
C428S670000, C428S409000, C428S690000, C428S690000, C428S690000
Reexamination Certificate
active
06709768
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a perpendicular magnetic recording medium, a process of production thereof, and a magnetic storage equipped therewith. The perpendicular magnetic recording medium has a magnetic layer composed of columnar magnetic crystal grains whose principal component is cobalt, and it is characterized by reduced thermal decay. The magnetic storage has a recording density in excess of 50 Gbit/in
2
.
2. Description of the Related Arts
There is an increasing demand for higher recording density in magnetic storage from the standpoint of increasing the storage capacity, miniaturizing the apparatus, and reducing the number of parts. The existing magnetic recording medium is based on longitudinal magnetic recording. It records information by means of mutually opposed domains (recording bits) which are magnetized in the direction parallel to the surface of the substrate. For a longitudinal magnetic recording medium to be capable of high-density recording, it should have a low noise level. One effective way of noise reduction is finely reducing in size of crystal grains and even out particle diameters (or reduce the dispersion of particle diameters). This is exemplified by the invention (disclosed in Japanese Patent Laid-open No. 269548/1998) relating to a longitudinal recording medium which specifies for noise reduction the optimum particle diameter and the optimum dispersion of particle diameters.
Increasing the recording density in longitudinal magnetic recording will have a limit because of the necessity for more finely reduced crystal grains than before. However, extremely small crystal grains encounter problems with thermal decay. In other words, their magnetization for recording is decayed by even such small thermal energy as generated at room temperature. In order to address the problem with thermal decay, there has been proposed the perpendicular magnetic recording system, which is attracting great attention. It is essentially suitable for high-density recording by virtue of its property that the thermal stability of magnetization improves as the recording density increases.
The recording medium for perpendicular magnetization under wide study is one which has a magnetic layer composed of practically columnar crystal grains, with their (00.1) plane oriented nearly parallel to the surface of the substrate for their magnetic anisotropy in the direction perpendicular to the substrate. The most widely studied recording medium with a CoCr alloy magnetic film has a coercive force of about 3000 Oe (equivalent to approximately 79.7 A/m in SI unit). In order to put to practical use the magnetic recording medium composed mainly of cobalt, the present inventors carried out extensive studies, which led to an important finding that a magnetic film of cobalt alloy with the c-axis (or the (00.1) direction) oriented perpendicular to the surface of the substrate has a stacking fault density which is two to three times higher than that of cobalt alloy magnetic film with longitudinal orientation.
The perpendicular magnetic recording also needs a magnetic recording medium with low noise and high thermal stability. No matter whether it is of longitudinal recording type or perpendicular recording type, the magnetic layer with many stacking faults will be poor in magnetic anisotropy, coercivity, and thermal stability. For high thermal stability of recording magnetization, it is necessary to reduce the stacking fault density in the magnetic film.
The major cause of stacking faults is ingression of a plane corresponding to the fcc-like structure into the hcp structure. It is believed that the stacking fault density will decrease if the magnetic film is formed at a low temperature desirable for the hcp structure to be stable. However, the present inventors' elucidation suggests that the magnetic film formed at low temperatures decreases in stacking fault density but does not increase in coercive force because crystal grains constituting the magnetic film have a broad distribution of particle diameters. Raising the film-forming temperature to reduce the dispersion of particle diameters increases the stacking fault density, with coercivity remaining low.
The longitudinal magnetic recording medium is inherently little subject to stacking faults because crystal grains constituting the magnetic layer are epitaxially grown on the underlayer such that the c-axis of magnetic grain is longitudinally oriented. Epitaxial growth takes place in the direction toward the most stable energy state. Thus, there is almost no possibility that epitaxial growth brings about an unstable energy state due to ingression of a crystal phase different from that of the fcc structure.
It was found from the present inventors' investigation that the stacking fault density in the longitudinal magnetic recording medium formed at about 250° C. is one half to one-third of that in the perpendicular magnetic recording medium. It was also found that the dispersion of particle diameters in the longitudinal magnetic recording medium is about 0.3 to 0.4, which is determined almost entirely by the dispersion of particle diameters in the underlying film of chromium alloy and which does not depend on the film-forming temperature.
The film-forming temperature affects the stacking fault density and the dispersion of particle diameters as shown in
FIGS. 1 and 2
respectively. It is to be noted from
FIG. 1
that the stacking fault density decreases as the film-forming temperature decreases. It is also to be noted from
FIG. 2
that the dispersion of particle diameters increases as the film-forming temperature decreases. This suggests that it is difficult to have both of a low stacking fault density and a low dispersion of particle diameters. Such an antinomic relation of the film-forming temperature with the stacking fault density and the dispersion of particle diameters has never been anticipated in the technology of longitudinal magnetic recording medium.
OBJECT AND SUMMARY OF THE INVENTION
It is an object of the present invention to provide a perpendicular magnetic recording medium which is made of conventional CoCr alloy as a magnetic material and yet has good thermal stability owing to adequate control over the stacking fault density and the dispersion of particle diameters. Being made of a conventional magnetic material, the recording medium is economically advantageous.
It is another object of the present invention to provide a method of adequately controlling the stacking fault density and the dispersion of particle diameters.
The objects of the present are achieved by controlling the stacking fault density (R) and the dispersion of particle diameters (&Dgr;D/<D>) of the magnetic film, which is composed of magnetic crystal grains whose principal component is cobalt, such that the product of &Dgr;D/<D>×R is no larger than 0.02.
The stacking fault density relates with coercive force as shown in FIG.
3
. Incidentally, dotted lines in
FIG. 3
are contour lines for some values of the dispersion of particle diameters which are determined by the coercive force and the stacking fault density. It is noted from
FIG. 3
that the coercive force increases as the stacking fault density decreases and the coercive force slightly decreases as the stacking fault density decreases further (due to increase in the dispersion of particle diameters).
FIG. 4
shows the contour lines of coercive force which are determined by the stacking fault density and the dispersion of particle diameters. It is noted that the coercive force no smaller than 4000 Oe is obtained in the area (under the thick line) in which the product of the stacking fault density and the dispersion of particle diameters is no larger than 0.02. The coercive force of 4000 Oe is necessary to suppress thermal decay. With a value of coercive force no smaller than 4000 Oe, the magnetic recording medium has a value of Ku·V/k·T no smaller than 60 which is necessary to ensure thermal stability for recor
Hosoe Yuzuru
Takahashi Yoshio
Tamai Ichiro
Tanahashi Kiwamu
Bernatz Kevin M
Hitachi Global Storage Technologies Japan Ltd.
Mattingly Stanger & Malur, P.C.
Nakarani D. S.
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