Stock material or miscellaneous articles – Circular sheet or circular blank
Reexamination Certificate
2003-03-21
2004-10-19
Mulvaney, Elizabeth (Department: 1774)
Stock material or miscellaneous articles
Circular sheet or circular blank
C428S064400, C428S064500, C428S064600, C430S270130
Reexamination Certificate
active
06805935
ABSTRACT:
CROSS REFERENCE TO RELATED APPLICATION
This application is based upon and claims the benefit of priority from the prior Japanese Patent Application No. 2002-86297 filed on Mar. 26, 2002 in Japan, the entire contents of which are incorporated by reference.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention generally relates to an optical recording medium for reversibly changing a state by irradiation with light beams to record information. More specifically,the invention relates to a phase change optical recording medium which has a change of state wherein the atomic arrangement of a thin film for holding recording changes between amorphous and crystalline arrangements.
2. Related Art
A typical phase change optical recording film has an amorphous atomic arrangement when its portion heated to its melting point or higher to melt is rapidly cooled. When the phase change optical recording film is held in a crystallized temperature range below the melting point for a predetermined time or longer, it is crystallized if its initial state is amorphous, whereas it remains crystal if its initial state is crystal. Since the intensity of reflected light from an amorphous region is different from the intensity of reflected light from a crystalline region, the principle of a phase change optical recording medium is that the intensity of reflected light is converted into the intensity of an electric signal to be analog-to-digital converted to read information.
There are two methods for increasing the amount of information capable of being recorded in a single recording medium, i.e. a recording capacity. One method is a method for scaling down the pitch of recording marks in track directions. In this method, if the degree of scale down proceeds, the pitch becomes smaller than the size of a reproducing light beam, so that there are some cases where two recorded marks are temporarily included in a reproducing beam spot. If the recording marks are sufficiently spaced from each other, a regenerative signal can be greatly modulated to obtain a signal having a large amplitude. However, if the recording marks are close to each other, the amplitude of the signal is small, so that errors are easy to occur when the signal is converted into digital data.
Another method for improving a recording density is a method for narrowing the track pitch. This method can increase the recording density without being greatly influenced by the decrease of the signal strength due to the scale down of the mark pitch. However, in this method, there is a problem in that, in a region in which a track pitch is substantially equal to or smaller than the size of a light beam, there is caused a so-called cross erase wherein information on a certain track deteriorates when a writing or erasing operation is carried out in an adjacent track.
Two causes of cross erase are considered. One cause is that, when adjacent tracks are irradiated with a beam, the light intensity of the beam at the bottom edge thereof within a subject track is not small, so that the recording mark of the track is deteriorated by only the effect of irradiation with light. The other cause is that, when adjacent tracks are heated by a light beam, generated heat is transferred to the tracks by heat transfer in film in-plane directions, so that the shape of a recording mark is deteriorated by the influence thereof. Since the influence of the cross erase due to the latter influence can be reduced by decreasing heat transfer in the film in-plane directions, it has been devised to reduce the cross erase by more greatly promoting heat conduction in directions perpendicular to the plane of a recording film than in the in-plane directions by forming a so-called rapid-cooling structure by arranging a film having a large conductivity and/or heat capacity in the vicinity of a recording film.
For example, a conventional phase change optical recording medium shown in
FIG. 10
comprises a substrate
301
, a metal reflecting film
302
formed on the substrate
301
, a transparent dielectric film
303
formed on the metal reflecting film
302
, a recording film
304
formed on the dielectric film
303
, a transparent dielectric film formed on the recording film
304
, and a cover layer
306
formed on the dielectric film
305
. That is, the dielectric film
303
is arranged between the recording film
304
and the metal reflecting film
302
for ensuring a signal strength by the reflection of light, and the dielectric film
303
is formed so as to be relatively thin, so that heat generated by the recording film
304
can easily escape to prevent heat from being transferred in the film in-plane direction. As the thickness of the dielectric film
303
decreases, heat transfer in direction perpendicular to the plane of the film can be promoted to improve cross erase.
However, if the dielectric film
303
is too thin, heat transfer to the reflecting film
302
starts simultaneously with heating due to laser beams during recording, so that there is a problem in that the temperature rise of the recording film
304
is insufficient, whereby the temperature of an area required to form a recording mark does not reach the melting point. In addition, if a laser power of erase level is applied, the mark cools immediately after heating. Therefore, the temperature of the mark can not be held in a temperature range capable of crystallizing the mark for a sufficiently long time, so that there is a problem in that it is difficult to crystallize the mark, i.e. to carry out an erasing operation, thereby remarkably deteriorating the erasing rate.
Conversely, if the dielectric film
303
is too thick, there is no problem on the power margin and erasing rate with respect to laser beams during recording. However, as described above, heat transfer into the plane of the film is not only promoted to violently cause cross erase, but the cooling rate of the recording film
304
is slow. Therefore, there is a problem in that the region melt during recording is crystallized again without being amorphous, so that the formed mark is too small.
Japanese Patent Laid-Open No. 2000-215516 discloses that cross erase can be suppressed by including at least a recording layer, a top protective layer, an intermediate layer and a reflecting layer in order from a light incident side and by defining characteristics of the materials of the intermediate and reflecting layers. However, since this method does not sufficiently select the material of the intermediate layer and selects a material having a low thermal conductivity, it is difficult to carry out rapid cooling, so that this method can not sufficiently reduce cross erase.
Thus, the thickness and heat conduction characteristics of the dielectric film between the metal reflecting film and the recording film are required to simultaneously eliminate the problems on the power sensitivity in recording, cross erase, recrystallization and erasing rate. However, conventional means can not simultaneously satisfy all of them.
SUMMARY OF THE INVENTION
It is therefore an object of the present invention to eliminate the aforementioned problems and to provide an optical recording medium which is capable of preventing cross erase and which has a high recording density.
According to a first aspect of the present invention, an optical recording medium includes: a reflecting film; a first transparent film provided on the reflecting film; a first semitransparent film provided on the first transparent film; a second transparent film provided on the first semitransparent film; a recording film provided on the second transparent film, the recording film being capable of reversibly changing an atomic arrangement; and a third transparent film provided on the recording film, wherein the first semitransparent film has a complex refractive index of n−ik satisfying relationships of 0<n<1 and 1<k, and a product of a thickness d (nm) of the first semitransparent film and an extinction coefficient k of the complex refractive index is d×k≦44.
Acc
Ashida Sumio
Ichihara Katsutaro
Nakamura Naomasa
Ohmachi Noritake
Yusu Keiichiro
Kabushiki Kaisha Toshiba
Mulvaney Elizabeth
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