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BACKGROUND OF THE INVENTION
The present invention relates to a phase change optical recording medium for recording and reproducing information by irradiating the medium with a light beam.
A phase change optical recording medium, in which recording and reproduction are carried out by irradiating the medium with a light beam, has advantages of large capacity, high-speed access and medium portability. As the recording density of the
medium increases, the field of application thereof is expected to be broadened. The operation of the phase change optical recording medium is as follows. In recording, an optical recording layer in a crystalline state is irradiated with a light beam of
a recording power level to heat the recording site up to a temperature above the melting point thereof, and then the irradiated site is rapidly cooled in a short period of time less than the crystallization time, thereby forming an amorphous recording
mark. In this case, overwriting can be performed by light intensity modulation. The recorded information is readout by utilizing the difference in the reflectance between the crystalline region and the amorphous recording mark.
In order to obtain a satisfactory overwrite performance (including .GAMMA. characteristics and overwrite repeatability), the phase change optical recording medium should preferably have a stacked structure which allows rapid heating and rapid
cooling. FIG. 1 shows a typical structure of a conventional phase change optical recording medium which is now in practical use. As shown in FIG. 1, on a substrate 1, there are formed a first interference layer (lower protective layer) 2 made from a
relatively thick dielectric having a thickness of 100 to 200 nm, a thin optical recording layer 3 having a thickness of 10 to 30 nm, a second interference layer (upper protective layer) 4 made from a relatively thin dielectric having a thickness of 10 to
40 nm and a reflective layer 5 made from a relatively thick and highly thermal conductive metal having a thickness of 50 to 100 nm.
As a technique which further enhances the recording density of the phase change optical recording medium, pulse width modulation recording (mark-edge detection) and land-groove (L-G) recording are known. The pulse width modulation recording
makes it possible to reduce bit pitch by recording data in the edges of recording marks. According to this method, the recording density can be about 1.5 times that of conventional mark position recording. In the land-groove recording, the depth of
groove is set to about 1/6 of the laser wavelength so as to reduce cross talk, which allows to record data on both land and groove. According to the L-G recording, the recording density can be about twice that of the conventional method in which data is
recorded only in either land or groove.
In the L-G recording, it is required to suppress cross erase, i.e., a phenomenon that the recording mark edges in adjacent tracks are erased. Since the optical recording medium of FIG. 1 has a stacked structure capable of rapid heating and
cooling, which effectively suppresses cross erase, there is little trouble in so far as the L-G recording is concerned. Meanwhile, in order to attain the pulse width modulation recording, it is required to minimize fluctuation in mark edge position.
However, since the structure of FIG. 1 is likely to cause fluctuation in mark edge position, the pulse width recording is hard to realize. The reason is explained as follows. As to the recording layer alone, the reflectance of an amorphous region is
smaller than that of a crystalline region. Besides, in the structure of FIG. 1, light passed through the recording layer is totally reflected by the uppermost reflective layer 5 and returned to the recording layer 3. Taking these conditions into
consideration, the effective absorbance (A*) of the recording layer, which is observed from the incident side of light beam, is greater in the amorphous region (Aa*) than in the crystalline region (Ac*). It is problematic to carry out overwriting under
the condition of Aa*>Ac*. That is, since the crystalline region is slowly heated up due to the smaller absorption and also requires a latent heat of melting, the region is hard to melt relative to the amorphous region. Therefore, the size of
recording mark to be newly formed differs depending on whether the overwritten site is crystalline or amorphous, which means the fluctuation in mark edge position becomes greater.
Accordingly, in order to attain the pulse width modulation recording by suppressing the fluctuation in mark edge position upon overwriting, it has been found desirable that the condition of Aa*.ltoreq.Ac* be met. Under the circumstances, optical
recording media having an improved stacked structure so as to satisfy the above condition have been proposed as follows.
(1) A stacked structure similar to that of FIG. 1 except that the uppermost reflective layer is replaced with a semitransparent layer: See, for example, ISOM/ODS-joint international conference proceeding, pp.71 (Th.3.5). This stacked structure
meets the condition of Aa*.ltoreq.Ac* by allowing a part of light to transmit through the semitransparent layer.
(2) A stacked structure in which a semi-transparent layer is inserted between the substrate and the first interference layer in addition to that of FIG. 1: See, for example, U.S. Pat. No. 5,431,978. This stacked structure realizes the
condition of Aa*.ltoreq.Ac* by utilizing interference of light.
In the above optical recording media, however, the semitransparent layer reduces heat radiation, which makes thermal response slow. As a result, overwrite repeatability is deteriorated due to increase in thermal load on the recording layer as
well as the land-groove recording characteristics is deteriorated due to increase in cross erase.
As stated above, it has been difficult for conventional optical recording media to meet excellent overwrite repeatability and land-groove recording as well as excellent pulse width modulation recording.
BRIEF SUMMARY OF THE INVENTION
An object of the present invention is to provide a phase change optical recording medium which represents superior overwrite repeatability and land-groove recording characteristics and which is suitable to pulse width modulation recording.
According to an aspect of the present invention, there is provided a phase change optical recording medium having a structure that a phase change optical recording layer which transits between two states of a crystalline state and an amorphous
state when irradiated with light and other layers are stacked, wherein the optical recording layer has a micro-structure that particles of optical recording material are dispersed in a matrix made from a dielectric, and wherein the optical recording
layer meets the condition of Ama<Amc with respect to Maxwell Garnett absorption, where Ama and Amc are the magnitude of Maxwell Garnett absorption of the optical recording layer in the case where the particles are amorphous and crystalline,
respectively, so that the optical recording layer meets the condition of Aa*.ltoreq.Ac* with respect to effective absorbance, where Aa* and Ac* are the effective absorbance of the optical recording layer in the case where the particles are amorphous and
crystalline, respectively.
According to another aspect of the present invention, there is provided a phase change optical recording medium having a structure that a phase change optical recording layer which transits between two states of a crystalline state and an
amorphous state when irradiated with light and other layers are stacked so that the optical recording layer meets the condition of Aa*.ltoreq.Ac* with respect to effective absorbance, where Aa* and Ac* are the effective absorbance of the optical
recording layer in the case where the optical recording material is amorphous and crystalline, respectively, wherein the optical recording layer has a microstructure that particles of optical recording material are dispersed in a matrix made from a
dielectric, and wherein the size of the particles are smaller than the size of light spot.
In the optical recording medium according to the present invention, the thermal conductivity of the matrix is preferably smaller than that of the optical recording material.
In the present invention, the "effective" absorbance means the absorbance which is actually measured when the optical recording layer in the optical recording medium having a stacked structure is viewed from the incident side of light beam.
Additional object and advantages of the invention will be set forth in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention. The object and advantages of the invention
may be realized and obtained by means of the instrumentalities and combinations particularly pointed out in the appended claims.
BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING
The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate presently preferred embodiments of the invention, and together with the general description given above and the detailed description of
the preferred embodiments given below, serve to explain the principles of the invention.
FIG. 1 is a sectional view of a conventional phase change optical recording medium;
FIG. 2 is a sectional view of the phase change optical recording medium according to Example 1;
FIG. 3 shows the wavelength dependency of the transmittance of the optical recording layer constituting the optical recording media of Example 1;
FIG. 4 illustrates thermal response characteristics of the optical recording medium of Example 1 and Comparative Examples 1a and 1b;
FIG. 5 is a sectional view of the optical recording media according to Examples 2a and 2b;
FIG. 6 is a sectional view of the optical recording media according to Examples 2c and 2d;
FIG. 7 is a sectional view of the optical recording media according to Comparative Examples 2a and 2d; and
FIG. 8 illustrates the relationship between the track width and .DELTA.C/N of the optical recording media according to Example 3 and Comparative Examples 3a and 3b.
DETAILED DESCRIPTION OF THE INVENTION
The present invention is described in detail below.
An embodiment of the phase change optical recording medium of the present invention has a stacked structure that a phase change optical recording layer and other layers such as an interference layer and reflective layer, and further the optical
recording layer has a particle dispersion type microstructure whose Maxwell Garnett absorption is adjusted.
The optical recording layer constituting the phase change optical recording medium according to the present invention has a structure that particles of phase change optical recording material are dispersed in a matrix made from a dielectric.
As the phase change optical recording material, used is a material which transits reversibly between a crystalline state and an amorphous state and whose optical properties differ between the two states. Examples of the material include GeSbTe,
InSbTe, AgInSbTe, SnSeTe, GeTeSn and InSeTlCo.
The material for the matrix made from a dielectric for making disperse the particles of the optical recording material may be selected from the group consisting of inorganic materials such as an oxide, a nitride, a carbide and a boride, and
organic polymers. Examples of the inorganic materials include Si--O, Al--O, Zr--O, Si--N, B--N and Si--C. These inorganic materials do not necessarily have a stoichiometric composition. Examples of the organic polymers include polytetrafluoroethylene
(PTFE) and hydrocarbon polymers.
Next, Maxwell Garnett absorption is explained below. It is known that, in a film comprising metal particles or island-like metal, absorption occurs at a specific wavelength which is determined by such parameters as the material, sizes and volume
content of the particles and optical constants of the matrix in which the particles are dispersed. This absorption is called Maxwell Garnett absorption. The present inventors have formed a phase change optical recording layer having a structure that
particles of optical recording material are dispersed in a dielectric matrix, and have examined the Maxwell Garnett absorption at operating wavelength of the optical recording medium. As a result, they have found that, if such parameters as the sizes
and volume content of the particles and optical constants of the matrix are properly set, the magnitude of Maxwell Garnett absorption can be controlled so as to meet the condition of Ama<Amc, where Ama is Maxwell Garnett absorption in the case where
the particles are amorphous and Amc is that in the case where the particles are crystalline. Further, they have found that, even if the media has a stacked structure suitable to rapid heating and cooling, if the Maxwell Garnett absorption is so adjusted
as to meet the condition of Ama<Amc, effective absorbance of the optical recording layer can be controlled so as to meet the condition of Aa*.ltoreq.Ac*, where Aa* is effective absorbance of the optical recording layer in the case where the particles
are amorphous and Ac* is that in the case where the particles are crystalline.
Accordingly, an optical recording medium having the above-described structure is most suitable to a high-density recording, because such a medium not only brings about superior overwrite repeatability and cross erase characteristics owing to the
stacked structure suitable to rapid heating and quenching but also realizes the pulse width modulation recording owing to the condition of Aa*.ltoreq.Ac*.
The theoretically required conditions to control the Maxwell Garnett absorption (Am) in the optical recording layer so as to meet the condition of Ama<Amc at the operating wavelength of the medium, can be obtained in the following way.
Suppose the case where on a substrate having a refractive index of n.sub.s, there is formed a particle dispersion film having a thickness d and an imaginary part of .epsilon..sub.2 * of a complex dielectric constant. The Maxwell Garnett
absorption Am to the incident light irradiated perpendicularly into the dispersion film is approximately given by the following equation (i), where no interfacial reflection is taken into consideration: ##EQU1##
Further, .epsilon..sub.2 * is given by the following equation (ii). ##EQU2##
In the above equation, Q is a volume content of the particles, which is given by Q=VNv where V is a volume of a particle and Nv is a density by number of particles in the dispersion film. .epsilon..sub.1 and .epsilon..sub.2 are a real part and
an imaginary part, respectively, of the complex dielectric constant of the optical recording material. .epsilon..sub.m is a dielectric constant of the matrix material for dispersing the particles. Since a transparent dielectric is basically used for
the matrix material, only the real part .epsilon..sub.m is considered. In the equation (ii), although it is assumed that the particles have a spherical shape, Am may be theoretically expressed by an equation even in the case where the particles are not
spherical by giving some modification to the equation (ii).
Since each of .epsilon..sub.1, .epsilon..sub.2 and .epsilon..sub.m is a function of wavelength, each of .epsilon..sub.2 * and Am is also a function of wavelength. Ama, which is the magnitude of the Maxwell Garnett absorption in the case where
the particles are amorphous, is obtained by substituting the real part .epsilon..sub.1a and imaginary part .epsilon..sub.2a of the complex dielectric constant of the amorphous region for .epsilon..sub.1 and .epsilon..sub.2, respectively. Meanwhile, Amc,
which is the magnitude of the Maxwell Garnett absorption in the case where the particles are crystalline, is obtained by substituting the real part .epsilon..sub.1c and imaginary part .epsilon..sub.2c of the complex dielectric constant of the crystalline
region for .epsilon..sub.1 and .epsilon..sub.2, respectively. Accordingly, by appropriately selecting the sizes and the density by number of the particles and the material for the matrix, it is possible to fulfill the requirement for Ama<Amc.
By taking into consideration the fact that the optical recording material is nonmagnetic, the complex dielectric constant .epsilon. can be linked to a refractive index n and an extinction coefficient k by the following equations.
where .epsilon. is a dielectric constant of the dispersion type optical recording layer, .epsilon..sub.0 is the dielectric constant of vacuum, .upsilon. is a wavenumber (.upsilon.=c/.lambda., where c is light velocity and .lambda. is a
wavelength), and .sigma. is an electric conductivity of the dispersion type optical recording layer.
To be more specific, the parameters of the dispersion type optical recording layer, required to meet the above-described conditions, are explained below in the case where GeSbTe is used as a phase change optical recording material. In the case
of GeSbTe, the optical constants in an amorphous state are given as n=4.36 and k=1.72, while the optical constants in a crystalline state are given as n=4.46 and k=4.00. Therefore, the requirement for Ama<Amc can be fulfilled, if the parameters are
set as follows: the refractive index of the matrix n=1.4-3.0; the size of the GeSbTe particles is 1-20 nm; and the volume content of the particles is 25-85 vol %. If the optical recording material and the matrix material are changed, the optimal volume
content and size of the particles will also be changed.
Another embodiment of the phase change optical recording medium of the present invention has a structure that a phase change optical recording layer and other layers such as an interference layer and a reflective layer are stacked so that the
condition of Aa*.ltoreq.Ac* is fulfilled in which a dispersion type optical recording layer is used.
In order to prevent the scattering of light by the particles of the layer, the size of the particles to be dispersed in a matrix of the optical recording layer are designed to be sufficiently smaller than the spot size of the laser beam (normally
in the order of submicrons) to be irradiated upon recording. Preferably, the size of the particles are in the range of 10 to 100 nm, more preferably 20 to 50 nm. The spacing between the particles, i.e., the thickness of the matrix present between the
particles, is preferably in the range of 1 to 10 nm. If the particle spacing is less than 1 nm, deterioration of the optical recording material by mass transfer is likely to occur. If the particle spacing is greater than 10 nm, a sufficient reflectance
cannot be obtained.
Examples of the optical recording medium having a stacked structure that fulfills the requirement for Aa*.ltoreq.Ac*, include: (1) a structure having a substrate, and a first interference layer, a dispersion type optical recording layer, a second
interference layer and a semitransparent layer formed in this order on the substrate; and (2) a structure having a substrate, and a semitransparent layer, a first interference layer, a dispersion type optical recording layer, a second interference layer
and a reflective layer formed in this order on the substrate.
In the present invention, it is preferable that the thermal conductivity of the matrix be lower than that of the optical recording material. This is for the purpose of diminishing the heat transfer in in-plane directions to reduce the cross
erase. The thermal conductivity of the matrix is preferably 0.5 W/mK or less. The practical range is 0.1 to 0.5 W/mK.
A preferred example of the matrix having a lower thermal conductivity is a porous inorganic material or an organic polymer. An organic polymer is particularly preferable, because many of the organic polymers have a thermal conductivity lower
than that of the optical recording material, and therefore the matrix material can be selected from a variety of species.
Examples of the matrix, which is made from a porous inorganic material, include oxides, nitrides, carbides, borides, sulfides and fluorides, each having fine pores of in a range of several to tens of angstroms in size. Specific examples are
Si--O, Al--O, Zr--O, Si--N, B--N and Si--C. Generally, these inorganic compounds in a bulk state have a thermal conductivity higher than that of an optical recording material. However, the thermal conductivity of these compounds in a porous state are
lower than that of the optical recording material, because of the presence of the fine pores. Such a porous material can be prepared by deposition in gas or by bias sputtering under a relatively high pressure of an inorganic compound.
The matrix made from an organic polymer can be obtained by plasma polymerization of a hydrocarbon or fluorocarbon gas, or by reactive sputtering or reactive deposition of carbon in a hydrogen or in a fluorine-based gas, or otherwise by sputtering
or deposition of polytetrafluoroethylene.
Other materials for use in the phase change optical recording medium according to the present invention are described below.
Examples of the materials for the substrate include polycarbonate and polymethyl methacrylate (PMMA). A groove for tracking guide is formed on the surface of the substrate. Various films are stacked onto the surface of the substrate on which
the groove is formed.
Examples of the materials for the first interference layer (lower protective layer) and the second interference layer (upper protective layer) include oxides, nitrides, carbides, borides, sulfides, fluorides and mixtures thereof. Typical
materials are ZnS--SiO.sub.2, Ta.sub.2 O.sub.5 and the like.
Examples of the materials for the semitransparent layer include a metal, such as Al, Au and Cu, and an alloy containing these elements which is formed into a thin film so that the translucency is exhibited. In addition, a material such as Si
which transmits light even at a thick film can also be used.
Examples of the materials for the reflective layer include a metal, such as Al, Au and Cu, and an alloy containing these elements which material is formed into a thick film so that the light transmission inhibited.
In the phase change optical recording medium according to the present invention, a counter substrate which is made from the same material as that for the substrate, may be bonded to the uppermost layer in order to prevent a bend of the substrate
and stabilize the recording and readout operations. As the bonding layer, for example, an ultraviolet light-curable resin may be used.
Note that, Jpn. Pat. Nos. 1,709,012 and 1,847,417 disclose a phase change optical recording layer having a structure that particles of optical recording material are dispersed in a oxide ceramic matrix. However, the main purpose of the
structure is to prevent the oxidation of the optical recording material and thereby to prolong the life of the medium. These patents make no reference to the Maxwell Garnett absorption. Naturally, unlike the description of the present invention, these
patents make no mention of selecting the size and volume content of the particles along with the optical constants of the matrix so that the relationship of the Maxwell Garnett absorption as specified in the present invention is fulfilled. In addition,
the optical recording media of the above-mentioned patents have a stacked structure which does not fulfill the requirement for Aa*.ltoreq.Ac*. Therefore, the effect of the present invention obtained by using a dispersion type optical recording layer for
a stacked structure which fulfills the requirement for Aa*.ltoreq.Ac*, is not obvious from the descriptions of the above-mentioned patents.
EXAMPLES
Example 1
FIG. 2 is a sectional view of the phase change optical recording medium according to Example 1. On a polycarbonate substrate 1, there are formed in succession, a 150 nm-thick first interference layer 2 made from ZnS--SiO.sub.2, a 20 nm-thick
phase change optical recording layer 3 having a microstructure that GeSbTe particles 32 are dispersed in a TiO.sub.2 matrix (refractive index n=2.2) 31, a 20 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 50 nm-thick reflective
layer 5 made from AlMo. The stacked structure enables rapid heating and cooling as in the case of a conventional medium having the structure shown in FIG. 1.
The phase change optical recording medium is manufactured in the following way. A groove for tracking guide is formed on the polycarbonate substrate. The depth of the groove is about 1/6 of the laser wavelength (680 nm) for recording and
readout so as to be suitable to land-groove recording. The polycarbonate substrate is subjected to dehydration, and then placed in a multi-chambered sputtering apparatus followed by evacuating the apparatus. Next, the predetermined materials are
sputtered in succession to form films on the substrate. The first interference layer 2 is formed by RF sputtering in a sputtering chamber provided with a Zn--SiO.sub.2 target. Then, the recording layer 3 is formed by binary RF bias cosputtering in a
sputtering chamber provided with a GeSbTe target and a Zn--SiO.sub.2 target. The second interference layer 4 is then formed by RF sputtering in a sputtering chamber provided with a Zn--SiO.sub.2 target. Finally, the reflective layer 5 is formed by DC
sputtering in a sputtering chamber provided with an AlMo target.
The GeSbTe particle content by volume of the recording layer 3 can be controlled by the power ratio applied to the targets at the time of the binary cosputtering. The particle size of the GeSbTe particles can be controlled by the bias power
applied to the substrate.
In this example, on the basis of the calculation according to the Maxwell Garnett absorption theory, the power ratio applied to targets and the bias power applied to the substrate are controlled so that the GeSbTe particle content by volume of
the recording layer 3 is set to be 71 vol % and the average particle size is set to be 15 nm.
In order to measure the transmittance of the recording layer, the recording layer alone is formed on a glass substrate by the same condition as described above. FIG. 3 shows the dependency of the transmittance (Tr) on wavelength (.lambda.). In
FIG. 3, the curve (a) refers to the transmittance of the as-deposited amorphous recording layer, while the curve (c) refers to the transmittance of the recording layer crystallized by heating the as-deposited recording layer.
In FIG. 3, the Maxwell Garnett absorption has occurred at the wavelength (.lambda..sub.0) at which the transmittance drops. .lambda..sub.0 is the laser wavelength at which the disk is actually operated. For example, the wavelength is nearly 650
nm for DVD having a capacity of about 5 GB for one side. Since the GeSbTe particle content by volume of the recording layer and the particle size of the GeSbTe particles are controlled in the above-described manner, the Maxwell Garnett absorption at
.lambda..sub.0 is controlled so that the value Ama in the case where the GeSbTe particles are in the amorphous state is smaller than the value Amc in the case where the GeSbTe particles are in a crystalline state.
In the wavelength range other than the wavelength range at which the Maxwell Garnett absorption is observed, the transmittance is kept at a nearly constant value such that the transmittance for an amorphous state is higher than that for a
crystalline state. This indicates the characteristics inherent to GeSbTe. As shown in FIG. 3, since the requirement for Ama<Amc is fulfilled, the requirement for Aa*.ltoreq.Ac* can be fulfilled in the stacked structure shown in FIG. 2.
Two prior art optical recording media (Comparative Examples 1a and 1b) are prepared in order to compare the characteristics with those of the optical recording medium of Example 1 shown in FIG. 2.
Comparative Example 1a corresponds to the optical recording medium having the structure shown in FIG. 1. That is, on a polycarbonate substrate 1, there are formed in succession, a 150 nm-thick first interference layer 2 made from ZnS--SiO.sub.2,
a 20 nm-thick optical recording layer 3 made from GeSbTe, a 20 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 50 nm-thick reflective layer 5 made from Au.
Comparative Example 1b is an optical recording medium having a semitransparent layer in place of the reflective layer of FIG. 1. That is, on a polycarbonate substrate 1, there are formed in succession, a 200 nm-thick first interference layer 2
made from ZnS--SiO.sub.2, a 10 nm-thick optical recording layer 3 made from GeSbTe, a 20 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 50 nm-thick semitransparent layer 5 made from Si. As the absorbance is adjusted by use of the
semitransparent layer, the requirement for Aa*.ltoreq.Ac* is fulfilled.
As in Example 1, the wavelength dependency of the transmittance of the optical recording layers of Comparative Examples 1a and 1b is examined. However, the Maxwell Garnett absorption is not observed and the transmittance is nearly constant for
both amorphous state and crystalline state. The relationship between the effective absorbance (Aa*) in the amorphous state and the effective absorbance (Ac*) in the crystalline state for each optical recording layer is Aa*>Ac* for Comparative Example
1a, and Aa*<Ac* for Comparative Example 1b.
The thermal response of optical recording media of Example 1 and Comparative Examples 1a and 1b is evaluated by numerical calculation. The thermal constants used for the calculation are measured by a optical AC current method. FIG. 4 shows the
dependency of temperature (T) of the recording layer on the time (t). The steeper, the more preferable the thermal response is, since the durability in repeated overwriting is improved and the cross erase is reduced. As is shown in FIG. 4, the medium
of Comparative Example 1a has the steepest thermal response. Although the medium of Example 1 is somewhat inferior to the medium of Comparative Example 1a in the steepness of thermal response, the thermal response of the medium of Example 1 is good.
These media are markedly superior to the medium of Comparative Example 1b.
Further, after the initial crystallization by means of a bulk eraser is carried out, the disk characteristics of the optical recording media of Example 1 and Comparative Examples 1a and 1b are evaluated in the following way. In this evaluation,
a testing apparatus provided with a semiconductor laser having a wavelength of 650 nm and an object lens having NA of 0.6 is used. In the test, the linear speed of the disk is changed in a rang from 5 to 30 m/s and the power for recording and readout is
optimized depending on the linear speed.
(1) High-density recording characteristics
After overwriting random patterns several times, the jitter (as a ratio to the window width) is measured.
(2) Cross erase characteristics
As to specific three tracks (groove/land/groove), the following test is conducted for evaluation. First, a signal is recorded on the central track and then the signal is readout to measure the C/N ratio. Next, after random patterns have been
overwritten several times on the two tracks beside the central track, the signal of the central track is again readout to measure the C/N ratio. In this way, the percentage reduction in C/N ratio is determined.
(3) Overwrite performance
Random patterns are repeatedly overwritten to determine the number of repeated overwriting at which the jitter exceeds 12.8% (corresponding to a bit error rate of 10.sup.-4).
These results are shown in Table 1.
TABLE 1 ______________________________________ Cross Number of Jitter Erase repeated (%) (dB) overwriting ______________________________________ Example 1 6 -0.5 10.sup.6 Comparative 12 -0.5 10.sup.6 example 1a Comparative 6 -1.5
10.sup.5 example 1b ______________________________________
The following conclusion can be drawn from Table 1. The disk of Comparative Example 1a has a high jitter and is inferior in the high-density recording characteristics, although it is superior in the cross erase characteristics and overwrite
performance owing to good thermal response. The disk of Comparative Example 1b is inferior in cross erase characteristics and exhibits an inferior overwrite performance due to slow thermal response, although it has a superior high-density recording
characteristic because its absorbance is properly controlled. In contrast with these disks, the disk of Example 1 is superior to these disks in any of the characteristics, namely, the high density recording, cross erase characteristics and overwrite
performance. This is because the disk of Example 1 fulfills the requirement for Aa*<Ac* with regard to the absorbance, while maintaining the steep thermal response.
Example 2
FIG. 5 is a sectional view of the phase change optical recording media according to Examples 2a and 2b. FIG. 6 is a sectional view of the phase change optical recording media according to Examples 2c and 2d. FIG. 7 is a sectional view of the
phase change optical recording media according to Comparative Examples 2a and 2b.
Each of these optical recording media comprises a polycarbonate substrate 1 and layers formed thereon in succession. The polycarbonate substrate is provided with a groove having a depth of about 1/6 of the laser wavelength (680 nm). The track
pitch is controlled within a range of 0.6 to 0.8 .mu.m.
The optical recording layer 3 has a microstructure that GeSbTe particles 32 are dispersed in a ZnS--SiO.sub.2 matrix 31 (dispersion film X), or GeSbTe particles 32 are dispersed in a SiN matrix 31 (dispersion film Y). These optical recording
layers are formed by co-sputtering the targets of the matrix material and the optical recording material.
The optical recording medium of FIG. 5 has a structure that on a polycarbonate substrate 1, there are formed in succession, a 90 nm-thick first interference layer 2 made from ZnS--SiO.sub.2, a 50 nm-thick dispersion type optical recording layer
3, a 120 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 10 nm-thick upper semitransparent layer 6 made from Au. In addition, a counter substrate 11 made from polycarbonate is bonded to the upper semitransparent layer 5 by means of
an adhesive layer 10.
The optical recording medium of FIG. 6 has a structure that on a polycarbonate substrate 1, there are formed in succession, a 10 nm-thick lower semitransparent layer 7 made from Au, a 140 nm-thick first interference layer 2 made from
ZnS--SiO.sub.2, a 20 nm-thick dispersion type optical recording layer 3, a 120 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 100 nm-thick reflective layer 5 made from an AlTi alloy. In addition, a counter substrate 11 made from
polycarbonate is bonded to the reflective layer 5 by means of an adhesive layer 10.
The optical recording medium of FIG. 7 has a structure that on a polycarbonate substrate 1, there are formed in succession, a 150 nm-thick first interference layer 2 made from ZnS--SiO.sub.2, a 20 nm-thick dispersion type optical recording layer
3, a 25 nm-thick second interference layer 4 made from ZnS--SiO.sub.2, and a 100 nm-thick reflective layer 5 from an AlTi alloy. In addition, a counter substrate 11 made from polycarbonate is bonded to the reflective layer 5 by means of an adhesive
layer 10.
The stacked structure of the optical recording medium of FIG. 7 does not fulfill the requirement for Aa*<Ac*. In the dispersion type optical recording layer of FIG. 7, the wavelength range at which Maxwell Garnett absorption is observed is
set at a wavelength range not containing an operating wavelength. Therefore, although the optical recording layer of FIG. 7 is of dispersion type, the effective absorption is under the condition of Aa*>Ac* at the operating wavelength.
Further, optical recording media of Comparative Examples 2c-2e having a similar stacked structures shown in FIGS. 5-7, respectively, but each of which has an optical recording layer composed of a GeSbTe continuous film.
First, the microstructure of the dispersion-type optical recording layer is observed under a high-resolution TEM. The GeSbTe particles are nearly spherical and have an average size in the range of 30.+-.10 nm by half width of the distribution.
The spacing between the nearest particles is about 1 nm. The GeSbTe particle content by volume of the optical recording layer is about 50%.
In comparison with the thermal conductivity of GeSbTe (about 0.6 W/mK) as the optical recording material, ZnS--SiO.sub.2 has a lower thermal conductivity and SiN has a higher thermal conductivity.
Using a thermal conductivity measuring apparatus by means of an optical AC current method, the thermal conductivity of the optical recording layer is measured. As a result, the thermal conductivity of GeSbTe particles/ZnS--SiO.sub.2 (dispersion
film X) is about 0.5 W/mK and that of GeSbTe particles/SiN (dispersion film Y) is a | | |
