JP2003067938A - Measuring method of characteristics data to multilevel optical storage-medium and multilevel optical storage- medium to which pattern for measuring the characteristics data is recorded - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a method for simply and accurately measuring the asymmetry of a multilevel optical storage medium. SOLUTION: A step which measures a light reflectivity to a first virtual record cell row S00 in which more than one virtual record cell S0 is consecutively formed, a step which measures the light reflectivity to a second virtual record cell row S77 in which more than one virtual record cell S7 is consecutively formed and a step which measures the light reflectivity to a third virtual record cell row S07 in which the virtual record cell S0 and the virtual record cell S7 are alternately arranged are provided. The values of the light reflectivity obtained from the first and second virtual record cell rows S00 and S77 are values under the condition that the accordance of an adjacent virtual record cell with the contents of the virtual record cell concerned is guaranteed, and the value of the light reflectivity obtained from the third virtual record cell row is a value under the condition that the difference of the adjacent virtual record cell from the contents of the virtual record cell concerned is guaranteed.

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring characteristic data for a multilevel optical recording medium capable of multilevel recording in one virtual recording cell, and more specifically,
The present invention relates to a method for measuring asymmetry for a multilevel optical recording medium. The present invention also relates to a multilevel optical recording medium having a characteristic data measurement pattern recorded thereon, and more particularly to a multilevel optical recording medium having an asymmetry measurement pattern recorded thereon.

[0002]

2. Description of the Related Art Conventionally, an optical recording medium typified by a CD and a DVD has been widely used as a recording medium for recording digital data. The data recording method is to record data to be recorded on a track. The method of modulating to the length of the pit along it is widely used.

When such a recording method is used, when reading data, a reproducing laser beam is irradiated along the track of the optical recording medium, and the presence or absence of pits is determined by detecting the reflected light. Further, at the time of writing data, a recording laser beam is irradiated along the track of the optical recording medium to form a pit having a predetermined length.

However, in recent years, there has been a demand for higher density recording on an optical recording medium, and a so-called "multilevel recording system" has been proposed as a method for realizing this. Unlike the above-mentioned conventional recording method, the multi-level recording method is a method of assigning one of a plurality of recording marks having different meanings to one virtual recording cell, and is used for reproduction when reading data. The type of the recording mark assigned to each virtual recording cell is determined by irradiating the laser beam along the track of the multilevel optical recording medium and detecting the reflected light. When writing data, a recording laser beam is irradiated along the tracks of the multilevel optical recording medium, and recording marks to be assigned are recorded in each virtual recording cell.

Virtual recording cells to which recording marks different from each other are different in light transmittance with respect to the reproducing laser beam. Therefore, at the time of writing data, by controlling the irradiation amount of the recording laser beam at a multi-level for each virtual recording cell,
The light transmittance is controlled in multiple levels for each virtual recording cell.

Here, the "light transmittance" means the ratio of the laser beam that has passed through the virtual recording cell to the reproducing laser beam that has been irradiated onto the virtual recording cell. Therefore, when reading data, the reproducing laser beam irradiated to the virtual recording cell passes through the virtual recording cell,
The intensity of the laser beam that is reflected by the reflective layer and then passes through the same virtual recording cell again and is emitted to the outside of the multi-level optical recording medium is detected, whereby the type of recording mark assigned to each virtual recording cell is detected. Is determined.

As is clear from the above, in order to record data with higher density on a multi-level optical recording medium, it is effective to control the light reflectance of each virtual recording cell in multiple stages. . For example, if the light reflectance of each virtual recording cell is controlled in four steps, the information stored in one virtual recording cell is 2 bits, but the light reflectance of each virtual recording cell is controlled in eight steps. Then, the information stored in one virtual recording cell has 3 bits. In order to control the light reflectance in multiple stages, the light reflectance of the virtual recording cell to which the recording mark with the highest light transmittance and the recording mark with the lowest light transmittance are assigned. Also, it is required that the difference from the light reflectance of the virtual recording cell, that is, the so-called dynamic range is sufficiently wide. Therefore, as the recording layer used for the multilevel optical recording medium, a material that can secure a sufficient dynamic range is selected.

On the other hand, as another method for recording data with higher density on a multilevel optical recording medium, there is a method of further reducing the physical area of each virtual recording cell. If the area of each virtual recording cell is reduced, the number of virtual recording cells included in one multi-level optical recording medium can be increased, which enables higher density recording.

[0009]

However, when the area of each virtual recording cell becomes smaller than the converging area of the reproducing laser beam, it becomes impossible to irradiate the reproducing laser beam only to a single virtual recording cell. . in this case,
The reproduction laser beam inevitably irradiates not only the virtual recording cell to be read but also other adjacent virtual recording cells. Therefore, the amount of reflected light is the recording mark assigned to the virtual recording cell to be read. Not only that, it is affected by the recording marks assigned to other adjacent virtual recording cells.

Therefore, even in the virtual recording cells to which the same recording mark is assigned, the amount of reflected light varies depending on the contents of the adjacent virtual recording cells.
Therefore, the amplitude of the detected reflected light amount changes depending on the contents of the virtual recording cells before and after, but in this case, if the center of the amplitude fluctuates greatly depending on the contents of the virtual recording cells before and after, accurate data reproduction is possible. It may run out.
Such a variation characteristic of the center of the amplitude is called "asymmetry", and it is necessary to measure this when developing and manufacturing a multilevel optical recording medium.

Therefore, it is an object of the present invention to provide a method for simply and accurately measuring the asymmetry of a multilevel optical recording medium.

Another object of the present invention is to provide a multi-level optical recording medium on which an asymmetry measurement pattern is recorded, which enables simple and accurate asymmetry measurement.

[0013]

The object of the present invention is to:
A method for measuring characteristic data for a multi-level optical recording medium capable of multi-level recording in one virtual recording cell, wherein a first virtual recording cell in which first information is recorded is continuously formed. A step of measuring the light reflectance of the virtual recording cell array, and a second step different from the first information.
Measuring a light reflectance with respect to a second virtual recording cell row in which a plurality of virtual recording cells in which the information is recorded are continuously formed, and a virtual recording cell in which the first information is recorded, Measuring a light reflectance with respect to a third virtual recording cell row in which the virtual recording cells in which the second information is recorded are alternately arranged.

According to the present invention, the values of the light reflectances obtained from the first and second virtual recording cell rows are guaranteed to match the contents of the adjacent virtual recording cells. And the value of the light reflectance obtained from the third virtual recording cell row is the value in the state in which it is guaranteed that the adjacent virtual recording cell is different from the content of the virtual recording cell. Become. This makes it possible to measure asymmetry of the multilevel optical recording medium accurately and easily.

In a preferred aspect of the present invention, the first information is information corresponding to a virtual recording cell having the highest light reflectance.

In a further preferred aspect of the present invention, the second information is information corresponding to a virtual recording cell having the lowest light reflectance.

The object of the present invention is also a multi-level optical recording medium capable of multi-level recording in one virtual recording cell, wherein a plurality of virtual recording cells in which the first information is recorded are continuously formed. The first virtual recording cell array, a second virtual recording cell array in which a plurality of virtual recording cells in which second information different from the first information is recorded are continuously formed, A multi-layer recorded with a characteristic data measurement pattern including at least a virtual recording cell in which information 1 is recorded and a third virtual recording cell row in which the virtual recording cells in which the second information is recorded are alternately arranged. Achieved by a level optical recording medium.

According to the present invention, since the characteristic data measuring pattern is recorded, the asymmetry can be measured accurately and easily by measuring the light reflectance using the characteristic data measuring pattern. Become.

In a preferred aspect of the present invention, the first information is information corresponding to a virtual recording cell having the highest light reflectance.

In a further preferred aspect of the present invention, the second information is information corresponding to a virtual recording cell having the lowest light reflectance.

In a further preferred aspect of the present invention, the characteristic data measuring pattern is recorded in the lead-in area.

In a further preferred aspect of the present invention, at least two virtual recording cell columns selected from the first virtual recording cell column, the second virtual recording cell column and the third virtual recording cell column. Are continuously formed.

[0023]

DETAILED DESCRIPTION OF THE INVENTION Referring to the accompanying drawings,
A preferred embodiment of the present invention will be described in detail.

FIG. 1 is a cutaway perspective view showing the structure of a multilevel optical recording medium 1 (hereinafter, also referred to as "optical recording medium 1").

The optical recording medium 1 is a CD-R type optical recording medium (write-once type optical recording medium) here, and as shown in FIG. 1, the substrate 11, the recording layer 12, the reflection film 13 and the protective layer. It is configured with 14. The substrate 11 is formed in a disk shape using a transparent resin as a base material. A groove 11a for guiding a laser beam and a land 11b are spirally formed on one surface (upper surface in FIG. 1) of the substrate 11 from the vicinity of the central portion toward the outer edge portion. The recording layer 12 includes a cyanine dye, a merocyanine dye,
An organic dye such as a methine dye and its derivative, a benzenethiol metal complex, a phthalocyanine dye, a naphthalocyanine dye, and an azo dye is formed by coating the organic dye so as to cover the groove 11a and the land 11b. The recording layer 12 is decomposed and deteriorated by being irradiated with a recording laser beam by a recording device, and its light transmittance changes according to the irradiation amount of the laser beam. The reflective film 13 is a thin film layer for reflecting the reproducing laser beam that has passed through the substrate 11 and the recording layer 12 at the time of reproducing recorded data recorded on the optical recording medium 1, and is mainly made of metal such as gold or silver. The raw material is formed on the recording layer 12 by, for example, sputtering. The protective layer 14 is a layer that protects the reflective film 13 and the recording layer 12, and is formed so as to cover the outer surface of the reflective film 13.

Next, regarding the recording principle of the optical recording medium 1,
A description will be given with reference to the drawings.

In this optical recording medium 1, as shown in FIG. 1, the groove 11a is formed along the rotation direction (circumferential direction) thereof.
.. are virtually defined, and virtual recording cells S, S ... Are defined as recording units.

FIG. 2 is a conceptual diagram conceptually showing the recording marks Ma to Mg recorded on the optical recording medium 1. As shown in FIG. 2, the length of the virtual recording cell S in the direction along the groove 11a is defined to be shorter than the focused beam diameter (beam waist diameter) D. It should be noted that each virtual recording cell S is just a virtual cell assumed on the optical recording / reproducing apparatus side, and each virtual recording cell S is as shown in FIG.
The partition that defines the boundary of the optical recording medium 1 does not exist.

In this case, the irradiation time of the recording laser beam emitted from the pickup of the recording device (ie,
By controlling the irradiation amount of the laser beam) in multiple stages according to the value of the recording data, as shown in FIG.
Recording marks Ma to Mg (hereinafter, also referred to as “recording marks M” when not distinguished) having different degrees of decomposition and alteration of (mainly organic dye) are formed in the virtual recording cell S.
In the same figure, the degree of decomposition and alteration is conceptually shown by the size of the recording mark M. Further, when the recording data is recorded by the recording laser beam, the recording laser beam is irradiated while rotating the optical recording medium 1, so that the recording mark M becomes an ellipse having a length corresponding to the irradiation time. .

Therefore, when performing multi-level recording on the optical recording medium 1, the light reflectance when the virtual recording cell S is irradiated with the reproducing laser beam is, for example, 7 steps (8 steps including the unrecorded portion). Recording marks Ma to
Degradation and alteration degree of each Mg (change amount of light transmittance)
Stipulate. In this case, the light reflectance increases as the degree of decomposition and alteration of the recording layer 12 decreases. Therefore, the virtual recording cell S to which the recording mark M is not assigned has the characteristic of maximum light reflectance, and the virtual recording cell S to which the smallest recording mark Ma is assigned is the largest light reflectance of the recording marks M. Of the recording marks Mb to M
The light reflectance decreases in the order of the virtual recording cells S to which f is assigned, and the virtual recording cell S to which the largest recording mark Mg is assigned has the characteristic of the minimum light reflectance. Therefore, by controlling the irradiation amount of the laser beam and appropriately setting the area ratio of the decomposed and deteriorated portion (that is, the light transmittance of the recording layer 12), the recording marks Ma to which the light reflectance becomes 7 steps can be obtained.
It becomes possible to form Mg.

Next, the characteristics of the organic dye used in the recording layer 12 of the optical recording medium 1 will be described with reference to the drawings.

The organic dye used in the recording layer 12 generally has the characteristic that the degree of decomposition and alteration increases as the irradiation time (irradiation amount) of the recording laser beam increases. On the other hand, the change in the light reflectance at this time is not linear with the irradiation time (irradiation amount) of the recording laser beam. Also, the irradiation time (irradiation amount) of the recording laser beam
Degradation deterioration due to, the degree is gentle for a while from the start of irradiation, the degree becomes steep and linear after the lapse of a predetermined time, then the degree becomes gentle again, after a certain irradiation time Indicates that the degree hardly increases.

Further, the light transmittance of the organic dye which has not been decomposed and modified, and the light transmission of the organic dye which has been decomposed and modified to the greatest extent (the organic dye which has been decomposed and modified until the degree of decomposition and modification hardly increases). The rate and the amount of change in light transmittance depending on the degree of decomposition and alteration also vary depending on the material of the organic dye used. Therefore, for example, when five kinds of optical recording media 1 in which the recording layers 12 are formed of different organic dyes are produced, each recording layer 12 of each optical recording medium 1 is manufactured.
The absolute light reflectances at are different from each other. Here, the “absolute light reflectance” means the optical reflectance of each optical recording medium 1 in the case where the value of the light reflectance of a disk body having a smooth surface coated with a thin film such as gold by sputtering is 100%. It means the light reflectance in the unrecorded portion (unrecorded virtual recording cell S).

FIG. 3 is a characteristic diagram showing the relative light reflectance characteristics of the optical recording medium 1 using various organic dyes.

The characteristics of the relative light reflectance in each recording layer 12 of each optical recording medium 1 also differ from each other, as shown by the characteristics C1 to C5 in FIG. As shown in the figure, the above-mentioned degree of decomposition and alteration contributes to the slope of the curves of the characteristics C1 to C5. Here, the "relative light reflectance" means the corresponding optical recording when the value of the absolute light reflectance of the unrecorded portion of each optical recording medium 1 (that is, the unrecorded virtual recording cell S) is 100%. It means the light reflectance of each recording portion of the medium 1 (that is, the recorded virtual recording cell S).

Further, due to the fact that the absolute light reflectance and the relative light reflectance differ for each organic dye, the relative dynamic range (D07), asymmetry (Asymm07), and B. E. Various characteristics such as R (bit error rate) are also different. further,
These various characteristics differ not only according to the material of the organic dye but also according to various parameters such as the coating thickness of the organic dye, the structure of the groove 11a (depth or width or shape of the groove) and the material of the reflective film 13. Here, the "relative dynamic range (D07)" means the value of the absolute light reflectance of the unrecorded portion of each optical recording medium 1 (that is, the unrecorded virtual recording cell S) is I0a, and the largest recording mark Mg is When the value of the absolute light reflectance of the assigned virtual recording cell S is I7a, it is defined by (I0a-I7a) * 100 / I0a (1).

Here, the absolute light reflectance I0a is a value obtained under the condition that it has the largest value, and the absolute light reflectance I7a is obtained under the condition that it has the smallest value. Value is used.
The absolute reflectance obtained from the virtual recording cell S having the same contents varies depending on the conditions for the following reason.

That is, in the multilevel optical recording medium 1, as described above, the groove 11a of the virtual recording cell S is formed.
Since the length along the direction is defined to be shorter than the focused beam diameter (beam waist diameter) D, it is not possible to irradiate a single virtual recording cell S with the reproducing laser beam. The reproduction laser beam is also irradiated to other adjacent virtual recording cells S. Therefore, the absolute light reflectance of the reproducing laser beam is affected by the recording mark assigned to another adjacent virtual recording cell S. That is, the absolute light reflectance obtained from each virtual recording cell S differs depending on what kind of recording mark is assigned to the adjacent virtual recording cell S.

Since the multilevel recording is possible only when the light reflectance of the optical recording medium 1 is accurately controlled in multiple stages, the absolute light reflection of the unrecorded virtual recording cell S having the highest light reflectance is achieved. The rate is rather large (for example, 40% to 80
%), And the virtual recording cell S having the largest absolute light reflectance
(Virtual recording cell S to which the recording mark Ma is assigned)
If the difference in light reflectance from the smallest virtual recording cell S (virtual recording cell S to which the recording mark Mg is assigned) is not large to some extent, it becomes difficult to reproduce the recording data recorded in multi-level. From this viewpoint, the relative dynamic range (D07) is preferably 50% or more.

On the other hand, "Asymmetry (Asymm0
7) ”means a virtual recording cell S having the highest light reflectance (unrecorded virtual recording cell S) and a virtual recording cell S having the lowest light reflectance (virtual recording cell S to which a recording mark Mg is assigned). The value of the absolute light reflectance of the unrecorded virtual recording cell S obtained under the condition that the reflectance difference (amplitude) of No. 1 is minimized is I0b, and the recording mark Mg obtained under the same condition is assigned. When the absolute light reflectance of the virtual recording cell S is I7b,

[0041]

[Equation 1] Is defined by

Such an asymmetry (Asymm0
7) is reflection of the virtual recording cell S having the highest light reflectance (unrecorded virtual recording cell S) and the virtual recording cell S having the lowest light reflectance (virtual recording cell S to which the recording mark Mg is assigned) The pattern in which the difference in the ratio (amplitude) is the largest, the virtual recording cell S (the unrecorded virtual recording cell S) having the largest light reflectance and the virtual recording cell S (the recording mark Mg having the smallest light reflectance) It is possible to perform measurement by forming patterns such that the difference (amplitude) in reflectance from the assigned virtual recording cell S) is minimized and irradiating these patterns with a reproducing laser beam.

FIG. 4 shows an asymmetry measurement pattern 20.
It is a conceptual diagram which shows notionally the virtual recording cell row in which was formed.

As shown in FIG. 4, the asymmetry measurement pattern 20 has ten consecutive unrecorded virtual recording cell rows S00 and ten consecutive virtual recording cell rows S77 to which the ten recording marks Mg are allocated. And a virtual recording cell column S07 in which four unrecorded virtual recording cells S0 and four virtual recording cells S7 to which recording marks Mg are assigned are alternately arranged. Although not particularly limited,
The lead-in area is preferable as the position where the asymmetry measurement pattern 20 is formed. The lead-in area is an area that is first read when the optical recording medium 1 is loaded in the recording / reproducing apparatus. In the optical recording medium 1, in addition to the maximum light reflectance information and the minimum light reflectance information, the optical recording medium is recorded. Information indicating that the medium 1 is a multi-level optical recording medium (hereinafter, also referred to as “medium specifying information”) and an unrecorded portion of the recording mark M are recorded or recorded by, for example, 7-step multi-level recording. Various information such as information (hereinafter, also referred to as “recorded data stage information”) indicating that the information is recorded is recorded.

In the asymmetry measurement pattern 20 shown in FIG. 4, the virtual recording cell array S0 is arranged from the upstream side.
0, the virtual recording cell row S77, and the virtual recording cell row S07 are arranged in this order, but the arrangement order is not particularly limited.

In the measurement of asymmetry (Asymm07), such an asymmetry measurement pattern 20 is used.
A reproducing laser beam is irradiated to the absolute recording medium, and the absolute light reflectance of the cells included in the virtual recording cell column S00, the absolute light reflectance of the cells included in the virtual recording cell column S77, and the virtual recording cell column S07 Absolute light reflectance of the virtual recording cell S0 and the virtual recording cell S included in the virtual recording cell column S07.
7 and the absolute light reflectance of each of the cells included in the virtual recording cell sequence S00 is I0a, and the absolute light reflectance of the cells included in the virtual recording cell sequence S77 is I0a.
7a, the absolute light reflectance of the virtual recording cell S0 included in the virtual recording cell row S07 is I0b, and the virtual recording cell row S
The absolute light reflectance of the virtual recording cell S7 included in
As b, the asymmetry is calculated by substituting these into the equations (1) and (2).

Here, as the absolute light reflectance I0a, the first virtual recording cell S00 in the virtual recording cell row S00 is used.
The absolute light reflectance obtained from the virtual recording cells S other than -start and the last virtual recording cell S00-end is used. The absolute light reflectance I7a is the virtual recording cell row S7.
Among the seven, the absolute light reflectance obtained from the virtual recording cells S other than the first virtual recording cell S77-start and the last virtual recording cell S77-end is used. Further, as the absolute light reflectance I0b, the absolute light reflectance obtained from the virtual recording cells S0 other than the first virtual recording cell S07-start and the last virtual recording cell S07-end in the virtual recording cell row S07. Used, absolute light reflectance I7
b is the first virtual recording cell S07-start and the last virtual recording cell S of the virtual recording cell sequence S07.
The absolute light reflectance obtained from the virtual recording cell S7 other than 07-end is used.

Here, the virtual recording cell S07-start
The virtual recording cell S07-end may be the virtual recording cell S0 or S7. FIG. 4 shows an example in which the virtual recording cell S07-start is the virtual recording cell S0 and the virtual recording cell S07-end is the virtual recording cell S7.

As a result, it is possible to obtain the absolute light reflectance I0a under the condition of the largest value and the absolute light reflectance I7a under the condition of the smallest value. D07)
And a virtual recording cell S having the highest light reflectance (unrecorded virtual recording cell S) and a virtual recording cell S having the lowest light reflectance (virtual recording cell S to which a recording mark Mg is assigned). The absolute light reflectance I0b of the unrecorded virtual recording cell S under the condition that the difference (amplitude) in reflectance between the recording mark Mg and the recording mark Mg
Absolute light reflectance I7b of the virtual recording cell S to which is assigned
Can be obtained, and asymmetry (Asymm07) can be obtained by further using these.

As described above, according to the asymmetry (Asymmm07) measurement using the asymmetry measurement pattern 20, the absolute light reflectances I0a and I7 satisfying the respective conditions are obtained.
Since a, I0b, and I7b can be easily obtained, it becomes possible to easily measure asymmetry (Asymm07).

Next, the relationship between the asymmetry (Asymm07) and various characteristics of the optical recording medium 1 will be described.
The optical recording medium 1 used for the measurement was a groove 11
The depth of a is 200 nm and the width of the groove 11a is 7
20 nm, the optical recording medium 1 using a phthalocyanine dye as the recording film 12 is used, and the asymmetry (Asymm) is used.
The above-mentioned method was used for the measurement of 07).

FIG. 5 shows the asymmetry (Asymm07).
6 is a graph showing the relationship between the symbol error rate (SER) and the symbol error rate (SER).

As shown in FIG. 5, the symbol error rate (SER) is 0 when the asymmetry (Asymm07) is 0.
Low values are obtained in the region close to%. In general,
Since the symbol error rate (SER) is required to be 0.04 or less, in consideration of this, the asymmetry (Asymm07) of the optical recording medium 1 is about −20.
% To about 20% is preferred.

FIG. 6 shows the asymmetry (Asymm07).
6 is a graph showing the relationship between the bit error rate (BER) and the bit error rate (BER).

As shown in FIG. 6, the bit error rate (BER) is 0% for asymmetry (Asymm07).
Low values are obtained in the region close to. Generally, the bit error rate (BER) is required to be 1 × 10 ⁻⁴ or less, and in consideration of this, the asymmetry (Asymm07) of the optical recording medium 1 is about −15.
% To about 10% is preferred.

Next, an optical recording / reproducing apparatus 40 for recording recording data on the optical recording medium 1 and reproducing the recording data will be described.

FIG. 7 is a block diagram schematically showing the structure of the optical recording / reproducing device 40.

As shown in FIG. 7, the optical recording / reproducing apparatus 4
Reference numeral 0 is a so-called CD-R recorder, which includes a spindle servo 41, a spindle motor 42, a pickup 43,
A focus tracking servo 44, a feed servo 45 and a controller 46 are provided. Spindle motor 42
Is controlled by the spindle servo 41 to rotate the optical recording medium 1 under the condition of constant linear velocity. Under the control of the control device 46, the pickup 43 drives a laser light source (both not shown) by a laser driver to irradiate the optical recording medium 1 with a recording laser beam or a reproducing laser beam. As a result, the virtual recording cell S
The recording mark M is recorded with respect to, and the electric signal is output from the virtual recording cell S according to the level of the reflected laser. In this case, at the time of recording the recording data, the laser driver of the pickup 43 follows the control of the control device 46 and, according to the content of the recording data to be recorded, the irradiation amount of the laser beam with which one virtual recording cell S is irradiated. (The number of laser pulses and / or irradiation power, pulse height, etc.) is adjusted. As a method of adjusting the irradiation amount of the laser beam, in addition to the adjusting method by the laser driver, an optical modulator is arranged on the optical path of the laser beam, and the control device 46 drives and controls the optical modulator. It can also be adjusted.

The pickup 43 is provided with an objective lens and a half mirror (neither is shown), and a recording or reproducing laser beam is recorded on the recording layer 12 of the optical recording medium 1.
Focus on. Specifically, the objective lens is subjected to focus tracking control by the focus tracking servo 44, whereby the recording or reproducing laser beam is focused on the recording layer 12 of the optical recording medium 1.
The pickup 43 is reciprocated by a feed servo 45 between the inner peripheral side and the outer peripheral side along the diameter direction of the optical recording medium 1. The control device 46 controls the drive of the spindle servo 41, the pickup 43, the focus tracking servo 44, and the feed servo 45, and at the same time, records the recording data recorded on the recording layer 12 based on the electrical signal output from the pickup 43. Decipher.

As described above, according to this embodiment, since the asymmetry measuring pattern 20 is used, the asymmetry (Asymm07) can be easily measured.

The present invention is not limited to the above embodiments, and various modifications can be made within the scope of the invention described in the claims, and these are also included in the scope of the present invention. It goes without saying that it is a thing.

For example, in the above embodiment, the asymmetry measuring pattern 20 has ten consecutive unrecorded virtual recording cell rows S00 and ten consecutive recording marks Mg assigned virtual recording cell rows S77. However, the number of virtual recording cells S forming the unrecorded virtual recording cell row S00 and the number of virtual recording cells S forming the virtual recording cell row S77 to which the recording mark Mg is assigned are 10 The number is not limited and may be another number. Similarly, in the above embodiment, the virtual recording cell in which the unrecorded four virtual recording cells S0 and the four virtual recording cells S7 to which the recording marks Mg are allocated are alternately arranged in the asymmetry measurement pattern 20. Although the column S07 is included, the number of unrecorded virtual recording cells S0 forming the virtual recording cell column S07 and the number of virtual recording cells S7 to which the recording mark Mg is assigned are not limited to four, and other It can be a number.

However, as described above, the first virtual recording cell S
00-start, S77-start and S07-s
start and the last virtual recording cells S00-end, S7
7-end and S07-end are not suitable for absolute light reflectance measurement and asymmetry measurement, the number of virtual recording cells S forming the virtual recording cell sequence S00 and the virtual recording cell sequence S77 The number of recording cells S needs to be at least three, and the virtual recording cell row S07
The number of virtual recording cells S forming the above is required to be at least four. On the other hand, if the number of virtual recording cells S forming the virtual recording cell row S00, the virtual recording cell row S77, and the virtual recording cell row S07 is too large, the number of virtual recording cells available for recording information decreases. Therefore, it is preferable to set the number of virtual recording cells S constituting these virtual recording cell rows S00, S77, S07 to 50 or less. Furthermore, the number of virtual recording cells S forming the virtual recording cell row S00 does not have to match the number of virtual recording cells S forming the virtual recording cell row S77, and these may be different from each other. Absent.

Further, in the above embodiment, the unrecorded virtual recording cell sequence S00, the virtual recording cell sequence S77 to which the recording mark Mg is assigned, the unrecorded virtual recording cell S0 and the recording mark Mg are assigned. The asymmetry measurement pattern 20 is formed by the virtual recording cell array S07 in which the virtual recording cells S7 are alternately arranged.
The asymmetry measurement pattern is not limited to this, and the asymmetry measurement pattern may be configured by a plurality of virtual recording cell rows made of other combinations. For example, an unrecorded virtual recording cell column S00, a virtual recording cell column S44 to which the recording mark Md is assigned, and an unrecorded virtual recording cell S0 and a virtual recording cell S4 to which the recording mark Md are assigned are alternately arranged. The asymmetry measurement pattern may be configured by the virtual recording cell sequence S04, and the virtual recording cell sequence S11 to which the recording mark Ma is assigned, the virtual recording cell sequence S66 to which the recording mark Mf is assigned, and the recording mark Ma are Virtual recording cell column S in which virtual recording cells S1 assigned and virtual recording cells S6 assigned recording marks Mf are alternately arranged
16 may form an asymmetry measurement pattern. When the former asymmetry measurement pattern is used, the asymmetry (Asymmm04) between the absolute light reflectance of the unrecorded virtual recording cell S and the absolute light reflectance of the virtual recording cell S to which the recording mark Md is assigned is calculated. When the latter pattern for asymmetry measurement is used, the virtual recording cell S to which the recording mark Ma is assigned and the absolute light reflectance of the virtual recording cell S to which the recording mark Mf is assigned can be measured. The asymmetry (Asymm16) in the interval can be accurately measured.

Further, in the above embodiment, the three virtual recording cell arrays S00, S77 and S07 which form the asymmetry measuring pattern 20 are continuously formed, but these virtual recording cell arrays S00, S77 and S07 are formed.
Other virtual recording cells may exist between and.

In the above embodiment, the recording layer 1
Although the example in which the organic dye is adopted as 2 is described, the multilevel optical recording medium in the present invention is not limited to this, and an organic dye or an inorganic material other than the above is used for the recording layer 1.
It can be applied to the multilevel optical recording medium used in
It can also be applied to a multilevel optical recording medium for multilevel recording using a phase change recording layer or the like.

Further, in the above embodiment, the example in which the optical recording medium 1 is configured as a CD-R type optical recording medium is shown, but the present invention is not limited to this, and other optical recording is possible. It is generally applied to a medium, and is not limited to a disk-shaped rotating body.

Further, in the above embodiment, the optical recording medium 1 is configured such that the laser beam for recording and reproducing is irradiated from the substrate 11 side. However, the reflective layer, the recording layer and the protective layer are sequentially provided on the substrate. It can also be applied to an optical recording medium that is laminated and has a structure in which a recording and reproducing laser beam is irradiated from the protective layer side.

Further, in the above-described embodiment, the recording marks Ma to Mg of seven stages having different degrees of decomposition and alteration from each other are recorded in the virtual recording cell to store 3-bit information in one virtual recording cell. However, the number of recording steps is not limited to this, and any number of steps may be used as long as one virtual recording cell can store information exceeding 1 bit.

[0070]

As described above, according to the present invention, a method for easily and accurately measuring asymmetry of a multilevel optical recording medium is provided. Further, according to the present invention, there is provided a multilevel optical recording medium on which an asymmetry measurement pattern is recorded, which enables simple and accurate asymmetry measurement.

[Brief description of drawings]

FIG. 1 is a cutaway perspective view showing a configuration of a multilevel optical recording medium 1.

FIG. 2 is recording marks Ma to M recorded on an optical recording medium 1.
It is a conceptual diagram which shows g conceptually.

FIG. 3 is a characteristic diagram showing relative light reflectance characteristics of the optical recording medium 1 using various organic dyes.

FIG. 4 is a conceptual diagram conceptually showing a virtual recording cell row in which an asymmetry measurement pattern 20 is formed.

FIG. 5 is a graph showing the relationship between asymmetry (Asymm07) and symbol error rate (SER).

FIG. 6 is a graph showing the relationship between asymmetry (Asymm07) and bit error rate (BER).

FIG. 7 is a block diagram schematically showing a configuration of an optical recording / reproducing device 40.

[Explanation of symbols]

1 Multi-level optical recording medium 11 board 11a groove 11b land 12 recording layers 13 Reflective film 14 Protective layer 20 Asymmetry measurement patterns 40 Optical recording / reproducing apparatus 41 Spindle servo 42 spindle motor 43 pickup 44 Focus tracking servo 45 feed servo 46 Control device

   ─────────────────────────────────────────────────── ─── Continued front page    (72) Inventor Shuji Tsukamoto             1-13-1, Nihonbashi, Chuo-ku, Tokyo             -In DC Inc. (72) Inventor Takashi Dorai             1-13-1, Nihonbashi, Chuo-ku, Tokyo             -In DC Inc. (72) Inventor Yutaka Taya             1-13-1, Nihonbashi, Chuo-ku, Tokyo             -In DC Inc. (72) Inventor Motohiro Inoue             1-13-1, Nihonbashi, Chuo-ku, Tokyo             -In DC Inc. F term (reference) 5D090 AA01 BB03 BB20 CC04 DD03                       EE11 GG11 HH01

Claims (8)

[Claims] 1. A method of measuring characteristic data for a multilevel optical recording medium capable of multilevel recording in one virtual recording cell, wherein a plurality of virtual recording cells in which first information is recorded are continuously formed. Measuring a light reflectance of the first virtual recording cell array, and a plurality of virtual recording cells continuously recording second information different from the first information. Measuring the light reflectance of the second virtual recording cell array, and a second virtual recording cell in which the first recording information-recording virtual recording cell and the second recording information-recording virtual recording cell are alternately arranged. 3. A method of measuring characteristic data, which comprises a step of measuring a light reflectance with respect to the virtual recording cell array of 3. 2. The characteristic data measuring method according to claim 1, wherein the first information is information corresponding to a virtual recording cell having the highest light reflectance. 3. The characteristic data measuring method according to claim 1, wherein the second information is information corresponding to a virtual recording cell having the lowest light reflectance. 4. A multi-level optical recording medium capable of multi-level recording in one virtual recording cell, wherein a first virtual recording cell in which a plurality of virtual recording cells in which first information is recorded is continuously formed. The recording cell row and the second information different from the first information
Second virtual recording cell row in which a plurality of virtual recording cells in which the above information is recorded are continuously formed, a virtual recording cell in which the first information is recorded and a virtual recording cell in which the second information is recorded. A multi-level optical recording medium on which a characteristic data measurement pattern is recorded, which comprises at least a third virtual recording cell array in which recording cells are alternately arranged. 5. The multilevel optical recording medium according to claim 4, wherein the first information is information corresponding to a virtual recording cell having the highest light reflectance. 6. The multilevel optical recording medium according to claim 4 or 5, wherein the second information is information corresponding to a virtual recording cell having the lowest light reflectance. 7. The pattern for measuring characteristic data is recorded in a lead-in area.
7. The multilevel optical recording medium according to any one of items 1 to 6. 8. At least two virtual recording cell columns selected from the first virtual recording cell column, the second virtual recording cell column and the third virtual recording cell column are continuously formed. 8. The one of claims 4 to 7 characterized in that
The multilevel optical recording medium according to the item.