JP2009080929A - Measurement method and evaluation method - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To reduce interlayer crosstalk in an optical recording medium including three or more information recording layers, especially interlayer crosstalk between information recording layers not adjacent to each other. <P>SOLUTION: The optical recording medium is provided with: a substrate 11; a protective layer 19; an L0 layer 20, an L1 layer 30 and an L2 layer 40 which are disposed between the protective layer 19 and the substrate 11; a transparent intermediate layer 12 disposed between the L0 layer 20 and the L1 layer 30; and a transparent intermediate layer L3 disposed between the L1 30 and the L2 layer 40. A thickness Da of the transparent intermediate layer 12 is different from a thickness Db of the transparent intermediate layer 13. Thus, when data is reproduced from the L0 layer 20, a beam spot of a laser beam L' reflected from the L1 layer 30 is not focused on the L2 layer 40, and hence interlayer crosstalk from the L2 layer 40 to the L0 layer 20 is effectively reduced. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

The present invention relates to an evaluation method of the measurement method and an optical recording medium to measure the magnitude of the interlayer crosstalk of the optical recording medium member (optical recording medium having three or more information recording layers that are the product layer).

  Conventionally, optical recording media represented by CDs and DVDs are widely used as recording media for recording digital data. The recording capacity required for such an optical recording medium increases year by year, and various proposals have been made to achieve this. As one of the methods, a method in which an information recording layer included in an optical recording medium has a two-layer structure has been proposed, and has been put to practical use in DVD-Video and DVD-ROM, which are read-only optical recording media. Such a read-only optical recording medium has a structure in which pits formed on the substrate surface serve as an information recording layer, and such a substrate is laminated via a transparent intermediate layer. Therefore, if a structure in which three or more information recording layers are stacked and a transparent intermediate layer is interposed between adjacent information recording layers, the storage capacity of the optical recording medium can be further increased.

  However, in an optical recording medium having three or more information recording layers, crosstalk (interlayer crosstalk) between information recording layers becomes more prominent than the optical recording medium having a two-layer structure that is currently in practical use. . Such problems can be reduced to some extent by increasing the thickness of the transparent intermediate layer provided between the information recording layers, but in order to ensure compatibility with optical recording media that are currently in practical use. The thickness of the transparent intermediate layer cannot be increased without limit. For this reason, as the number of information recording layers increases, the thickness of the transparent intermediate layer has to be set thinner, so that an optical recording medium including three or more information recording layers, particularly an optical recording including four or more information recording layers. In the medium, the influence of interlayer crosstalk becomes very significant.

  In addition, according to the study by the present inventors, it has been found that interlayer crosstalk does not occur only between information recording layers adjacent to each other but remarkably occurs between information recording layers not adjacent to each other depending on conditions.

Therefore, an object of the present invention is to provide an optical recording medium having three or more information recording layers and effectively reducing the interlayer crosstalk, and a method for measuring the size of the interlayer crosstalk and a method for evaluating the optical recording medium. Is to provide .

Another object of the present invention is to measure the size of interlayer crosstalk for providing an optical recording medium having three or more information recording layers and effectively reducing interlayer crosstalk between non-adjacent information recording layers. And a method for evaluating an optical recording medium .

Still another object of the present invention is an optical recording medium having three or more information recording layers, which is compatible with optical recording media currently in practical use by suppressing the thickness of the transparent intermediate layer. It is to provide a method for measuring the size of interlayer crosstalk and a method for evaluating an optical recording medium, in order to provide an optical recording medium in which interlayer crosstalk is effectively reduced.

The measurement method according to the present invention includes a substrate constituting one surface, a protective layer constituting the other surface, three or more information recording layers provided between the substrate and the protective layer, and each of the information This is a measurement method for measuring the size of interlayer crosstalk generated during data reproduction processing on a predetermined information recording layer for an optical recording medium provided with a plurality of transparent intermediate layers provided between the recording layers. Recording data on the information recording layer other than the predetermined information recording layer, and measuring the size of the interlayer crosstalk based on a reproduction signal obtained by the reproduction processing on the predetermined information recording layer. It is characterized by.

The measuring method according to the present invention is characterized in that the magnitude of the interlayer crosstalk is measured based on the reproduction signal obtained by the reproduction processing on the predetermined information recording layer in an unrecorded state.

The measurement method according to the present invention is characterized in that the magnitude of the interlayer crosstalk is measured in a state where the data is recorded on all the information recording layers except the predetermined information recording layer.

The measuring method according to the present invention is characterized in that a C / N ratio of the reproduction signal is measured as the magnitude of the interlayer crosstalk.

The measurement method according to the present invention is characterized in that an 8T signal in a 1,7RLL modulation system is recorded as the data.

According to these measurement methods, the size of interlayer crosstalk can be suitably measured for an optical recording medium having three or more information recording layers.

The evaluation method according to the present invention is characterized in that the optical recording medium is evaluated based on the magnitude of the interlayer crosstalk measured according to any one of the measurement methods described above. According to this evaluation method, an optical recording medium having three or more information recording layers can be suitably evaluated.

The evaluation method according to the present invention includes a first information recording layer as the information recording layer, and a surface on the side that becomes the light incident surface of the one and the other surfaces as viewed from the first information recording layer. The second information recording layer close to the second information recording layer and the third information recording layer close to the light incident surface as viewed from the second information recording layer, and as the transparent intermediate layer, the first information recording layer A first transparent intermediate layer provided between the information recording layer and the second information recording layer; and a second transparent layer provided between the second information recording layer and the third information recording layer. Two transparent intermediate layers, the first transparent intermediate layer is thicker than the second transparent intermediate layer, and the thickness of the second transparent intermediate layer is 100%, Before the difference between the thickness of the first transparent intermediate layer and the thickness of the second transparent intermediate layer is 5% to 100% And evaluating the optical recording medium based on the first information recording layer in the optical recording medium to the magnitude of the interlayer crosstalk measured as the predetermined information recording layer.

Effect of layer crosstalk is most pronounced in the first information recording layer, or less, the second information recording layer, it is common to the order of the third information recording layer. Therefore, according to this measuring method, as possible it can be suitably evaluated optical recording medium based on the magnitude of the most interlayer crosstalk interlayer crosstalk sensitive about the first information recording layer. In addition, it is possible to favorably evaluate an optical recording medium having compatibility with an optical recording medium that is currently in practical use .

  Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the accompanying drawings.

FIG. 1A is a cutaway perspective view showing the appearance of the optical recording medium 10 according to the present invention, and FIG. 1B is an enlarged partial sectional view of a portion A shown in FIG.

As shown in FIG. 1 , the optical recording medium 10 is a disc-shaped optical recording medium having an outer diameter of about 120 mm and a thickness of about 1.2 mm, and includes a support substrate 11, transparent intermediate layers 12 and 13, and light transmission. A layer (protective layer) 19, an L0 layer 20 provided between the support substrate 11 and the transparent intermediate layer 12, an L1 layer 30 provided between the transparent intermediate layer 12 and the transparent intermediate layer 13, and transparent An L2 layer 40 provided between the intermediate layer 13 and the light transmission layer 19 is provided.

  The L0 layer 20 constitutes the information recording layer farthest from the light incident surface 19a. Hereinafter, the L1 layer 30 and the L2 layer 40 are arranged in this order toward the light incident surface 19a. The L2 layer 40 is arranged in the light incident surface 19a. Is the closest information recording layer. Therefore, when recording and / or reproducing data on the L0 layer 20, it is necessary to irradiate the laser beam L via the L1 layer 30 and the L2 layer 40, and data recording is performed on the L1 layer 30. When performing reproduction, it is necessary to irradiate the laser beam L through the L2 layer 40. In the present specification, the information recording layer relatively close to the light incident surface 19a is referred to as an “upper layer” information recording layer, and the information recording layer relatively close to the support substrate 11 is referred to as a “lower layer” information recording layer. Sometimes.

  The support substrate 11 is a disk-shaped substrate having a thickness of about 1.1 mm that is used to ensure the thickness required for the optical recording medium 10 (about 1.2 mm). Grooves or pit rows (both not shown) are formed in a spiral shape from the outer edge toward the outer edge. Various materials can be used as the material of the support substrate 11, and for example, glass, ceramics, or resin can be used. Among these, a resin is preferable from the viewpoint of ease of molding. Examples of such resins include polycarbonate resins, olefin resins, acrylic resins, epoxy resins, polystyrene resins, polyethylene resins, polypropylene resins, silicone resins, fluorine-based resins, ABS resins, and urethane resins. Of these, polycarbonate resins and olefin resins are particularly preferable from the viewpoint of processability. However, since the support substrate 11 does not become an optical path of the laser beam L, it is not necessary to have high light transmittance.

The transparent intermediate layer 12 serves to separate the L0 layer 20 and the L1 layer 30 from each other with a sufficient physical and optical distance, and grooves or pit rows (both not shown) are provided on the surface thereof. Yes. The transparent intermediate layer 13 serves to separate the L1 layer 30 and the L2 layer 40 from each other with a sufficient physical and optical distance, and a groove or a pit row (both not shown) is provided on the surface thereof. ing. Although it does not specifically limit as a material of the transparent intermediate | middle layers 12 and 13, It is preferable to use an ultraviolet curable acrylic resin. Since the transparent intermediate layers 12 and 13 serve as an optical path of the laser beam L when data is recorded / reproduced with respect to the lower information recording layer, the transparent intermediate layers 12 and 13 need to have sufficiently high light transmittance. Although details will be described later , in the optical recording medium 10, the relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is:
Da ≠ Db
Is set to

  The light transmission layer 19 serves as an optical path of the laser beam L and constitutes a light incident surface 19a. The thickness of the light transmission layer 19 is preferably set to 30 μm to 200 μm. The material of the light transmission layer 19 is not particularly limited, but it is preferable to use an ultraviolet curable acrylic resin as in the transparent intermediate layers 12 and 13. As described above, since the light transmission layer 19 serves as an optical path of the laser beam L, it is necessary to have a sufficiently high light transmittance.

  The L0 layer 20, the L1 layer 30, and the L2 layer 40 are information recording layers for holding data, respectively, and may be read-only information recording layers or information recording layers that can be written by the user. Also good. When the information recording layer is writable by the user, it may be a write-once information recording layer or a rewritable information recording layer. Furthermore, the L0 layer 20, the L1 layer 30, and the L2 layer 40 may be the same type of information recording layers, or some or all of them may be different types of information recording layers. For example, the L0 layer 20 may be a read-only information recording layer, the L1 layer 30 and the L2 layer 40 may be write-once information recording layers, or the L0 layer 20 may be a read-only information recording layer. The layer 30 may be a write-once information recording layer, and the L2 layer 40 may be a rewritable information recording layer.

  When the L0 layer 20, the L1 layer 30, and / or the L2 layer 40 is a read-only information recording layer, a spiral pit row is formed on the surface of the support substrate 11, the transparent intermediate layer 12, and / or the transparent intermediate layer 13. As a result, information is retained. In this case, it is preferable to increase the reflectance with respect to the laser beam L irradiated during reproduction by providing a reflective film on the information recording layer, but high light transmittance is required for the L1 layer 30 and the L2 layer 40. Therefore, when the L1 layer 30 and / or the L2 layer 40 is used as a read-only information recording layer, it is necessary to set the thickness of the corresponding reflective film very thin.

  When the L0 layer 20, the L1 layer 30, and / or the L2 layer 40 is an information recording layer that can be written by the user, the surface of the support substrate 11, the transparent intermediate layer 12, and / or the transparent intermediate layer 13 is spiral. The information recording layer is provided with a recording film capable of forming a recording mark. Such a groove serves as a guide track for the laser beam L at the time of data recording. Irradiation of the intensity-modulated laser beam L along the groove makes the recording film irreversible (in the case of a write-once type) or A reversible (rewritable) recording mark is formed.

  When data is reproduced from the optical recording medium 10 having such a structure, the laser beam L is irradiated from the incident surface 19a side, and the focal point thereof is set to one of the L0 layer 20, the L1 layer 30, and the L2 layer 40. It is done.

  FIG. 2 is a diagram schematically showing the optical path of the laser beam L when data is reproduced from the optical recording medium 10. FIG. 2A shows a case where data recorded in the L2 layer 40 is reproduced, and FIG. When data recorded on the L1 layer 30 is reproduced, (c) shows a case where data recorded on the L0 layer 20 is reproduced.

  As shown in FIG. 2A, when data recorded on the L2 layer 40 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L2 layer 40. As a result, the amount of reflected light of the laser beam L mainly depends on the reflectivity in the beam spot of the L2 layer 40, that is, the presence or absence of a recording mark, and is recorded in the L2 layer 40 by detecting the change. Data can be played back. At this time, since the beam spot of the laser beam L is also formed in the L0 layer 20 and the L1 layer 30, the reflectance distribution (recording mark arrangement state) in the L0 layer 20 and the L1 layer 30 is the reflected light amount of the laser beam L. Will be affected. That is, data recorded in the L0 layer 20 and the L1 layer 30 leaks into the reproduction signal from the L2 layer 40. In this specification, such leakage of data from an information recording layer that is not a reproduction target is referred to as “interlayer crosstalk”.

  Interlayer crosstalk becomes more conspicuous as the beam spot of the laser beam L formed on the information recording layer that is not the target of reproduction becomes smaller, and therefore adjacent to the reproduction of data recorded on the L2 layer 40. Medium interlayer crosstalk occurs between the L1 layer 30 and weak interlayer crosstalk between the L0 layer 20 and the L1 layer 30.

  As shown in FIG. 2B, when data recorded in the L1 layer 30 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L1 layer 30. At this time, since the beam spot of the laser beam L is also formed on the L0 layer 20 and the L2 layer 40, interlayer crosstalk occurs between these information recording layers. In this case, since both the L0 layer 20 and the L2 layer 40 are adjacent to the L1 layer 30, the data recorded in the L1 layer 30 is intermediate between the L0 layer 20 and the L2 layer 40. Inter-layer crosstalk occurs.

  Further, as shown in FIG. 2C, when data recorded on the L0 layer 20 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L0 layer 20. At this time, since the beam spot of the laser beam L is also formed in the L1 layer 30 and the L2 layer 40, interlayer crosstalk occurs between these information recording layers. Further, in this case, the laser beam L ′ reflected by the L1 layer 30 is focused at or near the L2 layer 40. Although the laser beam L ′ is light reflected by the L1 layer 30 and has a considerably lower intensity than the laser beam L, the beam spot on the L2 layer 40 is the laser beam L (from the light incident surface 19a to the support substrate 11 side). Compared to the beam spot of the transmitted light toward), the aperture is very small. Therefore, the laser beam L ′ reflected by the L1 layer 30 causes significant interlayer crosstalk from the L2 layer 40 to the L0 layer 20. Therefore, when data recorded on the L0 layer 20 is reproduced, moderate interlayer crosstalk occurs between the adjacent L1 layers 30, and large interlayer crosstalk occurs between the L2 layers 40. .

FIG. 3 is a diagram summarizing the degree of interlayer crosstalk given from one information recording layer to another information recording layer in the optical recording medium 10. Referring to FIG. 3, it is the L0 layer 20 that is most strongly influenced by the interlayer crosstalk, and then the L1 layer 30 and the L2 layer 40 is the least affected by the interlayer crosstalk. I know that there is.

  Next, a structure capable of reducing such interlayer crosstalk will be examined.

  First, a method for reducing the interlayer crosstalk, which is the largest interlayer crosstalk, from the L2 layer 40 to the L0 layer 20 will be considered.

  The reason why the interlayer crosstalk from the L2 layer 40 to the L0 layer 20 is very large is that the beam spot of the laser beam L ′ reflected by the L1 layer 30 is very small on the L2 layer 40 as described above. . In order to reduce this influence, the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 are made different (Da ≠ Db), thereby the beam spot of the laser beam L ′ on the L2 layer 40. Should be expanded.

  FIG. 4 is a diagram schematically showing the optical path of the laser beam L (L ′) when the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 are different. When Da> Db is set, (b) shows a case where Da <Db is set. As shown in FIG. 4A, when Da> Db is set, the focal point of the laser beam L ′ reflected by the L1 layer 30 is viewed from the L2 layer 40 on the light incident surface 19a side (light transmission layer 19). ), The beam spot of the laser beam L ′ on the L2 layer 40 is enlarged. As shown in FIG. 4B, when Da <Db is set, the focal point of the laser beam L ′ reflected by the L1 layer 30 is the support substrate 11 side (transparent intermediate layer 13) when viewed from the L2 layer 40. ), The beam spot of the laser beam L ′ on the L2 layer 40 is also enlarged. Thereby, interlayer crosstalk from the L2 layer 40 to the L0 layer 20 due to the laser beam L ′ can be reduced.

  Here, in order to sufficiently reduce the interlayer crosstalk from the L2 layer 40 to the L0 layer 20 by the laser beam L ′, the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is It is preferably 5% or more (value when the thickness of the thinner transparent intermediate layer is 100%, the same applies hereinafter), and more preferably 10% or more. However, when increasing these differences, considering that the interlayer crosstalk between adjacent information recording layers increases when the transparent intermediate layer 12 or the transparent intermediate layer 13 is thinned, one of the transparent intermediate layer 12 and the transparent intermediate layer 13 It is necessary to increase the thickness. In this case, if one of the transparent intermediate layer 12 and the transparent intermediate layer 13 is excessively thick, it may be difficult to ensure compatibility with currently used optical recording media. In this case, the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is preferably 100% or less, and more preferably 70% or less. That is, the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is preferably 5% to 100%, and more preferably 10% to 70%.

  Next, it is examined which of the transparent intermediate layer 12 and the transparent intermediate layer 13 should be set thick.

  Which of the transparent intermediate layer 12 and the transparent intermediate layer 13 should be set thicker can be determined based on whether the interlayer crosstalk received by the L0 layer 20 or the interlayer crosstalk received by the L2 layer 40 is significant. . That is, if the total layer thickness (Da + Db) of the transparent intermediate layer 12 and the transparent intermediate layer 13 is fixed, the thickness Db of the transparent intermediate layer 13 should be set larger than the thickness Da of the transparent intermediate layer 12. The interlayer crosstalk from the L0 layer 20 to the L1 layer 30 increases and the interlayer crosstalk from the L2 layer 40 to the L1 layer 30 decreases. Conversely, as the thickness Db of the transparent intermediate layer 13 is set smaller than the thickness Da of the transparent intermediate layer 12, the interlayer crosstalk from the L0 layer 20 to the L1 layer 30 decreases, and from the L2 layer 40 Interlayer crosstalk to the L1 layer 30 increases. That is, as long as the total layer thickness (Da + Db) of the transparent intermediate layer 12 and the transparent intermediate layer 13 is constant, it can be said that the overall interlayer crosstalk received by the L1 layer 30 does not change so much.

  On the other hand, the interlayer crosstalk received by the L0 layer 20 by the laser beam L (excluding the reflected laser beam L ′) sets the thickness Da of the transparent intermediate layer 12 larger than the thickness Db of the transparent intermediate layer 13. The interlayer crosstalk received by the L2 layer 40 decreases as the thickness Db of the transparent intermediate layer 13 is set larger than the thickness Da of the transparent intermediate layer 12. That is, when the total layer thickness (Da + Db) of the transparent intermediate layer 12 and the transparent intermediate layer 13 is constant, the interlayer crosstalk received by the L0 layer 20 and the interlayer crosstalk received by the L2 layer 40 are the thicknesses of the transparent intermediate layer 12. There is a trade-off relationship between Da and the thickness Db of the transparent intermediate layer 13. Therefore, the determination that gives priority to the one where the influence of the interlayer crosstalk is essentially remarkable may be made.

  Considering that the interlayer crosstalk received by the L0 layer 20 is more significant than the interlayer crosstalk received by the L2 layer 40 due to the influence of the laser beam L ′, the thickness of the transparent intermediate layer 13 is considered. It can be said that the thickness Da of the transparent intermediate layer 12 is preferably thicker (Da> Db) than the thickness Db. Therefore, if the relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is set in this way, this is effectively suppressed in the L0 layer 20 that is most susceptible to interlayer crosstalk. It becomes possible to do.

As described above, the optical recording medium 10 includes three information recording layers (L0 layer 20, L1 layer 30, and L2 layer 40), and the thickness of the transparent intermediate layer 12 that separates the L0 layer 20 and the L1 layer 30 from each other. The relationship between Da and the thickness Db of the transparent intermediate layer 13 that separates the L1 layer 30 and the L2 layer 40 is Da ≠ Db
Therefore, interlayer crosstalk from the L2 layer 40 to the L0 layer 20 due to the laser beam L ′ reflected by the L1 layer 30 can be reduced.

The relationship between Da and Db is expressed as Da> Db.
If it is set to, this can be effectively suppressed in the L0 layer 20 that is most susceptible to interlayer crosstalk.

The optical recording medium having three laminated information recording layers has been described above as an example. However, the optical recording medium in the present invention is not limited to this, and the optical recording medium having four or more information recording layers is used. also Ru included. In this case, the thickness of any of the transparent intermediate layer adjacent well if they differ from each other, it is more preferable that the thickness of all adjacent transparent intermediate layer are different from each other. Will now be described preferred not form state of the optical recording medium body having four information recording layers laminated.

FIG. 5 is a partial cross-sectional view of the optical recording medium 100 . The external appearance of the optical recording medium 100 is a disk-shaped optical recording medium having an outer diameter of about 120 mm and a thickness of about 1.2 mm, similar to the optical recording medium 10 shown in FIG. The state which expanded the A section is shown. Note that among the constituent elements included in the optical recording medium 100, the same constituent elements as those of the optical recording medium 10 described above are denoted by the same reference numerals, and redundant description is omitted.

As shown in FIG. 5 , the optical recording medium 100 is provided between the support substrate 11, the transparent intermediate layers 12 to 14, the light transmission layer (protective layer) 19, and the support substrate 11 and the transparent intermediate layer 12. L0 layer 20, L1 layer 30 provided between transparent intermediate layer 12 and transparent intermediate layer 13, L2 layer 40 provided between transparent intermediate layer 13 and transparent intermediate layer 14, and transparent intermediate layer And an L3 layer 50 provided between the layer 14 and the light transmission layer 19. That is , the optical recording medium 100 has a configuration in which the transparent intermediate layer 14 and the L3 layer 50 are added to the optical recording medium 10 described above, and the L3 layer 50 is the information recording layer closest to the light incident surface 19a. Is configured.

  Therefore, when recording / reproducing data on the L0 layer 20, it is necessary to irradiate the laser beam L through the L1 layer 30, the L2 layer 40, and the L3 layer 50. When recording / reproducing is performed, it is necessary to irradiate the laser beam L through the L2 layer 40 and the L3 layer 50. When recording / reproducing data on the L2 layer 40, the L3 layer 50 is required. It is necessary to irradiate the laser beam L via

The transparent intermediate layer 14 serves to separate the L2 layer 40 and the L3 layer 50 from each other with a sufficient physical and optical distance, and a groove or a pit row (both not shown) is provided on the surface thereof. Yes. As the material of the transparent intermediate layer 14, the same material as that of the transparent intermediate layers 12 and 13 may be used . In the optical recording medium 100, regarding the relationship between the thickness Da of the transparent intermediate layer 12, the thickness Db of the transparent intermediate layer 13, and the thickness Dc of the transparent intermediate layer 14,
Da ≠ Db and Db ≠ Dc
It is preferable that at least one of them is satisfied and both of them are satisfied.

  Similarly to the L0 layer 20, the L1 layer 30, and the L2 layer 40, the L3 layer 50 may be a read-only information recording layer or a user-writable information recording layer. Further, the L0 layer 20, the L1 layer 30, the L2 layer 40, and the L3 layer 50 may be the same type of information recording layers, or some or all of them may be different types of information recording layers. Absent.

  When reproducing data from the optical recording medium 100 having such a structure, the laser beam L is irradiated from the incident surface 19a side, and the focal point is any one of the L0 layer 20, the L1 layer 30, the L2 layer 40, and the L3 layer 50. Can be combined into one.

  FIG. 6 is a diagram schematically showing the optical path of the laser beam L when reproducing data from the optical recording medium 100. FIG. 6A shows a case where data recorded on the L3 layer 50 is reproduced, and FIG. When reproducing the data recorded on the L2 layer 40, (c) shows the case of reproducing the data recorded on the L1 layer 30, and (d) shows the case of reproducing the data recorded on the L0 layer 20. .

  As shown in FIG. 6A, when data recorded on the L3 layer 50 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L3 layer 50. Since the L beam spot is also formed in other information recording layers, interlayer crosstalk occurs between these other information recording layers. As described above, the interlayer crosstalk becomes more noticeable as the beam spot of the laser beam L formed on the information recording layer that is not the target of reproduction becomes smaller, so that the data recorded in the L3 layer 50 is reproduced. Means that a moderate interlayer crosstalk occurs between the adjacent L2 layers 40, a weak interlayer crosstalk occurs between the L1 layer 30 and a slight interlayer crosstalk between the L0 layer 20 and the L2 layer 40. Become.

  As shown in FIG. 6B, when data recorded on the L2 layer 40 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L2 layer 40. Since the beam spot of the beam L is also formed in other information recording layers, interlayer crosstalk occurs between these other information recording layers. In this case, since both the L1 layer 30 and the L3 layer 50 are adjacent to the L2 layer 40, the data recorded in the L2 layer 40 is reproduced between the adjacent L1 layer 30 and L3 layer 50. A moderate interlayer crosstalk occurs, and a weak interlayer crosstalk with the L0 layer 20 occurs.

  Further, as shown in FIG. 6C, when data recorded in the L1 layer 30 is reproduced, focus control is performed so that the beam spot of the laser beam L is substantially minimized in the L1 layer 30. Since the beam spot of the laser beam L is also formed in other information recording layers, interlayer crosstalk occurs between these other information recording layers. Further, in this case, since the laser beam L ′ reflected by the L2 layer 40 is focused at or near the L3 layer 50, the beam spot of the laser beam L ′ on the L3 layer 50 is very small. For this reason, the laser beam L ′ reflected by the L2 layer 40 causes significant interlayer crosstalk from the L3 layer 50 to the L1 layer 30. Therefore, when data recorded on the L1 layer 30 is reproduced, a moderate interlayer crosstalk occurs between the adjacent L0 layer 20 and the L2 layer 40, and a large interlayer crosstalk occurs between the L3 layer 50 and the L3 layer 50. Will occur.

  Further, as shown in FIG. 6D, when data recorded in the L0 layer 20 is reproduced, focus control is performed so that the beam spot of the laser beam L in the L0 layer 20 is substantially minimized. Since the beam spot of the laser beam L is also formed in other information recording layers, interlayer crosstalk occurs between these other information recording layers. Further, in this case, since the laser beam L ′ reflected by the L1 layer 30 is focused at or near the L2 layer 40, the beam spot of the laser beam L ′ on the L2 layer 40 is very small. Therefore, the laser beam L ′ reflected by the L1 layer 30 causes significant interlayer crosstalk from the L2 layer 40 to the L0 layer 20. On the other hand, although the laser beam L is also reflected by the L2 layer 40, the focal point of the reflected laser beam L ′ is relatively far from the L3 layer 50. The impact is minor. Therefore, when data recorded in the L0 layer 20 is reproduced, a moderate interlayer crosstalk occurs between the adjacent L1 layers 30 and a large interlayer crosstalk occurs between the L2 layer 40 and the L3 layer 50. There will be a slight interlayer crosstalk between the two.

FIG. 7 is a table summarizing the degree of interlayer crosstalk given from one information recording layer to another information recording layer in the optical recording medium 100. Referring to FIG. 7, it can be understood that the L1 layer 30 is most strongly influenced by the interlayer crosstalk as a whole, and the L0 layer 20, the L2 layer 40, and the L3 layer 50 are in this order.

  In order to reduce such interlayer crosstalk, the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 are different from each other (Da ≠ Db) as described above. By expanding the beam spot of the laser beam L ′ formed on the L2 layer 40 at the time of data reproduction, the thickness Db of the transparent intermediate layer 13 and the thickness Dc of the transparent intermediate layer 14 are made different (Db ≠ Dc) The beam spot of the laser beam L ′ formed on the L3 layer 50 at the time of data reproduction from the L1 layer 30 may be enlarged.

  FIG. 8 is a diagram schematically showing the optical path of the laser beam L (L ′) when the thickness Db of the transparent intermediate layer 13 and the thickness Dc of the transparent intermediate layer 14 are different. When Db> Dc is set, (b) shows a case where Db <Dc is set. The optical path of the laser beam L (L ′) when the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 are different is as shown in FIG.

  As shown in FIG. 8A, when Db> Dc is set, the focal point of the laser beam L ′ reflected by the L2 layer 40 is viewed from the L3 layer 50 on the light incident surface 19a side (light transmission layer 19). ), The beam spot of the laser beam L ′ on the L3 layer 50 is enlarged. Also, as shown in FIG. 8B, when Db <Dc is set, the focal point of the laser beam L ′ reflected by the L2 layer 40 is the support substrate 11 side (transparent intermediate layer) when viewed from the L3 layer 50. 14), the beam spot of the laser beam L ′ on the L3 layer 50 is also enlarged. Thereby, interlayer crosstalk from the L3 layer 50 to the L1 layer 30 due to the laser beam L ′ can be reduced.

Further, while effectively suppressing interlayer crosstalk caused by the laser beam L (excluding the reflected laser beam L ′), the thicknesses of the transparent intermediate layers 12 to 14 are set to Da ≠ Db and Db ≠ Dc. To set it up,
Da <Db and Db> Dc
It is preferable to set to. According to this, it becomes possible to effectively suppress this in the L1 layer 30 and the L2 layer 40 that are strongly influenced by the interlayer crosstalk caused by the laser beam L (excluding the reflected laser beam L ′). In addition, since it is possible to suppress an increase in the total layer thickness (Da + Db + Dc) of the transparent intermediate layers 12 to 14, there is an advantage that it is easy to ensure compatibility with optical recording media that are currently in practical use.

In this case, the magnitude relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Dc of the transparent intermediate layer 14 is not particularly limited, and any of Da> Dc, Da <Dc, and Da = Dc may be used. Considering that the influence of the interlayer crosstalk is more remarkable in the L0 layer 20 than in the L3 layer 50, the relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Dc of the transparent intermediate layer 14 is
Da> Dc
It is preferable to set to.

Therefore, the relationship of the thicknesses (Da, Db, Dc) of the transparent intermediate layers 12 to 14 is
Db>Da> Dc
It is most preferable to set to. With this setting, it is possible to most effectively suppress the interlayer crosstalk generated between the information recording layers and to suppress the increase in the total layer thickness (Da + Db + Dc) of the transparent intermediate layers 12 to 14. Therefore, it is possible to sufficiently ensure compatibility with the optical recording medium currently in practical use.

Incidentally, Oite the optical recording medium having a 5 or more information recording layers, it is preferable that any three of the thickness of the transparent intermediate layer successive set so as to satisfy the above relationship. Further, in an optical recording medium having five or more information recording layers, as shown in FIG. 9, when data is reproduced from the lower information recording layer (L0 layer 20), four reflected laser beams L ′ are present. Since there is a risk of focusing in the upper information recording layer (L4 layer 60) or the vicinity thereof which is far away, not only the thickness of two adjacent transparent intermediate layers is set to be different from each other, but also any four continuous four Of the transparent intermediate layers (transparent intermediate layers 12 to 15), the total thickness (Da + Db) of two transparent intermediate layers (transparent intermediate layers 12, 13) positioned on the support substrate 11 side and the light incident surface 19a side More preferably, the total thickness (Dc + Dd) of the two transparent intermediate layers (transparent intermediate layers 14 and 15) is set to be different from each other.

Optical recording medium of the present invention is not limited to the above state-like, and various modifications are possible within the scope of the invention described in the claims, measurement methods and evaluation methods thereof and the target Needless to say, these are also included within the scope of the present invention.

For example, the optical recording medium 10, 100, the laser beam L is incident from the thin light transmissive layer 19 side of the layer thickness, is a so-called next-generation optical recording medium, an optical recording medium according to the present invention this The present invention is not limited to such a next-generation type optical recording medium, and is also applicable to a measurement method and an evaluation method for a type of optical recording medium in which a laser beam L is incident from the substrate side such as a DVD. Is possible. In the DVD type optical recording medium, the element corresponding to the support substrate 11 is a light transmissive substrate having a thickness of about 0.6 mm, and the element corresponding to the light transmissive layer 19 is a dummy substrate having a thickness of about 0.6 mm. Therefore, in the present invention, the “substrate” means a light-transmitting substrate when the surface is a light incident surface like a DVD type optical recording medium, and the optical recording medium 10 When the surface does not become a light incident surface, it means a support substrate. Similarly, in the present invention, the “protective layer” means a light transmission layer when the surface is a light incident surface as in the optical recording medium 10, and as in a DVD type optical recording medium. When the surface does not become a light incident surface, it means a support substrate.

The present invention, as long as you target optical recording medium having three or more information recording layers laminated, the type of each information recording layer (read-only type, write-once, rewritable) is not particularly limited In an optical recording medium having three or more information recording layers stacked, the upper information recording layer (L1, L2,...) As viewed from the information recording layer (L0 layer) located at the lowermost layer is used. Not only is a very high light transmittance required, but also a difference in reflectance between before and after recording needs to be sufficient. In order to satisfy these conditions, when the upper information recording layer is a write-once type, the recording film is made of a mixture of ZnS and SiO ₂ or LaSiON (La ₂ O ₃ , SiO ₂ and Si ₃ N _4). It is preferable to use a material in which magnesium (Mg) and / or aluminum (Al) is added to a dielectric base material mainly composed of a mixture of Such a material not only has a very high light transmittance for the laser beam L in the blue wavelength region (λ = 380 nm to 450 nm), but also has a sufficient difference in reflectance before and after recording. It is suitable as a material for the recording film to be constituted.

  The recording mechanism for a recording film made of such a material is accompanied by a phase change. That is, when a predetermined portion of the recording film made of the above material is irradiated with the laser beam L, the phase state of the portion is changed by the heat to form a recording mark. At this time, since the reflectance with respect to the laser beam L differs greatly between the portion where the recording mark is formed in the recording film and the other portion (blank region), data can be recorded / reproduced using this. .

  Here, magnesium (Mg) and / or aluminum (Al) added to the dielectric base material serves as a recording auxiliary material for the dielectric base material. That is, although the dielectric base material alone causes a phase change, the addition of a recording auxiliary material further promotes the phase change of the dielectric base material, and as a result, the recording characteristics and the reproduction characteristics are greatly improved. To do. Further, the recording auxiliary material itself may change its state (for example, crystal growth) with the phase change of the dielectric base material. In this case, the C / N ratio is further improved by this change.

  On the other hand, although the light transmittance does not matter for the lowermost information recording layer, the laser beam L is irradiated through the upper information recording layers (L1, L2,...), So that the reflection is very high. A rate is required. In order to satisfy such a condition, when the lowermost information recording layer is a write-once type, the recording material can be the above-mentioned material, but a laminate composed of at least two inorganic reaction films. More preferably, the body is used.

  In this case, as the material of one inorganic reaction film, aluminum (Al), silicon (Si), germanium (Ge), carbon (C), tin (Sn), gold (Au), zinc (Zn), copper ( Cu), boron (B), magnesium (Mg), titanium (Ti), manganese (Mn), iron (Fe), gallium (Ga), zirconium (Zr), silver (Ag), bismuth (Bi) and platinum ( It is preferable that one material selected from the group consisting of Pt) is a main component, and the other inorganic reaction film is mainly composed of another material selected from the above group. In particular, in order to suppress the noise level of the reproduced signal to a lower level, the main component of one inorganic reaction film is copper (Cu), aluminum (Al), zinc (Zn), or silver (Ag), and the other inorganic reaction film. It is preferable that silicon (Si), germanium (Ge), or tin (Sn) is used as the main component, and the main component of one inorganic reaction film is copper (Cu) and the main component of the other inorganic reaction film is silicon (Si). ) Is most preferable. In this case, the main component of the inorganic reaction film located on the light transmission layer side is preferably silicon (Si), and the main component of the inorganic reaction film located on the support substrate side is preferably copper (Cu). By using a material containing such an element as a main component as the material of the inorganic reaction film, the noise level of the reproduction signal can be suppressed to a lower level and the environmental load can be suppressed.

  When the main component of one inorganic reaction film is copper (Cu), aluminum (Al), zinc (Zn), tin (Sn), gold (Au) or magnesium (Mg) is added thereto. Preferably, when the main component of one inorganic reaction film is aluminum (Al), magnesium (Mg), gold (Au), titanium (Ti) or copper (Cu) is added thereto. In the case where the main component of one inorganic reaction film is zinc (Zn), it is preferable that magnesium (Mg), aluminum (Al) or copper (Cu) is added thereto. When the main component of the inorganic reaction film is silver (Ag), it is preferable that copper (Cu) or palladium (Pd) is added thereto. When such an element is added, the noise level of the reproduction signal can be further reduced, and the reliability for long-term storage can be enhanced.

  The recording mechanism for the recording film having such a structure is that the materials constituting each inorganic reaction film are melted and mixed by the heat of the laser beam L. At this time, since the reflectivity with respect to the laser beam L differs greatly between the recording mark portion mixed with the material constituting each inorganic reaction film and the unmixed portion (blank region), data recording / reproduction is performed using this. It can be performed.

Hereinafter, concrete description will be given about the present invention with reference to Examples, the present invention is not intended to be limited to these Examples.

[Characteristic comparison test 1]
In the characteristic comparison test 1, it was examined how much interlayer crosstalk occurs from the L3 layer 50 to the other information recording layers (L0 layer 20, L1 layer 30, and L2 layer 40) in the information recording layer having a four-layer structure.

[Preparation of sample]
A four-layer optical recording medium sample # 1 having the same structure as that shown in FIG. 5 was produced by the following method.

  First, a disk-shaped support substrate 11 made of polycarbonate having a thickness of 1.1 mm, a diameter of 120 mm, and a spiral groove (track pitch (groove pitch) = 0.32 μm) formed on the surface by an injection molding method. Was made.

Next, this support substrate 11 is set in a sputtering apparatus, and a reflective film having a thickness of 100 nm made of an alloy of silver (Ag), palladium (Pd), and copper (Cu) is formed on the surface on which the groove is formed, ZnS A second dielectric film having a thickness of 39 nm comprising a mixture of SiO ₂ and SiO ₂ (molar ratio = 80: 20), copper (Cu) as a main component, aluminum (Al) being added thereto at 23 atomic%, and gold (Au) being An inorganic reaction film having a thickness of 5 nm added with 13 atm%, an inorganic reaction film having a thickness of 5 nm made of silicon (Si), and a first dielectric having a thickness of 20 nm made of a mixture of ZnS and SiO ₂ (molar ratio = 80: 20). A body film was sequentially formed by sputtering. Thus, the L0 layer 20 was completed.

  Next, the support substrate 11 on which the L0 layer 20 was formed was set in a spin coater, and while rotating, an acrylic ultraviolet curable resin was dropped on the L0 layer 20 and spin coated. Next, a translucent resinous stamper having a spiral groove pattern is placed on the surface of the spincoated resin layer, and the resin solution layer is cured by irradiating the resin solution with ultraviolet rays through the stamper. The stamper was peeled off. Thereby, a transparent intermediate layer 12 (Da = 10 μm) having a spiral groove (track pitch (groove pitch) = 0.32 μm) and a thickness of 10 μm was completed.

Next, the support substrate 11 on which the L0 layer 20 and the transparent intermediate layer 12 are formed is set in a sputtering apparatus, and _both a mixed target of ZnS and SiO ₂ (molar ratio = 80: 20) and a target made of magnesium (Mg) are used. Was used to form an L1 recording film having a thickness of 32 nm with an atomic ratio of a mixture of ZnS and SiO ₂ and magnesium (Mg) of about 50:50 by sputtering. Thus, the L1 layer 30 was completed.

  Next, using the same method as the formation of the transparent intermediate layer 12, a transparent intermediate layer 13 (Db = 10 μm) having a thickness of 10 μm is formed on the L1 layer 30, and then the same method as the formation of the L1 recording film is performed. The L2 recording film having a thickness of 24 nm was formed on the transparent intermediate layer 13 by sputtering. Thus, the L2 layer 40 was completed.

  Further, after forming the transparent intermediate layer 14 (Dc = 10 μm) having a thickness of 10 μm on the L2 layer 40 using the same method as the formation of the transparent intermediate layer 12, the same method as the formation of the L1 recording film is used. Then, an L3 recording film having a thickness of 18 nm was formed on the transparent intermediate layer 14 by a sputtering method. Thus, the L3 layer 50 was completed.

  Then, an acrylic ultraviolet curable resin was coated on the L3 layer 50 by a spin coating method, and this was irradiated with ultraviolet rays to form a light transmission layer 19 having a thickness of 85 μm.

  Thus, the optical recording medium sample # 1 was completed.

[Evaluation of Sample] (Example of Evaluation Method According to the Present Invention)
Next, the optical recording medium sample # 1 is set in an optical disk evaluation apparatus (trade name: DDU1000, manufactured by Pulstec Inc.) and rotated at a linear velocity of 5.3 m / sec, and the numerical aperture is 0.85. A laser beam having a wavelength of 405 nm is irradiated to the L3 layer 50 (an example of “an information recording layer other than a predetermined information recording layer” in the present invention) through an objective lens, and an 8T single signal in the 1,7RLL modulation system ( An example of “data” in the present invention was recorded. On the other hand, recording was not performed on the L0 layer 20, the L1 layer 30, and the L2 layer 40 (an example of the “predetermined information recording layer” in the present invention) . The L0 layer 20, the L1 layer 30, the L2 layer 40, and the L3 layer 50 were irradiated with the laser beam L set to the reproduction power Pr, and the C / N ratio of the obtained 8T signal was measured (the present invention). An example of a measuring method according to).

  The measurement results are shown in FIG. As shown in FIG. 10, it was confirmed that the 8T signal recorded in the L3 layer 50 also leaked in the unrecorded L0 layer 20, L1 layer 30, and L2 layer 40. Such interlayer crosstalk is the largest in the L1 layer 30 and is in the order of the L2 layer 40 and the L0 layer 20 below. In particular, the interlayer crosstalk to the L1 layer 30 is directed to the L2 layer 40 and the L0 layer 20. It was much larger than the inter-layer crosstalk. This is because the thickness Db of the transparent intermediate layer 13 and the thickness Dc of the transparent intermediate layer 14 match (Db = Dc = 10 μm), so that when the L1 layer 30 is focused on the laser beam L, the L2 layer 40 It is considered that this is because the laser beam L ′ reflected at 1 is focused on the L3 layer 50 where the 8T signal is recorded. The L2 layer 40 has a larger interlayer crosstalk from the L3 layer 50 than the L0 layer 20 because the L2 layer 40 is closer to the L3 layer 50.

[Characteristic comparison test 2]
In the characteristic comparison test 2, the relationship between the difference in thickness between the two transparent intermediate layers and the interlayer crosstalk in the three-layer optical recording medium was examined.

[Preparation of sample]
A three-layer optical recording medium sample # 2-1 having the same structure as that shown in FIG. 1 was produced by the following method.

  First, a disk-shaped support substrate 11 made of polycarbonate having a thickness of 1.1 mm, a diameter of 120 mm, and a spiral groove (track pitch (groove pitch) = 0.32 μm) formed on the surface by an injection molding method. Was made.

Next, the support substrate 11 is set in a sputtering apparatus, and a target composed of a mixed target of ZnS and SiO ₂ (molar ratio = 80: 20) and magnesium (Mg) is formed on the surface on which the grooves and lands are formed. Using both of them, a 32 nm thick L0 recording film having an atomic ratio of a mixture of ZnS and SiO ₂ and magnesium (Mg) of about 50:50 was formed by sputtering. Thus, the L0 layer 20 was completed.

Next, the support substrate 11 on which the L0 layer 20 was formed was set in a spin coater, and while rotating, an acrylic ultraviolet curable resin was dropped on the L0 layer 20 and spin coated. Next, a translucent resinous stamper having a spiral groove pattern is placed on the surface of the spincoated resin layer, and the resin solution layer is cured by irradiating the resin solution with ultraviolet rays through the stamper. The stamper was peeled off. As a result, a transparent intermediate layer 12 (Da = 1 3 μm) having a thickness of 13 μm and a spiral groove (track pitch (groove pitch) = 0.32 μm) was completed.

Next, using the same method as the formation of the L0 layer 20, a 24 nm thick L1 recording film having an atomic ratio of a mixture of ZnS and SiO ₂ and magnesium (Mg) of about 50:50 is formed by sputtering. Filmed. Thus, the L1 layer 30 was completed.

  Next, using the same method as the formation of the transparent intermediate layer 12, a transparent intermediate layer 13 (Db = 10 μm) having a thickness of 10 μm is formed on the L1 layer 30, and then the same method as the formation of the L1 recording film is performed. The L2 recording film having a thickness of 18 nm was formed on the transparent intermediate layer 13 by sputtering. Thus, the L2 layer 40 was completed.

  Then, an acrylic ultraviolet curable resin was coated on the L2 layer 40 by a spin coating method, and this was irradiated with ultraviolet rays to form a light transmissive layer 19 having a thickness of 88.5 μm.

  Thus, the optical recording medium sample # 2-1 was completed.

  Next, the optical intermediate layer 13 was set to 13 μm in thickness and the light transmissive layer 19 was set to 87 μm in thickness, using the same method as the optical recording medium sample # 2-1. Recording medium sample # 2-2 was produced.

  Further, optical recording was performed using the same method as that of the optical recording medium sample # 2-1 except that the thickness (Db) of the transparent intermediate layer 13 was set to 15 μm and the thickness of the light transmission layer 19 was set to 86 μm. Media sample # 2-3 was produced.

  Then, optical recording was performed using the same method as that of the optical recording medium sample # 2-1 except that the thickness (Db) of the transparent intermediate layer 13 was set to 17 μm and the thickness of the light transmission layer 19 was set to 85 μm. Media sample # 2-4 was prepared.

[Evaluation of sample] (Another example of the evaluation method according to the present invention)
Next, under the same conditions as the evaluation of the sample in the optical recording medium sample # 1, the L2 layer 40 of the optical recording medium samples # 2-1 to # 2-4 (information other than the predetermined information recording layer in the present invention) 8T single signal (an example of “data” in the present invention) was recorded on each “other example of the recording layer” . In each optical recording medium sample, recording was not performed on the L0 layer 20 and the L1 layer 30. Then, the L0 layer 20 (another example of the “predetermined information recording layer” in the present invention) of each optical recording medium sample is irradiated with the laser beam L set at the reproduction power Pr, and an 8T signal due to interlayer crosstalk (Another example of the measuring method according to the present invention) was measured . The L0 layer 20 is an information recording layer that remarkably receives interlayer crosstalk from the L2 layer 40 due to the influence of the laser beam L ′ reflected by the L1 layer 30.

  The measurement results are shown in FIG. As shown in FIG. 11, the interlayer crosstalk from the L2 layer 40 to the L0 layer 20 is the optical recording medium sample # 2-2 (in which the thickness Da of the transparent intermediate layer 12 is equal to the thickness Db of the transparent intermediate layer 13). Da = Db = 13 μm), and it was confirmed that the interlayer crosstalk decreases as the difference between the two increases. As a result, it was confirmed that when the thicknesses of the adjacent transparent intermediate layers were matched, the interlayer crosstalk from the information recording layers separated by two occurred remarkably.

  The optical recording medium sample # 2 in which the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is 3 μm, compared to the optical recording medium sample # 2-3 in which the difference is 2 μm. The reason why the crosstalk between the L-1 layer and the L2 layer 40 is shorter in the optical recording medium sample # 2-1.

[Characteristic comparison test 3]
In characteristic comparison test 3, in an optical recording medium having a three-layer structure, it was examined how the total interlayer crosstalk of each information recording layer changes by changing the thicknesses of the two transparent intermediate layers.

[Preparation of sample]
Basically, the same method as the preparation of the sample in the characteristic comparison test 2 was used, and various thicknesses were set so that the total layer thickness (Da + Db) of the transparent intermediate layer 12 and the transparent intermediate layer 13 was 40 μm. A number of optical recording medium samples # 3 were produced.

[Evaluation of Sample] (Another Example of Evaluation Method According to the Present Invention)
Next, under the same conditions as the evaluation of the sample in the optical recording medium sample # 1, the two information recording layers included in each optical recording medium sample # 3 (the “information recording layers other than the predetermined information recording layer in the present invention”). to yet another example) of the "records an example) of the" data "in the 8T single signal (present invention, the remainder of the information recording layer (another example of the further the" predetermined information recording layer "in the invention) Was not recorded. Then, among the information recording layers of each optical recording medium sample, the information recording layer that was not recorded is irradiated with the laser beam L set at the reproduction power Pr, and two information recording layers on which signals are recorded The leakage of the 8T signal from the measurement was measured (another example of the measurement method according to the present invention) .

  The measurement results are shown in FIG.

  As shown in FIG. 12, it was confirmed that the interlayer crosstalk to the L2 layer 40 tended to decrease monotonously as the thickness Db of the transparent intermediate layer 13 increased. In addition, the interlayer crosstalk to the L1 layer 30 was minimized when the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 matched (Da = Db = 20 μm). There was no great dependence on the thickness of the transparent intermediate layer, and the overall value was high.

  On the other hand, it was confirmed that the interlayer crosstalk to the L0 layer 20 tends to decrease as the thickness Da of the transparent intermediate layer 12 increases. This decrease tends to be in the range where the thickness Da of the transparent intermediate layer 12 is 20 μm or less. However, it became abrupt when the thickness Da of the transparent intermediate layer 12 exceeded 20 μm.

  Here, in the range where the thickness Da of the transparent intermediate layer 12 is 20 μm or less, the decrease in the interlayer crosstalk to the L0 layer 20 due to the increase in the thickness Da of the transparent intermediate layer 12 is moderate in this range. As the thickness Da of the transparent intermediate layer 12 increases, the influence of interlayer crosstalk from the L1 layer 30 decreases, while the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 decreases. From this, it is considered that the interlayer crosstalk from the L2 layer 40 has increased. On the other hand, in the range where the thickness Da of the transparent intermediate layer 12 exceeds 20 μm, the decrease in the interlayer crosstalk to the L0 layer 20 due to the increase in the thickness Da of the transparent intermediate layer 12 is rapid in this range. As the thickness Da of the intermediate layer 12 increases, not only the influence of interlayer crosstalk from the L1 layer 30 decreases, but also the difference between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 increases. From this, it is considered that the interlayer crosstalk from the L2 layer 40 is also reduced.

  Thus, in the optical recording medium having a three-layer structure, the overall interlayer crosstalk is reduced by setting the relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 to Da> Db. It was confirmed that the most effective suppression was possible.

[Characteristic comparison test 4]
In characteristic comparison test 4, in the optical recording medium having a four-layer structure, it was examined how the total interlayer crosstalk of each information recording layer changes by changing the thickness of the three transparent intermediate layers.

[Preparation of sample]
Basically, using the same method as the preparation of the sample in the characteristic comparison test 1, the thicknesses of the transparent intermediate layer 12, the transparent intermediate layer 13, and the transparent intermediate layer 14 are adjusted so that the total thickness (Da + Db + Dc) is 60 μm. A number of optical recording medium samples # 4 were prepared with various settings.

[Evaluation of Sample] (Another Example of Evaluation Method According to the Present Invention)
First, a sample (Da) in which the transparent intermediate layer 12, the transparent intermediate layer 13, and the transparent intermediate layer 14 are equal in thickness in the optical recording medium sample # 4 under the same conditions as the evaluation of the sample in the optical recording medium sample # 1. = Db = Dc = 20 μm, hereinafter referred to as “basic sample”), and four different information recording layers (another example of the “information recording layer other than the predetermined information recording layer” in the present invention) ) to record an example) of the "data" in the 8T single signal (present invention, made the recording for the rest of the information recording layer (further another example of the "predetermined information recording layer" in the invention) There wasn't. Then, among the information recording layers included in the four basic samples, the information recording layer that was not recorded is irradiated with the laser beam L set at the reproduction power Pr, and the three recorded signals are recorded. The leakage of 8T signal from the information recording layer was measured (another example of the measuring method according to the present invention) .

  As a result, the interlayer crosstalk to the L0 layer 20, the L1 layer 30, the L2 layer 40, and the L3 layer 50 is 20.6 dB, 23.3 dB, 19.8 dB, and 13.1 dB, respectively, and the basic sample (Da = Db = Dc = 20 μm), the interlayer crosstalk to the L1 layer 30 was the largest, and the order was the L0 layer 20, the L2 layer 40, and the L3 layer 50 hereinafter.

  Next, for the remaining optical recording medium sample # 4, 8T single signal recording and interlayer crosstalk measurement were performed in the same manner as described above, and interlayer crosstalk with respect to the basic sample (Da = Db = Dc = 20 μm) was measured. Improvement values are plotted in a ternary diagram. Here, the improvement value is defined by the difference (CE2−CE1) between the largest crosstalk (CE1) of the basic sample and the largest crosstalk (CE2) of the remaining optical recording medium sample # 4. For example, in an optical recording medium sample # 4, the interlayer crosstalk for the L0 layer 20, the L1 layer 30, the L2 layer 40, and the L3 layer 50 is 20.6 dB, 21.3 dB, 20.6 dB, and 16.1 dB, respectively. Then, the improvement value of the present optical recording medium sample # 4 is −2 dB (= 21.3 dB−23.3 dB).

  The measurement results are shown in FIG. As shown in FIG. 13, the thickness Da of the transparent intermediate layer 12 is 20% to 40% of the total layer thickness, the thickness Db of the transparent intermediate layer 13 is 35% to 60% of the total layer thickness, A high improvement rate was observed in the optical recording medium sample # 4 having a thickness Dc of 20% to 40% of the total layer thickness. The thickness Da of the transparent intermediate layer 12 was 22% to 36% of the total layer thickness, and the transparent intermediate layer The optical recording medium sample # 4 in which the thickness Db of the layer 13 is 36% to 55% of the total layer thickness and the thickness Dc of the transparent intermediate layer 14 is 22% to 32% of the total layer thickness shows a particularly high improvement rate. It was.

  Thereby, in the optical recording medium having a four-layer structure, the relationship between the thickness Da of the transparent intermediate layer 12 and the thickness Db of the transparent intermediate layer 13 is set to Da <Db, and the thickness Db of the transparent intermediate layer 13 is set. It was confirmed that the overall interlayer crosstalk can be effectively suppressed by setting the relationship between Db> Dc and the thickness Dc of the transparent intermediate layer 14 to Db> Dc.

  Further, as shown in FIG. 13, in the region of Da <Db and Db> Dc, the region of Da> Dc tends to have a slightly higher overall improvement rate than the region of Da <Dc. It is done. Thereby, in the optical recording medium having a four-layer structure, the relationship among the thickness Da of the transparent intermediate layer 12, the thickness Db of the transparent intermediate layer 13, and the thickness Dc of the transparent intermediate layer 14 is set to Db> Da> Dc. Thus, it was confirmed that the overall interlayer crosstalk can be most effectively suppressed.

As described above, interlayer crosstalk generated in an optical recording medium including three or more information recording layers can be effectively reduced. In particular, compatibility since the interlayer crosstalk in the information recording layers which is not in contact next is effectively reduced, the optical recording medium which is currently commercialized by suppressing the overall thickness of the transparent intermediate layer It is possible to effectively reduce interlayer crosstalk while ensuring.

(A) is a notch perspective view which shows the external appearance of the optical recording medium 10, (b) is the fragmentary sectional view which expanded the A section shown to (a). FIG. 6 is a diagram schematically showing an optical path of a laser beam L when data is reproduced from the optical recording medium 10, where (a) shows the data recorded on the L2 layer 40, and (b) shows the L1 layer 30. When the recorded data is reproduced, (c) shows the case where the data recorded in the L0 layer 20 is reproduced. 4 is a diagram summarizing the degree of interlayer crosstalk given from one information recording layer to another information recording layer in the optical recording medium 10. FIG. It is a figure which shows typically the optical path of laser beam L (L ') when thickness Da of the transparent intermediate layer 12 and thickness Db of the transparent intermediate layer 13 differ, (a) is Da> Db. When set, (b) shows a case where Da <Db is set. 1 is a partial cross-sectional view of an optical recording medium 100. FIG. FIG. 6 is a diagram schematically showing an optical path of a laser beam L when reproducing data from the optical recording medium 100. FIG. 5A shows a case where data recorded on the L3 layer 50 is reproduced, and FIG. In the case of reproducing the recorded data, (c) shows the case of reproducing the data recorded in the L1 layer 30, and (d) shows the case of reproducing the data recorded in the L0 layer 20. 4 is a diagram summarizing the degree of interlayer crosstalk given from one information recording layer to another information recording layer in the optical recording medium 100. FIG. It is a figure which shows typically the optical path of laser beam L (L ') when thickness Db of the transparent intermediate layer 13 and thickness Dc of the transparent intermediate layer 14 differ, (a) is Db> Dc When set, (b) shows a case where Db <Dc. FIG. 5 is a schematic diagram for explaining the reason why an optical recording medium having five or more information recording layers is affected by interlayer crosstalk from four information recording layers separated from each other. 3 is a graph showing measurement results in a characteristic comparison test 1; 5 is a graph showing measurement results in a characteristic comparison test 2. 10 is a graph showing measurement results in characteristic comparison test 3. It is a ternary diagram showing the measurement results in the characteristic comparison test 4.

DESCRIPTION OF SYMBOLS 10,100 Optical recording medium 11 Support substrate 12-15 Transparent intermediate layer 19 Light transmission layer 19a Light incident surface 20 L0 layer 30 L1 layer 40 L2 layer 50 L3 layer 60 L4 layer

Claims (7)

  A substrate constituting one surface of the optical recording medium, a protective layer constituting the other surface of the optical recording medium, three or more information recording layers provided between the protective layer and the substrate, and each information An optical recording medium comprising: a plurality of transparent intermediate layers provided between recording layers, wherein at least a pair of adjacent transparent intermediate layers have different thicknesses.   The information recording layer includes a first information recording layer, a second information recording layer close to a surface on the side that becomes a light incident surface of the one and the other surfaces when viewed from the first information recording layer, A third information recording layer close to the light incident surface when viewed from the second information recording layer, and the transparent intermediate layer is between the first information recording layer and the second information recording layer. And a first transparent intermediate layer provided between the second information recording layer and the third information recording layer, and the first transparent intermediate layer. The optical recording medium according to claim 1, wherein the layer is thicker than the second transparent intermediate layer.   When the thickness of the second transparent intermediate layer is 100%, the difference between the thickness of the first transparent intermediate layer and the thickness of the second transparent intermediate layer is 5% to 100%. The optical recording medium according to claim 2.   The information recording layer includes a first information recording layer, a second information recording layer close to a surface on the side that becomes a light incident surface of the one and the other surfaces when viewed from the first information recording layer, A third information recording layer close to the light incident surface when viewed from the second information recording layer, and a fourth information recording layer close to the light incident surface when viewed from the third information recording layer, The transparent intermediate layer includes a first transparent intermediate layer provided between the first information recording layer and the second information recording layer, the second information recording layer, and the third information recording. A second transparent intermediate layer provided between the third information recording layer and a third transparent intermediate layer provided between the third information recording layer and the fourth information recording layer. 2. The optical recording medium according to claim 1, wherein the second transparent intermediate layer is thicker than the first and third transparent intermediate layers.   The optical recording medium according to claim 4, wherein the first transparent intermediate layer is thicker than the third transparent intermediate layer.   The thickness of the first transparent intermediate layer is 20% to 40% and the thickness of the second transparent intermediate layer is 35% to 60% with respect to the total thickness of the first to third transparent intermediate layers. 6. The optical recording medium according to claim 4, wherein the thickness of the third transparent intermediate layer is 20% to 40%.   The thickness of the first transparent intermediate layer is 22% to 36% and the thickness of the second transparent intermediate layer is 36% to 55% with respect to the total layer thickness of the first to third transparent intermediate layers. The optical recording medium according to claim 6, wherein a thickness of the third transparent intermediate layer is 22% to 32%.

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