JP2010198669A - Optical recording medium and method for manufacturing the same - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a method for forming, using a simple procedure, a hologram material layer of interference fringes that does not have reduction in playback efficiency, even if the hologram material layer generating recording contraction in an optical recording medium is irradiated with a playback laser beam having wavelength which is identical to that of a recording laser beam. <P>SOLUTION: Polarization laser beams of two luminous fluxes which can interfere with each other are made incident, in the hologram material layer from opposite directions, at an incident angle θ which is symmetric with the center of the hologram material layer, and the interval Dp between interference fringes in the interference fringe pattern is specified to be an optimum interference fringe interval by which the maximum diffraction efficiency is obtained by irradiation with a laser beam having a reproducing wavelength, even if recording contraction is generated by the recording laser beam. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

  The present invention relates to an optical recording medium and a method for manufacturing the same.

  Patent Document 1 discloses a data writing system for performing bit-by-bit recording by changing the reflectance by locally modifying the format hologram after forming a format hologram (reflection hologram) on a recording medium. A method is disclosed.

  Non-Patent Document 1 describes: 1. Hologram destruction by short pulse laser. 2. Inelastic deformation of hologram by local heating based on light collection; Three methods of local denaturation have been proposed in which the unexposed part disappears due to continued light collection. Further, it is disclosed that there are positive tuning and negative tuning as inelastic deformation of the hologram.

  On the other hand, a photopolymer generally used as a hologram recording material causes volume shrinkage due to a photopolymerization reaction by laser light, and as a result, an interference fringe interval of a reflection hologram may be narrowed. In this case, if reproduction is performed with a reproduction laser beam having the same wavelength as the laser beam used when forming the interference fringes, there is a problem that a Bragg mismatch occurs and a sufficient reproduction output cannot be obtained.

  When a photopolymer is used as a hologram material and a pair of coherent polarized laser beams are irradiated at 180 ° opposite to each other and information is recorded on the optical recording medium on which a reflection hologram is formed by local heating as described above. FIG. 10 shows the detection signal profile.

  In FIG. 10, the position on the circumference of the optical recording medium is shown on the horizontal axis. Recording was performed with local heating at a location of X = 0 on the horizontal axis. The vertical axis represents the degree of modulation (reflectance change) when reproducing while moving the position on the circumference.

  From FIG. 10, it can be seen that the reflectance decreases at the locally heated recording locations, but the reflectance increases at locations adjacent to both sides. This is because the volume of the photopolymer is changed by local heating, and the interference fringe interval changes depending on the position on the optical recording medium. It is considered that both ends of the recording location are expanded by heating, and the interference fringe spacing that has been narrowed is widened to satisfy the Bragg diffraction condition, thereby increasing the reflectance. Such a change in reflectance is not preferable because it easily leads to an error when the binary threshold is cut from the reproduction signal.

Japanese translation of PCT publication No. 2002-502057

P. R. Mclead, et. al. , Appl Opt vol.47, 2696 (2008)

  The present invention has been made in view of the above problems, and even when a hologram material that causes volume shrinkage such as a photopolymer is used, an increase in reflectance on both sides of a place of local heating can be suppressed, and recording can be performed. It is an object of the present invention to provide an optical recording medium in which a large reproduction output can be obtained by a reproducing laser beam having the same wavelength as the reproducing laser beam.

  The present inventor irradiates the hologram material with a coherent polarized laser beam from the opposite direction to form a reflection hologram, by tilting the incident optical axis with respect to the normal line of the optical recording medium, It has been found that the interference fringe spacing in the reflection hologram can be optimized for reproduction laser light even if local heating occurs due to irradiation of the recording laser light.

  That is, the above-described problems can be solved by the following embodiments.

(1) An optical recording medium having an information recording layer on which a pattern of interference fringes is formed by irradiating a hologram recording material layer with two light beams of laser beams, and an interference fringe interval Dp in the pattern is on the information recording layer An optical recording medium characterized in that Dp ≧ Dpmax is satisfied, where Dpmax is an optimum interference fringe interval that maximizes the diffraction efficiency of the interference fringes upon irradiation with a reproducing laser beam.

(2) The recording material shrinkage rate of the hologram material is set such that Dp is such that the interference fringe spacing Λ × (1−α) ≧ Dpmax at the time of recording (1) An optical recording medium according to 1.

(3) The optical recording medium according to (1) or (2), wherein the interference fringes are reflection holograms.

(4) An optical recording medium for forming a reflection hologram in the hologram recording material layer by irradiating the hologram recording material layer with two laser beams having the same wavelength as that of the information recording laser beam facing from both sides In the manufacturing method, the two laser beams are symmetric with respect to the medium normal perpendicular to both surfaces of the hologram material layer in the thickness direction of the hologram material layer with respect to the medium normal Irradiating so as to intersect at an equal angle θ, A method for producing an optical recording medium

  According to the present invention, even in an optical recording medium in which a photopolymer that causes volume shrinkage due to local heating is used as a hologram recording material, it is possible to suppress an increase in reflectance on both sides of a local heating point and to reproduce at the same wavelength as during recording. There is an effect that a large reproduction output can be obtained by the laser beam.

A diagram showing the relationship between the degree of reflectance reduction and the recording shrinkage when recording shrinkage occurs in the reflection hologram layer of an optical recording medium Vector diagram showing the relationship between the incident laser beam light vector and the incident angle of the reflection hologram 1 is a block diagram showing a reflection hologram forming optical system for carrying out a method for manufacturing an optical recording medium according to Embodiment 1 of the present invention. Sectional drawing which shows typically the outline of the optical recording medium in which the reflection type hologram layer was formed by the reflection type hologram formation optical system of FIG. The block diagram which shows the hologram measuring optical system for confirming the reflection type hologram formed by the reflection type hologram formation optical system shown by FIG. Block diagram showing a recording / reproducing optical system for recording / reproducing information on an optical recording medium on which a reflection hologram is formed by the hologram forming optical system A diagram showing the relationship between the incident angle of a hologram reproducing laser beam and the reflectance of reflected light on an optical recording medium on which a reflective hologram layer is formed A diagram showing the relationship between the position near the recording mark formed at one point of the reflection type hologram layer and the reflection change rate Block diagram showing another embodiment of the reflection hologram forming optical system A diagram showing the relationship between the position in the vicinity of a recording mark formed at one point of an optical recording medium having a conventional reflection type hologram layer and the reflection change rate

  In the embodiment of the present invention, after the recording shrinkage caused by irradiating the reflection hologram layer with the recording laser beam, the interval between the interference fringes is the reproduction output when reproducing the information by irradiating the reproduction laser beam. The exposure interference interval is widened in advance when the reflective hologram layer is formed so that the optimum interference fringe interval, which is the maximum interval, is obtained.

  When a reflective hologram layer is formed, when two polarized laser beams that can interfere with each other are irradiated facing each other from both sides of the medium, the incident optical axis is inclined from the medium normal to the same angle (exposure angle) to perform interference exposure. Do. In this case, the exposure angle θ is calculated in advance from the recording shrinkage rate of the hologram material.

  FIG. 1 shows a result of simulating the degree of decrease in reflectance when recording contraction occurs in a reflection hologram layer uniformly formed over the depth direction of 10 μm of the optical recording medium.

  For example, with a recording shrinkage of 0.5%, the reflectance decreases to about 60%. Therefore, when a hologram material having a recording shrinkage of 0.5% is used, if the interference fringe spacing in the reflective hologram layer is increased by 0.5%, the recording laser beam is irradiated during recording. Even if the recording shrinkage occurs, a favorable change in reflectance can be obtained even if reproduction is performed with a reproducing laser beam having the same wavelength as the recording laser beam.

  In FIG. 1, the alternate long and short dash line shows the relationship between the recording shrinkage rate and the absolute value of the diffraction efficiency, and the solid line shows the diffraction efficiency when the recording shrinkage rate is 0.00% and the diffraction when the recording shrinkage rate is larger than this. The ratio to efficiency is shown.

  The relationship between the ratio of increasing the interference fringe spacing as described above and the tilt angle θ from the medium normal of the two light beams at the time of hologram formation can be obtained as follows.

  FIG. 2 shows the relationship between the vectors of the incident laser beam in the reflection hologram forming portion, and k1 and k2 represent the light wave vectors of the laser beam incident at the crossing angle θ with respect to the medium normal direction.

  Here, K is the interference vector, λ is the wavelength of the incident laser beam, and Λ is the distance between the interference fringes. These relationships and the relationship with θ are expressed by the following equations (1) to (4). It is expressed by the formula.

  The above is a general formula, but when the target interference fringe interval is Dp, the optimum interference fringe interval Dpmax, that is, the recording shrinkage rate is α after this Dp causes recording shrinkage in the hologram material. It is most preferable that Λ × (1−α) = Dpmax. Actually, there are variations in material characteristics, and when Dp <Dpmax, an increase in reflectance occurs on both sides of the recording signal, which is not preferable. Therefore, the variation is absorbed as Dp ≧ Dpmax.

  Embodiments of the present invention will be described below with reference to the drawings.

  In this embodiment, a reflection hologram layer is formed on a hologram recording material by the reflection hologram forming optical system 10 shown in FIG. 3 to obtain an optical recording medium 12 (see FIG. 4). The hologram reflectivity (diffraction efficiency) is confirmed by the reflection type hologram measuring optical system 30 shown in FIG. 6, and further recording / reproducing is performed on the optical recording medium 12 by the recording / reproducing optical system shown in FIG.

  As shown in FIG. 4, the optical recording medium 12 according to the example has an information recording layer 12F formed by forming an interference fringe pattern to be a reflection hologram layer 12H in the depth direction on the hologram recording material layer. is doing.

  First, a reflection hologram forming optical system 10 for manufacturing an optical recording medium 12 according to an embodiment of the present invention will be described with reference to FIG.

  The reflection hologram forming optical system 10 includes an external resonance LD (hereinafter referred to as ECLD) 13 that emits a laser beam, an anamorphic prism 14 that shapes the laser beam emitted from the ECLD 13 into a substantially circular shape, and an optical isolator 15. An optical shutter 16, a spatial filter 17 comprising a lens pair 17A, 17B, and a pinhole 17C therebetween for improving the beam profile of the laser beam that has passed through the optical shutter 16 and reducing the beam diameter; The half-wave plate 19 that shifts the phase of the laser beam reflected by the mirror 18 to be s-polarized light, the beam splitter 20 that splits the s-polarized beam into two light beams, and the beam splitter 20 are transmitted. An optical recording medium in which the s-polarized beam is held by the sample holder 21 ( The optical recording medium before hologram formation is referred to as a sample below) and the reflected light from the beam splitter 20 is incident on the optical recording medium 12 of the sample holder 21 from the opposite direction. In this way, the mirror 22B is configured to reflect, and the sample holder 21 and two apertures 23A and 23B disposed between the mirrors 22A and 22B, respectively.

  The beam splitter 20 and the mirrors 22A and 22B have the same optical path length to the sample holder 21 of the two polarized beams split from the beam splitter 20, and the two polarized beams mutually pass through the information recording layer 12F. It is set to penetrate from the opposite direction. The optical paths of the two polarized beams are above and below each other with respect to both the front and back surfaces of the information recording layer 12F (upper and lower surfaces in FIG. 3) or the medium normal VL perpendicular to the upper and lower surfaces of the sample 12. They are made to intersect at a symmetrical angle θ.

  Next, the reflection hologram measuring optical system 30 shown in FIG. 5 will be described.

  This reflection hologram measuring optical system 30 is different from the reflection hologram forming optical system 10 shown in FIG. 3 in that a pair of photodetectors 31A and 31B, a pair of polarizing beam splitters 32A and 32B, and a pair of quarter-wave plates. 33A, 33B and the shielding plate 34 are added, and the mirror 22A is excluded. The reflection angle of the mirror 22B is such that the reflected laser beam is incident on the optical recording medium 12 and the information recording layer 12F along a medium normal VL perpendicular to the lower surface thereof.

  Since other configurations are the same as those of the reflection hologram forming optical system 10, the same components as those in FIG.

  In the reflection hologram measuring optical system 30, a polarizing beam splitter 32A and a quarter-wave plate 33A are arranged in this order between the mirror 22A and the aperture 23A, and between the mirror 22B and the aperture 21B. The polarizing beam splitter 32B and the quarter wavelength plate 33B are arranged in this order, and the photodetector 31A enters the polarizing beam splitter 32A from the direction of the sample holder 21 through the aperture 23A, and is reflected by the laser beam. It is supposed to receive light.

  The photodetector 31B receives the reflected light from the polarization beam splitter 32B of the laser beam reflected in the direction of the sample holder 21 by the mirror 22B.

  Next, the recording / reproducing optical system 40 for the optical recording medium 12 shown in FIG. 6 will be described.

  The recording / reproducing optical system 40 includes a collimator lens 43, a half-wave plate 44, a polarized light between a laser diode 42 that emits a blue laser having a wavelength of 405 nm and the optical recording medium 12 on which the reflection hologram is formed. The beam splitter 45, the quarter wavelength plate 46, and the objective lens 48 are arranged in this order, and the condensing lens 50 and the condensing lens 50 collect the reflected light from the optical recording medium 12 that has returned to the polarizing beam splitter 45. Are provided with a pinhole 52 for reducing the diameter of the light beam from 0.2 to 0.2 mm, and a photodetector 54 for receiving the laser beam with the reduced beam diameter.

  In this recording / reproducing optical system 40, the laser beam, which is the diffused light emitted from the laser diode 42, is converted into parallel light by the collimator lens 43 and further converted into p-polarized light by the half-wave plate 44.

  This p-polarized laser beam passes through the polarization beam splitter 45, is circularly polarized by the quarter-wave plate 46, and is condensed in the optical recording medium 12 by the objective lens 48. The focused light locally denatures the reflection hologram formed in the optical recording medium 12.

  For reproduction, a reproducing laser beam having the same wavelength as the recording wavelength is used. As in the case of recording, the reproduction laser beam is focused on circularly polarized light in the optical recording medium 12 by the objective lens 48, and the focused light becomes parallel light near the focus point and interferes with the reflection hologram. To generate reflected light (diffracted light).

  The reflected light passes through the objective lens 48 and the quarter-wave plate 46 in the opposite direction, becomes s-polarized light, is reflected by 90 ° at the polarization beam splitter 45, and is collected by the condenser lens 50. The beam diameter is narrowed after passing through the pinhole 52, and then detected by the photodetector 54.

Here, in the optical recording medium 12, the region in which the incident laser beam becomes parallel light near the focus point is based on the wavelength λ, the numerical aperture NA of the objective lens, and the refractive index n of the hologram medium. NA, the light collection depth L = 4λn / NA ² .

  Therefore, when λ = 405 nm, NA = 0.85, and the refractive index n = 1.62 of the hologram medium, the light collection width is w = 0.48 μm and the light collection depth is L = 3.6 μm. The reflected light from the reflective hologram layer can be detected. The pinhole 52 provided immediately before the photodetector 54 is for blocking the reflected light (stray light) from other than the reflective hologram layer at the focus position.

  Next, a reflection hologram layer that is an interference fringe pattern is formed on the sample 12 by the reflection hologram forming optical system 10 shown in FIG. 3, and this reflection hologram layer is used as the reflection hologram measuring optical system shown in FIG. The process of confirming the hologram reflectance (diffraction efficiency) by 30 will be described.

  In Example 1, a hologram recording material was prepared as follows.

Synthesis of organometallic fine particle materials;
Tetra-n-butoxytitanium, Ti (OC ₄ H ₉ ) ₄ ; 3.65 g (manufactured by Kojundo Chemical Laboratory Co., Ltd.) and 2-ethyl-1.3-hexanediol (manufactured by Tokyo Chemical Industry Co., Ltd.) 3.1 g) was mixed in 1 ml of n-butanol solvent at room temperature and stirred for 10 minutes. Diphenyldimethoxysilane (manufactured by Shin-Etsu Chemical Co., Ltd., LS-5300) was added to a reaction solution of Ti (OC ₄ H ₉ ) 4 / 2-ethyl-1.3-hexaneniol = 1/2 (molar ratio). 6 g was added to obtain a metal alkoxide solution. Ti / Si = 1/2 (molar ratio).

  A solution consisting of 0.2 ml of water, 0.08 ml of 2N hydrochloric acid solution and 1 ml of butanol solvent was added dropwise to the metal icooxide solution at room temperature while stirring, and the mixture was stirred for 1 hour to conduct hydrolysis reaction and condensation reaction. It was. Thereby, a gel solution was obtained.

Photopolymerizable monomer;
As a photopolymerizable compound, 100 parts by weight of polyethylene glycol diacrylate (Aronix M-245, manufactured by Toagosei Co., Ltd.) and 3 parts by weight of Irgacure 907 (manufactured by Ciba Specialty Chemicals) as a photopolymerization initiator And 0.2 parts by weight of thioxanthen-9-one as a photosensitizer was added to obtain a mixture containing a photopolymerizable compound.

Hologram recording material solution;
The sol solution and the mixture of the photopolymerizable compound are mixed at room temperature so that the ratio of the organometallic matrix material (as a nonvolatile component) is 80 parts by weight and the ratio of the photopolymerizable compound is 20 parts by weight, The hydrolysis and condensation reaction was further allowed to proceed for another hour in the light-shielded state to obtain a hologram recording material solution as a photopolymer.

Configuration of hologram substrate;
A groove 12B having a track pitch of 0.74 μm was formed on a glass disk substrate 12A having a diameter of 120 mm and a thickness of 1 mm by a 2P method as shown in FIG. A dichroic film 12C was formed thereon by sputtering.

  The dichroic film 12C was laminated with silicon nitride 80 nm / silicon oxide 110 nm / silicon nitride 80 nm / silicon oxide 110 nm / silicon nitride 80 nm.

Sample composition;
A glass substrate 12A having a groove 12B and a dichroic film 12C formed thereon is bonded to a glass substrate 12E having a thickness of 450 μm using a UV adhesive (adhesive layer 12D), and the hologram recording material solution Was applied at a temperature of 80 ° C. for 24 hours to evaporate the solvent, thereby obtaining a hologram recording material layer (information recording layer 12F) having a dry film thickness of 20 μm.

  This was covered with a cover layer 12G made of a polycarbonate sheet having a thickness of 100 μm to obtain an optical recording medium (sample) before formation of the reflective hologram layer.

Formation of a reflective hologram layer;
The sample 12 is set on the sample holder 21 in the reflection hologram forming optical system 10 shown in FIG. 3 to form a reflection hologram.

  In the reflection hologram forming optical system 10, the ECLD 13 emits a p-polarized laser beam having a wavelength of 405 nm. In the spatial filter 17, the beam profile is improved and the beam diameter is expanded to about 10 mm. The laser beam is reflected by the mirror 18, converted to s-polarized light by the half-wave plate 19, and then split by the beam splitter 20 into two beams of transmitted light and reflected light. These two light beams are respectively reflected by the mirrors 22A and 22B, are narrowed down to a beam diameter of 4 mm by the apertures 23A and 23B, and interfere with each other in the information recording layer 12F of the sample 12 set in the sample holder 21. By doing so, a reflection type hologram layer having an interference fringe pattern is formed.

  Here, the laser power for forming the hologram was 600 μW on the front surface of the hologram medium, and exposure was performed for 60 seconds. Thereafter, LED light having a central wavelength of 400 nm was irradiated, post-curing was performed, and the polymerization reaction of the hologram material was completed, whereby the optical recording medium 12 was completed.

  Nine types of optical recording media 12 were formed in which the angle θ of the s-polarized beam incident on the sample 12 with respect to the medium normal VL was changed by 1 ° from 0 ° to 8 °.

  The optical recording medium 12 having these reflection hologram layers is sequentially set on the sample holder 21 in the reflection hologram measurement optical system 30 and the reflection hologram is reproduced by a laser beam having a wavelength of 405 nm. As shown, the reflectance at θ = 0 ° to 8 ° was observed.

  From FIG. 7, it can be seen that the maximum reflectance is shown when θ = 5 °. When a hologram is formed at an angle θ indicating the maximum reflectance, the interference fringe spacing Dp becomes the optimum interference fringe spacing.

  This is because the interference fringe interval becomes smaller than the optimum interference fringe interval Λ at the time of recording due to recording contraction, so that Λ> Dpmax is set in advance so that the interference fringe interval becomes Dpmax after recording contraction occurs. It is good. Since the interference fringe interval becomes larger as θ becomes larger from the equation (4), θ ≧ 5 ° needs to be set, and it is preferable that Λ × (1−α) = Dpmax when the recording shrinkage rate is α. In the embodiment, θ = 6 ° in the range of θ ≧ 5 °. Even when θ = 5 °, an increase in the reflectance of the recording mark adjacent portion is suppressed, but about half of the interference fringe distribution is Dp <Dpmax, so that the distribution of Dp <Dpmax is reduced and the reflectance is secured. The optical recording medium 12 on which a reflection hologram was formed by irradiating the hologram material with a laser beam at an inclination angle θ = 6 ° from the medium normal was recorded and reproduced as follows.

  In the recording / reproducing optical system 40 shown in FIG. 6, the optical recording medium 12 is placed at the position of the optical recording medium indicated by reference numeral 12, and the blue laser is emitted from the laser diode 42 with the optical recording medium 12 stopped. Irradiated.

  Next, the optical recording medium 12 was rotated around the irradiated position, and the change in reflectance was observed. FIG. 8 is a graph similar to FIG. 10, and shows a reflectance fluctuation profile in a reproduction signal when recording / reproduction is performed by the recording / reproduction optical system 40.

  From FIG. 8, it can be seen that the medium satisfying Dp ≧ Dpmax has no increase in reflectivity at positions adjacent to both sides of the irradiation center, and a good recording signal profile is obtained.

  In the first embodiment, the reflection hologram is formed by the interference of the two s-polarized laser beams. However, the present invention is not limited to this, and both the two beams may be p-polarized. Alternatively, circularly polarized light may be used. In the case of p-polarized light, the beam polarization direction by the half-wave plate 19 in FIG. Further, θ is not limited to 6 °, and as can be seen from FIG. 7, 5 ° ≦ θ ≦ 7.5 ° may be set in consideration of recording shrinkage from an angle at which the reflectance is 0.16 or more. .

  FIG. 9 shows a reflection hologram forming optical system 70 in which two light beams are both circularly polarized beams.

  This reflection hologram forming optical system 70 is used by changing a part of the reflection hologram measuring optical system 30 shown in FIG. 5, and the same components as those in FIG. The description is omitted by attaching.

  The reflection type hologram forming optical system 70 omits the shielding plate 34 in the reflection type hologram measuring optical system 30 shown in FIG. 5 and reflects the laser beam transmitted through the beam splitter 20 so that the polarizing beam splitter 32A is provided. The structure differs in that it is transmitted and incident on the optical recording medium 12 in the sample holder 21 from the side opposite to the mirror 22B.

  Further, when the reflected light from the mirrors 22A and 22B is incident on the optical recording medium 12, it is different from the reflective hologram measuring optical system 30 in that it is incident at an angle θ with respect to the medium normal VL.

  In the reflection type hologram forming optical system 70, the laser beam emitted from the laser diode 13 is converted into a p-polarized laser beam in the half-wave plate 19, and this p-polarized laser beam is reflected by the beam splitter 20 as reflected light. It is divided into two luminous fluxes of transmitted light.

  The two polarized laser beams are reflected by the mirrors 22A and 22B, respectively, and then transmitted through the polarization beam splitters 32A and 32B, respectively, to be circularly polarized by the quarter-wave plates 33A and 33B.

  Next, the circularly polarized laser beams are incident on the optical recording medium 12 from above and below in the drawing, and interfere with each other in the hologram material layer to form a reflective hologram layer.

  According to the present invention, interference fringes can be formed on a hologram material layer that causes recording contraction with a simple configuration so that the reproduction efficiency does not decrease even when reproduction is performed with a reproduction laser beam having the same wavelength as the recording laser beam.

DESCRIPTION OF SYMBOLS 10,70 ... Reflection type hologram formation optical system 12 ... Optical recording medium 12A ... Glass disk substrate 12B ... Groove 12C ... Dichroic film 12E ... Glass substrate 12F ... Information recording layer 12G ... Cover layer 12H ... Reflective hologram layer 13 ... External resonance Type LD (ECLD)
30 ... Reflective hologram measuring optical system 40 ... Recording / reproducing optical system

Claims (4)

An optical recording medium having an information recording layer on which an interference fringe pattern is formed by irradiating a hologram recording material with a two-beam laser beam,
The interference fringe interval Dp in the pattern is Dp ≧ Dpmax, where Dpmax is the optimum interference fringe interval at which the diffraction efficiency at the interference fringe is maximized when the information recording layer is irradiated with the reproducing laser beam. An optical recording medium characterized by being configured as described above. In claim 1,
An optical recording medium characterized in that when the recording shrinkage ratio of the hologram material is α, the Dp is set such that the interference fringe spacing Λ × (1−α) ≧ Dpmax at the time of recording. In claim 1 or 2,
The optical recording medium, wherein the interference fringes are reflection holograms. This is a method for manufacturing an optical recording medium in which a hologram recording material layer is irradiated with a two-beam laser beam having the same wavelength as the information recording laser beam facing from both sides to form a reflection hologram in the hologram recording material. And
The two laser beam beams intersect with the medium normal perpendicular to both surfaces of the hologram material layer at an equal angle θ symmetric with respect to the medium normal in the thickness direction of the hologram material layer. The method of manufacturing an optical recording medium, characterized in that

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