WO2006118036A1 - Method and device for recording/reproducing hologram - Google Patents
Method and device for recording/reproducing hologram Download PDFInfo
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- WO2006118036A1 WO2006118036A1 PCT/JP2006/308261 JP2006308261W WO2006118036A1 WO 2006118036 A1 WO2006118036 A1 WO 2006118036A1 JP 2006308261 W JP2006308261 W JP 2006308261W WO 2006118036 A1 WO2006118036 A1 WO 2006118036A1
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- Prior art keywords
- light
- hologram recording
- hologram
- region
- reference light
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Classifications
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/04—Processes or apparatus for producing holograms
- G03H1/0465—Particular recording light; Beam shape or geometry
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/12—Heads, e.g. forming of the optical beam spot or modulation of the optical beam
- G11B7/135—Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
- G11B7/1381—Non-lens elements for altering the properties of the beam, e.g. knife edges, slits, filters or stops
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/26—Processes or apparatus specially adapted to produce multiple sub- holograms or to obtain images from them, e.g. multicolour technique
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H2250/00—Laminate comprising a hologram layer
- G03H2250/42—Reflective layer
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
- G11B7/0065—Recording, reproducing or erasing by using optical interference patterns, e.g. holograms
Definitions
- the present invention relates to a recording medium on which optical information recording or information reproduction is performed, such as an optical disk or a light field, and more particularly to hologram recording / reproduction of a recording medium having a hologram recording layer capable of recording or reproducing information by irradiation with a light beam.
- the present invention relates to a method and an apparatus. Background art
- Holograms that can record two-dimensional data at high density are attracting attention for high-density information recording.
- the feature of this hologram is that the wavefront of light carrying recorded information is recorded as a change in refractive index in volume on a recording medium made of a photosensitive material such as a photorefractive material.
- a recording medium is known in which a substrate, a hologram recording layer, and a reflection layer are formed in this order.
- the information light is converged and irradiated so as to have the smallest diameter on the boundary surface between the hologram layer and the protective layer of the recording medium and reflected by the reflective layer.
- the recording reference light is reflected by the hologram layer and the protective layer. Recording on the hologram recording medium by converging so that it has the smallest diameter on the front side of the boundary surface and irradiating as divergent light and causing interference
- the information light is converged on the reflective layer, and the recording reference
- the recording reference There is also a technology for irradiating the recording reference light so that the light is defocused on the reflective layer and the conjugate focal point of the recording reference light is located on the substrate side of the boundary surface between the substrate and the hologram recording layer.
- an object lens configuration of an aspect in which recording / reproduction is performed from one side of a hologram recording layer of a recording medium in Japanese Patent Application Laid-Open Nos. 1-11 3 1 1 9 3 8 and 2 0 4 -1 7 1 6 1 1 Examples are shown in Figs. 1 and 2, respectively.
- the reference light and the signal light are coaxially guided to the objective lens OB so that they overlap each other.
- the light always interferes on the optical axis.
- a reflective layer is placed at the focal point P of the signal light and the recording medium is placed between the objective lens and the reflective layer, the reference light and the signal light pass back and forth through the recording medium to perform hologram recording. Is called.
- the reference light passes back and forth through the recording medium, and the reflected reference light returns to the objective lens OB together with the reproduction light.
- the holograms specifically recorded in the recording medium are holograms A (recording interference between reflected reference light and reflected signal light), holograms, B (recording of interference between incident reference light and reflected signal light), hologram C (recording interference between reflected reference light and incident signal light), hologram D (incident There are four types of recordings where the interference between the reference beam and the incident signal beam is recorded.
- the reproduction light obtained from the recording medium during the reproduction process is also reproduced light from the hologram A (read out by the reflected reference light), holo Reproduction light from Gram B (read out with incident reference light), reproduction light from hologram (read out with reflected reference light), reproduction light from hologram D (read out with incident reference light) 4 It is a kind.
- an example of the problem to be solved by the present invention is to provide a hologram recording / reproducing method and a hologram apparatus that enable stable recording or reproduction.
- a recording medium having a hologram recording layer that stores therein optical interference fringes by coherent signal light and reference light as a diffraction grating is provided on a light irradiation surface of the hologram recording layer. Wear so that the reflective layer is located on the opposite side A support part for holding freely;
- a signal light generation unit including a spatial light modulator that is arranged on the optical axis and generates the signal light by modulating the reference light according to recording information;
- a hologram recording apparatus comprising: an interference unit configured to irradiate the hologram recording layer with the signal light and the reference light to form a diffraction grating by optical interference fringes inside the hologram recording layer;
- An anti-reflective mask disposed in the optical path of the reference light and partially blocking the reference light; an objective lens disposed coaxially with the anti-reflective mask and condensing the reference light that has passed through the reflective layer; It is characterized by including these.
- the hologram reproducing device is a hologram reproducing device for reproducing information from a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
- a support unit that holds the recording medium so that the reflective layer is positioned on the opposite side of the light irradiation surface of the hologram recording layer;
- An anti-reflection mask comprising a light-shielding region and a light-transmitting region which are anti-symmetric about the optical axis of the reference light, which is disposed in the optical path of the reference light and partially blocks the reference light;
- the reference light is condensed on the reflection layer so as to pass through the anti-reflection mask and the diffraction grating of the hologram recording layer to generate reproduction light from the diffraction grating, and the reproduction light is received.
- An objective lens ;
- the hologram recording method according to claim 22 is a hologram recording method for recording information on a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
- an anti-reflection mask consisting of a light-shielding region and a light-transmitting region that are anti-symmetric about the optical axis of the reference light, which partially shields the reference light, in the optical path of the reference light;
- a reflective layer on the opposite side of the light irradiation surface; and reflecting the reference light so as to pass through the hologram recording layer while passing through the light-transmitting region of the anti-reflection mask and converging by the objective lens. Irradiating the layer and reflecting on the reflective layer, and
- signal light obtained by modulating the reference light according to recording information is caused to interfere with the reference light in the hologram recording layer to form a diffraction grating.
- the hologram reproducing method according to claim 23 is a hologram reproducing method for reproducing information from a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
- an anti-reflection mask consisting of a light-shielding region and a light-transmitting region that are anti-symmetric about the optical axis of the reference light, which partially shields the reference light, in the optical path of the reference light;
- 1 and 2 are schematic partial cross-sectional views showing an optical system and a recording medium for explaining conventional hologram recording.
- FIG. 3 is a schematic partial sectional view showing a recording medium for explaining conventional hologram recording.
- FIG. 4 is a schematic configuration diagram showing an optical system and a recording medium for explaining the recording / reproducing apparatus of the embodiment according to the present invention.
- FIG. 5 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 6 is a schematic partial sectional view showing a recording medium according to another embodiment of the present invention.
- 7A to 7D are front views showing a reversal mask in the recording / reproducing apparatus according to the embodiment of the present invention.
- FIG. 13 is a schematic partial sectional view for explaining hologram recording / reproduction according to the embodiment of the present invention.
- FIG. 14 is a schematic partial cross-sectional view showing a recording medium for explaining hologram recording of an embodiment according to the present invention.
- FIG. 15 is a schematic partial sectional view showing an optical system for explaining hologram recording / reproduction according to an embodiment of the present invention.
- FIGS. 16A and 16B are front views showing a reversal mask in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 17 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 18 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 19 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 20 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 21 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 22 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 23 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 24 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 25 is a partial sectional view showing a liquid crystal element in a recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 26 is a front view as seen from the optical axis of the spatial light modulator in the recording / reproducing apparatus according to another embodiment of the present invention.
- FIG. 27 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
- 28A to 28C are front views showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention. Detailed Description of the Invention
- FIG. 4 shows a configuration example of the optical system of the hologram recording / reproducing apparatus in the present embodiment.
- the hologram recording / reproducing apparatus uses a recording medium 2 having a hologram recording layer 7 that stores optical interference fringes as a diffraction grating inside the coherent signal light SB and reference light RB, as opposed to the light irradiation surface of the hologram recording layer 7.
- a support portion (not shown) that is detachably held is provided so that the reflective layer 5 is positioned on the side.
- the hologram recording / reproducing apparatus is roughly composed of a hologram recording and reproducing optical system. These systems share the objective lens 0B and include an objective lens drive system and a servo error detection system (not shown). It is out.
- the hologram recording / reproducing optical system consists of a laser light source LD that generates coherent light for hologram recording and reproduction, a collimator lens CL, first and second half mirrors HM 1 and HM 2, and transmissive spatial light modulation.
- SLM laser light source
- anti-reverse mask RIM anti-reverse mask
- objective lens 0B imaging lens
- imaging lens ML CCD (Charge Coupled Device)
- CMOS Complementary Metal Oxide Semiconductor Device
- the anti-reverse mask RIM belonging to the reference light generation unit is composed of a light-shielding region SR and a light-transmitting region TR that are anti-symmetric about the optical axis of the reference light RB that partially blocks the reference light RB. I can arrange it.
- the spatial light modulator SLM belonging to the signal light generation unit is arranged on the optical axis and modulates the reference light RB according to the recording information to generate the signal light SB.
- the transmissive spatial light modulator SLM is a function of electrically shielding a part of incident light for each pixel by a liquid crystal panel having a plurality of pixel electrodes divided in a matrix, or is not transmitted and transmitted. It has a function to make a modulation state.
- This spatial light modulator SLM is connected to a spatial light modulator driving circuit (not shown), and has a distribution based on the page data to be recorded (information pattern of two-dimensional data such as bright and dark dot patterns on a plane).
- the signal beam SB is generated by modulating and transmitting the light flux as if it has.
- the objective lens OB of the interference unit condenses the reference light R B that is disposed coaxially with the anti-reflection mask R I M and passes through the reflection layer 5.
- the objective lens OB is set so that the reference light RB forms a spot without aberration on the reflection layer 5 of the recording medium.
- the signal light S B is subjected to the action of the spatial light modulator S L M, it forms a spot that is wider than the reference light R B.
- a hologram (diffraction grating) is formed inside the hologram recording layer 7 by the interference fringes of these lights.
- the laser light from the light source D is divided into the optical paths of the signal light SB and the reference light RB by the first half mirror HM 1 and the second light passes through the anti-reflection mask RIM and the spatial light modulator SLM, respectively.
- the beams are merged by the half mirror HM 2 and irradiated coaxially in the hologram recording layer 7 so as to overlap with the reference beam RB.
- the hologram recording / reproducing apparatus omits the second half mirror HM 2 and the optical path of the reference light RB so that the signal light SB overlaps the reference light RB in the hologram recording layer 7 as shown in FIG. It can be configured to be illuminated from the outside. If the optical path of the signal light SB and the reference light RB are completely separated, any of the optical paths of the reference light RB An anti-rotation mask R IM can be placed at some place.
- FIG. 6 shows an example of the recording medium 2.
- the recording medium 2 includes a reflective layer 5, a separation layer 6, a hologram recording layer 7, and a protective layer 8 stacked on the substrate 3 in the film thickness direction. Note that the reflective layer 5 may be separated from the hologram recording layer 7 and configured as a separate body.
- a light-transmitting photosensitive material capable of storing optical interference fringes such as a photopolymer, a light anisotropic material, a photorefractive material, a hole burning material, and a photochromic material is used.
- the substrate 3 supporting each of the above films is made of, for example, glass, polycarbonate, amorphous polyolefin, polyimide, PET, PEN, PES or other plastics, UV curable acrylic resin, or the like.
- the separation layer 6 and the protective layer 8 are made of a light transmissive material, and play a role of flattening the laminated structure and protecting the hologram recording layer and the like.
- Anti-rotation mask R I M is a light-dark pattern that is anti-rotation in the optical path of the effective diameter of reference beam RB.
- the anti-rotation mask RIM having strict anti-rotation symmetry means that the light shielding region SR and the light transmitting region TR are arranged around the optical axis of the reference light RB.
- the light shielding area When a rotation operation rotating by (2m-1) is performed, the light shielding area has a pattern that overlaps the light transmitting area, and the light transmitting area overlaps the light shielding area.
- m is an integer such as 1, 2, 3, 4, 5, 6.
- the light-shielding pattern becomes finer, and the effect of diffraction effects at the boundary of the light-shielding Z light-transmitting region occurs.
- the light source LD generates the reference light RB
- the antireflection mask RIM is partially blocked by the antireflection mask RIM arranged in the optical path of the reference light RB.
- the reflection layer 5 is irradiated so as to pass through the hologram recording layer 7 through the light transmission region TR, converged by the objective lens OB.
- the signal light SB modulated according to the recording information and the reference light RB are caused to interfere with each other in the hologram recording layer 7 to form a diffraction grating.
- the divergent coherent light emitted from the laser light source LD is converted into a parallel light beam by the collimator lens CL, and is condensed as the reference light RB on the recording medium 2 by the objective lens OB via the half mirror HM. Is done. Reproduced light is generated from the diffraction grating of the hologram recording layer and is reflected by the third half mirror HM 3 through the objective lens OB. Reproduced light is imaged on the image sensor IS by the imaging lens ML.
- the generation of the reference beam RB to the irradiation of the reflective layer 5 is the same as that in the photogram recording method, and the reproduction beam is generated from the diffraction grating by the irradiation, and the reproduction beam is transmitted through the objective lens B.
- the image sensor IS to reproduce information by photoelectric conversion.
- normal playback is performed if playback is performed with the same anti-reverse mask R I M as during recording.
- the objective is selected by placing the anti-reverse mask RIM in the reference beam path.
- the light from the objective lens B to the reflective layer 5 (bound light) or the light from the reflective layer 5 to the objective lens OB (return light) Only one of them will exist.
- the anti-rotation mask RIM having a strict anti-rotation symmetry is used, either light is always present in the irradiated portion of the recording medium 2, and there is no place where the light is not irradiated. As shown in Fig.
- the anti-reflection mask RIM is placed in the same way during reproduction, the same reference light RB as that when the hologram is recorded is irradiated, so that only normal reproduction light appears, and phase-shared reproduction light does not appear.
- the light shielding region SR and the light transmitting region TR of the anti-rotation mask RIM shown in FIG. 4 are provided with inversion means INV that inverts or rotates 180 degrees around the optical axis, so Phase conjugation reproduction can be achieved by reversing the light-blocking region SR and the light-transmitting region TR) of the anti-mask RIM or by rotating it 180 degrees around the optical axis.
- inversion means INV that inverts or rotates 180 degrees around the optical axis
- the anti-rotation mask RIM can be composed of a fixed plate-like body, but this is composed of a transmissive liquid crystal element, and at the time of writing, the liquid crystal element shows a light shielding region SR and a light transmissive region TR. It can also be controlled to be in a state.
- the objective lens OB is an ideal lens (for example, a Fourier transform lens)
- a light beam emitted from a point on the page data of the spatial light modulator forms an image on a point on the image plane of the image sensor IS.
- an actual objective lens is affected by lens aberration and MTF characteristics, resulting in image blurring. This is even more conspicuous when the numerical aperture NA of the objective lens OB is large or when the image height (distance from the optical axis of the dot on the page) is large.
- the pattern of the spatial light modulator SLM corresponds to page data.
- a hologram is formed by interfering with the reference light RB between the objective lens OB and the reflecting layer 5. Since the reproduced light appears as if there is a page dew in the original location, the optical path of the reproduced light is the same as that of the actual objective lens during recording, and the influence of the aberration of the objective lens B and the MTF is affected. The received image is blurred on the image sensor IS.
- phase conjugate reproduction the reproduced light appears so as to return back to the optical path of the original signal light SB. Therefore, the original page regardless of the performance of the objective lens ⁇ B The same image as the data can be formed. Therefore, if the NA of the objective lens OB to be used is large, or if there is a part where the spatial light modulator SLM has a large pattern and a large image height, the performance of the objective lens 0B can be improved by using phase conjugate reproduction. Good reproduction images can be obtained without any restrictions. However, since the phase conjugate reproduction light is inferior to the normal reproduction light in the SN ratio, it is preferable to use only the normal reproduction light if reproduction with a good SN ratio is desired. You can choose between normal playback and phase-conjugate playback depending on whether you want the SN ratio or imaging performance.
- the shape of the anti-rotation mask RIM is not strictly anti-rotation-symmetric, and the shading area SR illustrated in FIG. 16A has a slightly smaller area than the translucent area TR. Even if the shape conforms to anti-rotation symmetry (quasi-anti-anti-symmetry), it is possible to greatly reduce the area where “bound reference light” and “return reference light” exist simultaneously in the medium. The effect of the present invention to reduce the influence of a simple hologram can be obtained.
- the light-shielding region SR illustrated in Fig. 16B has a slightly larger area than the light-transmitting region TR, a region where no reference light exists in the medium is generated.
- the areas of the light-shielding region SR and the light-transmitting region TR are strictly equal, and these areas can be increased or decreased if the optical paths of incident light and reflected light in the medium are limited. Can do.
- the spatial light modulator SLM is arranged around the transmission central region TCR arranged on the optical axis that allows the reference light RB to pass through without modulation, and around the transmission central region TCR.
- a spatial light modulation annular region SLMRR composed of a transmissive matrix liquid crystal device that modulates the reference light RB according to information and generates the signal light SB spatially separated from the reference light RB.
- the anti-reflection mask RIM that acts only on the inner periphery may be disposed at any location so as not to affect the signal light s. .
- the anti-reflection mask RIM is arranged so as to partially block only the reference light RB passing through the transmission central region TCR without blocking the signal light SB.
- the transmission central region TCR can be formed of a through opening or a transparent material.
- the transmissive central region TCR is composed of a transmissive liquid crystal element, and is controlled so that the liquid crystal element is in a translucent state during recording. On the other hand, as shown in FIG.
- the spatial light modulator SLM and the anti-rotation mask RIM may be integrally formed, and the other configuration may be the same as the example of FIG.
- the spatial light modulator SLM is arranged around the central mask region CMR as the anti-rotation mask RIM and the central mask region CMR and modulates the reference light RB according to the recording information.
- a spatial light modulation annular region SLMRR composed of a transmissive matrix liquid crystal device that generates signal light SB spatially separated from the reference light RB.
- the central mask area CMR can be composed of a fixed plate, but the central mask area CMR is composed of a transmissive liquid crystal element, and the liquid crystal element displays the light shielding area SR and the translucent area TR during recording. It can also be controlled as is.
- the inner peripheral portion is the signal light SB and the outer peripheral portion is the reference light RB
- the laser beam from the light source LD Only the inner peripheral part of the signal can be modulated so that the inner peripheral part is the signal light SB and the outer peripheral part is the unmodulated reference light RB.
- the spatial light modulator SLM is a transmissive matrix liquid crystal device arranged on the optical axis that modulates the reference light RB in accordance with the recording information and generates the signal light SB.
- Spatial light modulation central region SLM CR consisting of and a transmission annular region TRR arranged around the spatial light modulation central region S LMC R and spatially separated from the signal light SB through the reference light RB without modulation. Consists of.
- the anti-rotation mask RIM is arranged so as to partially block only the reference light RB passing through the transmission annular region TRR without blocking the signal light SB.
- the transmissive annular region TRR consists of a through-opening or a transparent material. Further, the transmissive annular region TRR can be constituted by a transmissive liquid crystal element and can be controlled so that the liquid crystal element is in a light-transmitting state during recording. Further, as shown in FIG.
- the spatial light modulator SLM and the anti-rotation mask RIM may be integrally formed, and the other configuration may be the same as the example of FIG.
- the spatial light modulator SLM modulates the reference light RB in accordance with the recording information and passes it to generate a transmission light matrix liquid crystal disposed on the optical axis. It consists of a spatial light modulation central region SLMCR consisting of a device and an annular mask region RMR as a reversal mask RIM arranged around the spatial light modulation central region SLMCR.
- the annular mask area RMR is composed of a transmissive liquid crystal element, and the liquid crystal element is in a state where the annular mask area RM R displays the light shielding area SR and the light transmitting area TR during recording.
- the liquid crystal device portion of the spatial light modulator SLM or anti-rotation mask RIM—body-type spatial light modulator SLM is composed of a transmissive liquid crystal element, which consists of a pair of opposing polarizing plates 80 liquid crystal layer 83 (crystal molecules) sandwiched between transparent electrodes 81 a and 81 b and alignment films 82 a and 82 b sequentially formed on the inner surfaces of a and 80 b. Layer).
- the transparent electrodes 8 1 a and 8 1 b have one or more pairs of electrode shapes according to the shape of the anti-rotation mask RIM. As shown in FIG.
- the spatial light modulator SLM as a whole is a transmissive matrix liquid crystal device, and its control circuit 26 displays a predetermined pattern, for example, an inner central region A and an outer peripheral region B on its outer periphery. Each can also be configured to display an anti-reflection mask area and a page data area.
- the anti-rotation mask RIM is rotated 180 degrees around the optical axis. If a liquid crystal element is used, the same effect can be obtained only by electrical switching.
- Liquid crystal molecules have the property of rotating the polarization plane of light (rotation) only at the part where voltage is applied.
- the amount of rotation of the polarization plane varies depending on the thickness of the liquid crystal layer and the magnitude of the applied voltage. It is assumed that the polarization of the portion where voltage is applied between the transparent electrodes 8 1 a and 8 1 b is set to rotate 90 degrees. It is assumed that the polarization state of the light passing through the polarizing plate 80 a is linearly polarized light (referred to as A-polarized light) parallel to the paper surface.
- the polarizing plate 80 a is a polarizing plate that allows only the A polarized light to pass therethrough, and the polarizing plate 80 b is the same.
- a voltage is applied to the liquid crystal layer 83 only by a certain electrode pair, and the polarization plane is rotated by 90 degrees only for the light passing through this portion, and linearly polarized light perpendicular to the paper surface (referred to as B-polarized light). It becomes.
- the polarizing plate 80 b facing thereafter passes only the A-polarized light, only the light from the other electrode pair passes, and the other light is blocked.
- the liquid crystal element as a whole acts as an anti-rotation mask RIM that shields light only from a portion to which a voltage is applied.
- RIM anti-rotation mask
- the electrode pattern is made to correspond to the white and shaded portions, and voltage is applied only to the shaded portions.
- the shaded area is the light shielding region SR.
- the embodiment shown in FIGS. 17 to 24 (the signal light SB and the reference light RB are propagated separately along the optical axis at the inner and outer circumferences of the effective diameter of the laser beam from the light source LD.
- the embodiment shown in FIGS. 17 to 24 it is possible to use a QSLM with an anti-reverse mask integrated spatial light modulator that divides the luminous flux into the first to fourth quadrants as viewed from the optical axis.
- signal light SB is generated in a state in which a page data pattern for modulating the reference light RB is displayed in the first and third quadrants Ql and Q3 according to the recording information.
- the fourth quadrant Q2 and Q4 are used as the reference beam RB (however, the second quadrant Q2 is shielded). At this time, the second and fourth quadrants Q2 and Q4 corresponding to the reference beam RB become antisymmetric.
- the first to third quadrants Q1 to Q3 are shielded, and the reference light is in the same light transmission state (fourth quadrant Q4) as during recording.
- phase conjugate reproduction is possible by reversing the brightness and darkness during recording (fourth quadrant Q4 is light-shielded and second quadrant is translucent). Become.
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Abstract
Description
明細書 ホログラム記録再生方法及び装置 技術分野 TECHNICAL FIELD Field of the Invention
本発明は光ディスク、光力一ドなどの光学的に情報記録又は情報再生が行われ る記録媒体に関し、特に光束の照射により情報の記録又は再生可能なホログラム 記録層を有する記録媒体のホログラム記録再生方法及び装置に関する。 背景技術 The present invention relates to a recording medium on which optical information recording or information reproduction is performed, such as an optical disk or a light field, and more particularly to hologram recording / reproduction of a recording medium having a hologram recording layer capable of recording or reproducing information by irradiation with a light beam. The present invention relates to a method and an apparatus. Background art
高密度情報記録のために、 2次元データを高密度記録できるホログラムが注目 されている。 このホログラムの特徴は、記録情報を担持する光の波面を、 フォト リフラクティブ材料などの光感応材料からなる記録媒体に体積的に屈折率の変 化として記録することにある。記録媒体にホログラム多重記録を行うことによつ て記録容量を飛躍的に増大させることができる。構造としては、基板、 ホロダラ ム記録層及び反射層がこの順番で形成された記録媒体が知られている。 Holograms that can record two-dimensional data at high density are attracting attention for high-density information recording. The feature of this hologram is that the wavefront of light carrying recorded information is recorded as a change in refractive index in volume on a recording medium made of a photosensitive material such as a photorefractive material. By performing hologram multiplex recording on the recording medium, the recording capacity can be dramatically increased. As a structure, a recording medium is known in which a substrate, a hologram recording layer, and a reflection layer are formed in this order.
例えば、従来では、情報光は記録媒体のホログラム層と保護層の境界面上で最 も小径となるように収束照射され反射層で反射され、同時に、記録用参照光はホ ログラム層と保護層の境界面よりも手前側で最も小径となるように収束して発 散光として照射して、干渉させることでホログラム記録媒体に記録を行っていた For example, conventionally, the information light is converged and irradiated so as to have the smallest diameter on the boundary surface between the hologram layer and the protective layer of the recording medium and reflected by the reflective layer. At the same time, the recording reference light is reflected by the hologram layer and the protective layer. Recording on the hologram recording medium by converging so that it has the smallest diameter on the front side of the boundary surface and irradiating as divergent light and causing interference
(特開平 1 1— 3 1 1 9 3 8号公報、 参照)。 (See Japanese Patent Laid-Open No. 11-311 938).
またさらに、記録光学系において、情報光を反射層上に収束させ、記録用参照 光が反射層上ではデフォーカスするとともに、記録用参照光の共役焦点が基板と ホ口グラム記録層との境界面よりも基板側に位置するように、記録用参照光を照 射する技術もある (特開 2 0 0 4 - 1 7 1 6 1 1号公報、 参照)。 発明の開示 Furthermore, in the recording optical system, the information light is converged on the reflective layer, and the recording reference There is also a technology for irradiating the recording reference light so that the light is defocused on the reflective layer and the conjugate focal point of the recording reference light is located on the substrate side of the boundary surface between the substrate and the hologram recording layer. (See Japanese Patent Laid-Open No. 2 0 0 4-1 7 1 6 1 1). Disclosure of the invention
例えば特開平 1 1一 3 1 1 9 3 8号公報及び特開 2 0 0 4— 1 7 1 6 1 1号 公報における記録媒体のホログラム記録層の片側から記録再生される態様の対 物レンズ構成例をそれぞれ図 1及び図 2に示す。 For example, an object lens configuration of an aspect in which recording / reproduction is performed from one side of a hologram recording layer of a recording medium in Japanese Patent Application Laid-Open Nos. 1-11 3 1 1 9 3 8 and 2 0 4 -1 7 1 6 1 1 Examples are shown in Figs. 1 and 2, respectively.
いずれの従来技術においても、記録時には、 図に示すように、 '参照光と信号光 は同軸で互いに重なるように対物レンズ O Bに導かれるので、対物レンズ〇 Bで 集光される参照光と信号光は光軸上で常に干渉する状態にある。信号光の焦点 P の位置に反射層を配置して記録媒体を対物レンズ及び反射層の間に配置した場 合、 参照光及び信号光は記録媒体を往復で通過してホ口グラム記録が行われる。 再生時にも、参照光は記録媒体を往復で通過して、反射した参照光が再生光とと もに対物レンズ O Bへ戻ることとなる。 In any conventional technique, as shown in the figure, during recording, the reference light and the signal light are coaxially guided to the objective lens OB so that they overlap each other. The light always interferes on the optical axis. When a reflective layer is placed at the focal point P of the signal light and the recording medium is placed between the objective lens and the reflective layer, the reference light and the signal light pass back and forth through the recording medium to perform hologram recording. Is called. During reproduction, the reference light passes back and forth through the recording medium, and the reflected reference light returns to the objective lens OB together with the reproduction light.
図 3に示すように、記録媒体中に具体的に記録されるホログラムは、 いずれの 技術においても、ホログラム A (反射する参照光と反射する信号光との干渉が記 録されたもの)、 ホログラム B (入射する参照光と反射する信号光との干渉が記 録されたもの)、 ホログラム C (反射する参照光と入射する信号光との干渉が記 録されたもの)、 ホログラム D (入射する参照光と入射する信号光との干渉が記 録されたもの) の 4種類である。 また、再生過程において記録媒体から得られる 再生光も、 ホログラム Aからの再生光 (反射する参照光で読み出される)、 ホロ グラム Bからの再生光 (入射する参照光で読み出される)、 ホログラムじからの 再生光 (反射する参照光で読み出される)、 ホログラム Dからの再生光 (入射す る参照光で読み出される) の 4種類である。 As shown in FIG. 3, the holograms specifically recorded in the recording medium are holograms A (recording interference between reflected reference light and reflected signal light), holograms, B (recording of interference between incident reference light and reflected signal light), hologram C (recording interference between reflected reference light and incident signal light), hologram D (incident There are four types of recordings where the interference between the reference beam and the incident signal beam is recorded. In addition, the reproduction light obtained from the recording medium during the reproduction process is also reproduced light from the hologram A (read out by the reflected reference light), holo Reproduction light from Gram B (read out with incident reference light), reproduction light from hologram (read out with reflected reference light), reproduction light from hologram D (read out with incident reference light) 4 It is a kind.
このように、 これらの従来技術においては、ホログラム記録層中で全ての光線 Thus, in these prior arts, all the light rays in the hologram recording layer
(参照光の入射光及び反射光と情報光の入射光及び反射光)が干渉するので、複 数のホログラムが記録され再生されてしまう。 このことは、例えば、特開 2 0 0Since (incident reference light and reflected light and information light incident and reflected light) interfere with each other, a plurality of holograms are recorded and reproduced. This is, for example, disclosed in JP
4 - 1 7 1 6 1 1号公報の段落 (0 0 9 6 ) ( 0 0 9 7 ) に記載されているとお りである。 This is as described in paragraph (0 0 9 6) (0 0 9 7) of the publication No. 4-1 7 1 6 11.
従来方法では、反射面を有する記録媒体にホログラムを記録する場合、入射す る参照光と信号光と、反射する参照光と信号光間の 4通.りの干渉によつて 4つの ホログラムが記録されてしまうためにホログラム記録層の性能が無駄に使用さ れていた。 また、 情報の再生時においても、再生光と位相共役再生光が同時に出 現し、 それらが混在したまま、 同じ検出器で検出されるため、再生信号の読み取 り性能が劣化してしまう。 In the conventional method, when a hologram is recorded on a recording medium having a reflecting surface, four holograms are recorded by four-way interference between the incident reference light and signal light and the reflected reference light and signal light. As a result, the performance of the hologram recording layer was wasted. Also, when reproducing information, reproduced light and phase conjugate reproduced light appear simultaneously, and they are mixed and detected by the same detector, so the read performance of the reproduced signal is degraded.
また、参照光と信号光の生成及び合流のために多くの光学部品を要していたの で、 装置の小型化が望まれている。 In addition, since many optical components are required to generate and merge the reference light and signal light, it is desired to reduce the size of the apparatus.
そこで、本発明の解決しょうとする課題には、安定的に記録又は再生を行うこ とを可能にするホログラム記録再生方法及びホログラム装置を提供することが 一例として挙げられる。 Thus, an example of the problem to be solved by the present invention is to provide a hologram recording / reproducing method and a hologram apparatus that enable stable recording or reproduction.
請求項 1記載のホログラム記録装置は、可干渉性の信号光及び参照光による光 学干渉縞を回折格子として内部に保存するホログラム記録層を有する記録媒体 を、前記ホログラム記録層の光照射面の反対側に反射層が位置するよ'うに、装着 自在に保持する支持部と、 The hologram recording apparatus according to claim 1, wherein a recording medium having a hologram recording layer that stores therein optical interference fringes by coherent signal light and reference light as a diffraction grating is provided on a light irradiation surface of the hologram recording layer. Wear so that the reflective layer is located on the opposite side A support part for holding freely;
可干渉性の参照光を発生する光源と、 A light source that generates coherent reference light;
光軸上に配置され記録情報に応じて前記参照光を変調して信号光を生成する 空間光変調器を含む信号光生成部と、 A signal light generation unit including a spatial light modulator that is arranged on the optical axis and generates the signal light by modulating the reference light according to recording information;
前記信号光及び前記参照光を前記ホログラム記録層へ向け照射して、前記ホロ グラム記録層の内部に光干渉縞による回折格子を形成する干渉部と、を有するホ ログラム記録装置であって、 A hologram recording apparatus comprising: an interference unit configured to irradiate the hologram recording layer with the signal light and the reference light to form a diffraction grating by optical interference fringes inside the hologram recording layer;
前記参照光の光路に配置されかつ前記参照光を部分的に遮る回反マスクと、前 記回反マスクと同軸に配置されかつ通過した前記参照光を前記反射層へ集光す る対物レンズと、 を含むことを特徴とする。 An anti-reflective mask disposed in the optical path of the reference light and partially blocking the reference light; an objective lens disposed coaxially with the anti-reflective mask and condensing the reference light that has passed through the reflective layer; It is characterized by including these.
請求項 1 7記載のホログラム再生装置は、参照光及び信号光による光学干渉縞 を回折格子として内部に保存するホログラム記録層を有する記録媒体から情報 を再生するホログラム再生装置であって、 The hologram reproducing device according to claim 17 is a hologram reproducing device for reproducing information from a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
前記記録媒体を、前記ホログラム記録層の光照射面の反対側に反射層が位置す るように、 装着自在に保持する支持部と、 A support unit that holds the recording medium so that the reflective layer is positioned on the opposite side of the light irradiation surface of the hologram recording layer;
可干渉性の参照光を発生する光源と、 A light source that generates coherent reference light;
前記参照光の光路に配置されかつ前記参照光を部分的に遮る前記参照光の光 軸の周りに回反対称な遮光領域及び透光領域からなる回反マスクと、 An anti-reflection mask comprising a light-shielding region and a light-transmitting region which are anti-symmetric about the optical axis of the reference light, which is disposed in the optical path of the reference light and partially blocks the reference light;
前記参照光を前記回反マスク及び前記ホログラム記録層の前記回折格子を透 過するように前記反射層へ集光させて前記回折格子から再生光を生成するとと もに、 前記再生光を受光する対物レンズと、 The reference light is condensed on the reflection layer so as to pass through the anti-reflection mask and the diffraction grating of the hologram recording layer to generate reproduction light from the diffraction grating, and the reproduction light is received. An objective lens;
受光された前記再生光を検出する像センサと、 を含むことを特徴とする。 請求項 2 2記載のホログラム記録方法は、参照光及び信号光による光学干渉縞 を回折格子として内部に保存するホログラム記録層を有する記録媒体へ情報を 記録するホログラム記録方法であつて、 And an image sensor for detecting the received reproduction light. The hologram recording method according to claim 22 is a hologram recording method for recording information on a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
可干渉性の参照光を生成するステップと、 Generating a coherent reference beam;
前記参照光を部分的に遮る前記参照光の光軸の周りに回反対称な遮光領域及 び透光領域からなる回反マスクを、 前記参照光の光路に配置するステップと、 ホログラム記録層の光照射面の反対側に反射層を配置するステップと、 前記参照光を、前記回反マスクの透光領域を通過させかつ対物レンズにより収 束させつつ前記ホログラム記録層を透過するように前記反射層へ照射して前記 反射層で反射せし るステップと、 を含み、 Disposing an anti-reflection mask consisting of a light-shielding region and a light-transmitting region that are anti-symmetric about the optical axis of the reference light, which partially shields the reference light, in the optical path of the reference light; Disposing a reflective layer on the opposite side of the light irradiation surface; and reflecting the reference light so as to pass through the hologram recording layer while passing through the light-transmitting region of the anti-reflection mask and converging by the objective lens. Irradiating the layer and reflecting on the reflective layer, and
前記反射層で反射せしめるステップにおいて、記録情報に応じて前記参照光を 変調して得られた信号光を、前記参照光にて前記ホログラム記録層内で干渉させ て、 回折格子を形成することを特徴とする。 In the step of reflecting on the reflection layer, signal light obtained by modulating the reference light according to recording information is caused to interfere with the reference light in the hologram recording layer to form a diffraction grating. Features.
請求項 2 3記載のホログラム再生方法は、参照光及び信号光による光学干渉縞 を回折格子として内部に保存するホログラム記録層を有する記録媒体から情報 を再生するホログラム再生方法であって、 The hologram reproducing method according to claim 23 is a hologram reproducing method for reproducing information from a recording medium having a hologram recording layer in which optical interference fringes by reference light and signal light are stored as diffraction gratings.
可干渉性の参照光を生成するステップと、 Generating a coherent reference beam;
前記参照光を部分的に遮る前記参照光の光軸の周りに回反対称な遮光領域及 び透光領域からなる回反マスクを、 前記参照光の光路に配置するステップと、 ホログラム記録層の光照射面の反対側に反射層を配置するステップと、 前記参照光を、前記回反マスクの透光領域を通過させかつ対物レンズにより収 束させつつ前記ホ tiグラム記録層を透過するように前記反射層へ照射して前記 回折格子から再生光を生成するステップと、 Disposing an anti-reflection mask consisting of a light-shielding region and a light-transmitting region that are anti-symmetric about the optical axis of the reference light, which partially shields the reference light, in the optical path of the reference light; A step of disposing a reflective layer on the opposite side of the light irradiation surface; and passing through the photogram recording layer while allowing the reference light to pass through the translucent region of the anti-reflection mask and to be converged by the objective lens. Irradiate the reflective layer and Generating reproduction light from the diffraction grating;
前記再生光を前記対物レンズを介して像センサへ導くステップと、を含むこと を特徴とする。 図面の簡単な説明 Guiding the reproduction light to the image sensor through the objective lens. Brief Description of Drawings
図 1及び図 2は、従来のホログラム記録を説明するための光学系及び記録媒体 を示す概略部分断面図である。 1 and 2 are schematic partial cross-sectional views showing an optical system and a recording medium for explaining conventional hologram recording.
図 3は、従来のホログラム記録を説明する記録媒体を示す概略部分断面図であ る。 FIG. 3 is a schematic partial sectional view showing a recording medium for explaining conventional hologram recording.
図 4は、本発明による実施形態の記録再生装置を説明するための光学系及び記 録媒体を示す概略構成図である。 FIG. 4 is a schematic configuration diagram showing an optical system and a recording medium for explaining the recording / reproducing apparatus of the embodiment according to the present invention.
図 5は、本発明による他の実施形態の記録再生装置を説明するための光学系及 び記録媒体を示す概略構成図である。 FIG. 5 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 6は、 本発明による他の実施形態の記録媒体を示す概略部分断面図である。 図 7 A〜 D〜図 1 2は、本発明による実施形態の記録再生装置における回反マ スクを示す正面図である。 FIG. 6 is a schematic partial sectional view showing a recording medium according to another embodiment of the present invention. 7A to 7D are front views showing a reversal mask in the recording / reproducing apparatus according to the embodiment of the present invention.
図 1 3は、本発明による実施形態のホログラム記録再生を説明するための概略 部分断面図である。 FIG. 13 is a schematic partial sectional view for explaining hologram recording / reproduction according to the embodiment of the present invention.
図 1 4は、本発明による実施形態のホログラム記録を説明するための記録媒体 を示す概略部分断面図である。 FIG. 14 is a schematic partial cross-sectional view showing a recording medium for explaining hologram recording of an embodiment according to the present invention.
図 1 5は、本発明による実施形態のホログラム記録再生を説明するための光学 系を示す概略部分'断面図である。 ' 図 1 6 A、 Bは、本発明による他の実施形態の記録再生装置における回反マス クを示す正面図である。 FIG. 15 is a schematic partial sectional view showing an optical system for explaining hologram recording / reproduction according to an embodiment of the present invention. ' FIGS. 16A and 16B are front views showing a reversal mask in a recording / reproducing apparatus according to another embodiment of the present invention.
図 1 7は、本発明による他の実施形態の記録再生装置を説明するための光学系 及び記録媒体を示す概略構成図である。 FIG. 17 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 1 8は、本発明による他の実施形態の記録再生装置における空間光変調器を 示す正面図である。 FIG. 18 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
図 1 9は、本発明による他の実施形態の記録再生装置を説明するための光学系 及び記録媒体を示す概略構成図である。 FIG. 19 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 0は、本発明による他の実施形態の記録再生装置における空間光変調器を 示す正面図である。 FIG. 20 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 1は、本発明による他の実施形態の記録再生装置を説明するための光学系 及び記録媒体を示す概略構成図である。 FIG. 21 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 2は、本発明による他の実施形態の記録再生装置における空間光変調器を 示す正面図である。 FIG. 22 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 3は、本発明による他の実施形態の記録再生装置を説明するための光学系 及び記録媒体を示す概略構成図である。 FIG. 23 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 4は、本発明による他の実施形態の記録再生装置における空間光変調器を. 示す正面図である。 FIG. 24 is a front view showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 5は、本発明による他の実施形態の記録再生装置における液晶素子を示す 部分断面図である。 FIG. 25 is a partial sectional view showing a liquid crystal element in a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 6は、本発明による他の実施形態の記録再生装置における空間光変調器の 光軸から見た正面囟である。 ' 図 2 7は、本発明による他の実施形態の記録再生装置を説明するための光学系 及び記録媒体を示す概略構成図である。 FIG. 26 is a front view as seen from the optical axis of the spatial light modulator in the recording / reproducing apparatus according to another embodiment of the present invention. ' FIG. 27 is a schematic configuration diagram showing an optical system and a recording medium for explaining a recording / reproducing apparatus according to another embodiment of the present invention.
図 2 8 A〜Cは、本発明による他の実施形態の記録再生装置における空間光変 調器を示す正面図である。 発明の詳細な説明 28A to 28C are front views showing a spatial light modulator in a recording / reproducing apparatus according to another embodiment of the present invention. Detailed Description of the Invention
以下に本発明の実施の形態を図面を参照しつつ説明する。 Embodiments of the present invention will be described below with reference to the drawings.
図 4は本実施形態におけるホログラム記録再生装置の光学系の構成例を示す。 ホログラム記録再生装置は、可干渉性の信号光 S B及び参照光 R Bによる光学 干渉縞を回折格子として内部に保存するホログラム記録層 7を有する記録媒体 2を、ホログラム記録層 7の光照射面の反対側に反射層 5が位置するように、装 着自在に保持する支持部(図示せず) を備える。 ホログラム記録再生装置は、 大 きく分けてホログラムの記録及び再生光学系からなり、これらの系は対物レンズ 〇Bを共用して、対物レンズの駆動系やサーボエラ一検出系(図示せず) を含ん でいる。ホログラム記録再生光学系は、ホログラムの記録及び再生用の可干渉性 光を発生するレーザ光源 L D、 コリメ一夕レンズ C L、第 1及び第 2ハーフミラ 一 HM 1及び HM 2、透過型の空間光変調器 S L M、 回反マスク R I M、対物レ ンズ〇B、 結像レンズ ML、 C C D (電荷結合素子) や C MO S (相補型金属酸 化膜半導体装置) などのアレイからなり、 参照光 R Bの光路に配置される。 参照光生成部に属する回反マスク R I Mは、参照光 R Bを部分的に遮る参照光 R Bの光軸の周りに回反対称な遮光領域 S R及び透光領域 T Rからなり、参照光 R Bの光路に配置きれる。 ' 信号光生成部に属する空間光変調器 S L Mは、光軸上に配置され記録情報に応 じて参照光 R Bを変調して信号光 S Bを生成する。透過型の空間光変調器 S L M は、マトリクス状に分割された複数の画素電極を有する液晶パネルなどで電気的 に入射光の一部を画素毎に遮光する機能、又はすベて透過して無変調状態とする 機能を有する。 この空間光変調器 S L Mは空間光変調器駆動回路(図示せず) に 接続され、 これからの記録すべきページデータ(平面上の明暗ドットパターンな どの 2次元データの情報パターン)に基づいた分布を有するように光束を変調か つ透過して、 信号光 S Bを生成する。 FIG. 4 shows a configuration example of the optical system of the hologram recording / reproducing apparatus in the present embodiment. The hologram recording / reproducing apparatus uses a recording medium 2 having a hologram recording layer 7 that stores optical interference fringes as a diffraction grating inside the coherent signal light SB and reference light RB, as opposed to the light irradiation surface of the hologram recording layer 7. A support portion (not shown) that is detachably held is provided so that the reflective layer 5 is positioned on the side. The hologram recording / reproducing apparatus is roughly composed of a hologram recording and reproducing optical system. These systems share the objective lens 0B and include an objective lens drive system and a servo error detection system (not shown). It is out. The hologram recording / reproducing optical system consists of a laser light source LD that generates coherent light for hologram recording and reproduction, a collimator lens CL, first and second half mirrors HM 1 and HM 2, and transmissive spatial light modulation. SLM, anti-reverse mask RIM, objective lens 0B, imaging lens ML, CCD (Charge Coupled Device) and CMOS (Complementary Metal Oxide Semiconductor Device), etc. Placed in. The anti-reverse mask RIM belonging to the reference light generation unit is composed of a light-shielding region SR and a light-transmitting region TR that are anti-symmetric about the optical axis of the reference light RB that partially blocks the reference light RB. I can arrange it. ' The spatial light modulator SLM belonging to the signal light generation unit is arranged on the optical axis and modulates the reference light RB according to the recording information to generate the signal light SB. The transmissive spatial light modulator SLM is a function of electrically shielding a part of incident light for each pixel by a liquid crystal panel having a plurality of pixel electrodes divided in a matrix, or is not transmitted and transmitted. It has a function to make a modulation state. This spatial light modulator SLM is connected to a spatial light modulator driving circuit (not shown), and has a distribution based on the page data to be recorded (information pattern of two-dimensional data such as bright and dark dot patterns on a plane). The signal beam SB is generated by modulating and transmitting the light flux as if it has.
干渉部の対物レンズ O Bは、回反マスク R I Mと同軸に配置されかつ通過する 参照光 R Bを反射層 5へ集光する。対物レンズ O Bは、参照光 R Bが記録媒体の 反射層 5上で収差無くスポットを形成するように設定されている。一方、信号光 S Bは空間光変調器 S L Mの作用を受けているので参照光 R Bより拡がつたス ポットを形成する。 これらの光の干渉縞によって、ホログラム記録層 7の内部に ホログラム (回折格子) が形成される。 The objective lens OB of the interference unit condenses the reference light R B that is disposed coaxially with the anti-reflection mask R I M and passes through the reflection layer 5. The objective lens OB is set so that the reference light RB forms a spot without aberration on the reflection layer 5 of the recording medium. On the other hand, since the signal light S B is subjected to the action of the spatial light modulator S L M, it forms a spot that is wider than the reference light R B. A hologram (diffraction grating) is formed inside the hologram recording layer 7 by the interference fringes of these lights.
図 4の構成例では、光源し Dからのレーザ光は第 1ハ一フミラー HM 1で信号 光 S B及び参照光 R Bの光路に分けられそれぞれ回反マスク R I M及び空間光 変調器 S L Mを経て第 2ハーフミラー HM 2で合流せしめ、ホログラム記録層 7 中で参照光 R Bと重なるように同軸に照射される。 In the configuration example of FIG. 4, the laser light from the light source D is divided into the optical paths of the signal light SB and the reference light RB by the first half mirror HM 1 and the second light passes through the anti-reflection mask RIM and the spatial light modulator SLM, respectively. The beams are merged by the half mirror HM 2 and irradiated coaxially in the hologram recording layer 7 so as to overlap with the reference beam RB.
この他に、 ホログラム記録再生装置は、 図 5に示すように、第 2ハーフミラ一 HM 2を省略して、信号光 S Bはホログラム記録層 7中で参照光 R Bと重なるよ うに参照光 R Bの光路外から照射されるように、構成できる。信号光 S Bと参照 光 R Bの光路が完全に分かれているものであれば、参照光 R Bの光路中のいずれ かの場所に回反マスク R IMを配置することができる。 In addition, the hologram recording / reproducing apparatus omits the second half mirror HM 2 and the optical path of the reference light RB so that the signal light SB overlaps the reference light RB in the hologram recording layer 7 as shown in FIG. It can be configured to be illuminated from the outside. If the optical path of the signal light SB and the reference light RB are completely separated, any of the optical paths of the reference light RB An anti-rotation mask R IM can be placed at some place.
図 6は記録媒体 2の一例を示す。記録媒体 2は、基板 3上にその膜厚方向に積 層された、 反射層 5、 分離層 6、 ホログラム記録層 7及び保護層 8からなる。 な お、 反射層 5をホログラム記録層 7から離して別体で構成してもよい。 FIG. 6 shows an example of the recording medium 2. The recording medium 2 includes a reflective layer 5, a separation layer 6, a hologram recording layer 7, and a protective layer 8 stacked on the substrate 3 in the film thickness direction. Note that the reflective layer 5 may be separated from the hologram recording layer 7 and configured as a separate body.
ホログラム記録層 7には、 例えば、 フォトポリマや、 光異方性材料や、 フォト リフラクティブ材料や、ホールバーニング材料、 フォトクロミック材料など光学 干渉縞を保存できる透光性の光感応 料が用いられる。 For the hologram recording layer 7, for example, a light-transmitting photosensitive material capable of storing optical interference fringes such as a photopolymer, a light anisotropic material, a photorefractive material, a hole burning material, and a photochromic material is used.
上記の各膜を担持する基板 3は、 例えば、 ガラス、 或いはポリカーボネート、 アモルファスポリオレフィン、 ポリイミド、 PET、 PEN, PESなどのブラ スチック、 紫外線硬化型ァクリル樹脂などからなる。 The substrate 3 supporting each of the above films is made of, for example, glass, polycarbonate, amorphous polyolefin, polyimide, PET, PEN, PES or other plastics, UV curable acrylic resin, or the like.
分離層 6及び保護層 8は光透過性材料からなり、積層構造の平坦化や、ホログ ラム記録層などの保護の機能を担う。 The separation layer 6 and the protective layer 8 are made of a light transmissive material, and play a role of flattening the laminated structure and protecting the hologram recording layer and the like.
回反マスク R I Mは、参照光 RBの有効径の光路中に回反対称な明暗パターン Anti-rotation mask R I M is a light-dark pattern that is anti-rotation in the optical path of the effective diameter of reference beam RB.
(光軸周りに 180度回転させると明暗反転したパターンとなる)の遮光領域 S R及び透光領域 TRを有する。すなわち、厳密な回反対称性を有する回反マスク R IMとは、 遮光領域 SR及び透光領域 TRを参照光 RBの光軸の周りに兀It has a light-shielding region SR and a light-transmitting region TR (when the image is rotated 180 degrees around the optical axis, the pattern is inverted from light to dark). In other words, the anti-rotation mask RIM having strict anti-rotation symmetry means that the light shielding region SR and the light transmitting region TR are arranged around the optical axis of the reference light RB.
(2m— 1)だけ回転する回転操作を行なうと前記遮光領域が透光領域に、及び 前記透光領域が遮光領域に重なるようなパターンを有する。ここで、 mは 1, 2, 3, 4, 5, 6などの整数である。 mが大きくなるほど遮光パターンが細かくな り、遮光 Z透光領域の境界での回折効果による影響が生じるので、最大 m=6程 度が好ましい。 When a rotation operation rotating by (2m-1) is performed, the light shielding area has a pattern that overlaps the light transmitting area, and the light transmitting area overlaps the light shielding area. Where m is an integer such as 1, 2, 3, 4, 5, 6. As m increases, the light-shielding pattern becomes finer, and the effect of diffraction effects at the boundary of the light-shielding Z light-transmitting region occurs.
図 7 A〜Dは m== 1の回反対称の回反マスク R I Mの例を示す正 図である。 図 8は m= 2の回反対称の回反マスク R I Mの例を示す正面図である。 7A to 7D are front views showing examples of anti-rotation mask RIM with m == 1. FIG. 8 is a front view showing an example of an antisymmetric anti-rotation mask RIM with m = 2.
図 9は m= 3の回反対称の回反マスク R I Mの例を示す正面図である。 FIG. 9 is a front view showing an example of the anti-rotation mask R I M of m = 3.
図 1 0は m= 4の回反対称の回反マスク R I Mの例を示す正面図である。 FIG. 10 is a front view showing an example of an antisymmetric anti-rotation mask R I M with m = 4.
図 1 1は m= 5の回反対称の回反マスク R I Mの例を示す正面図である。 FIG. 11 is a front view showing an example of an antisymmetric anti-rotation mask R I M with m = 5.
図 1 2は m= 6の回反対称の回反マスク R I Mの例を示す正面図である。 FIG. 12 is a front view showing an example of an antisymmetric anti-rotation mask R I M with m = 6.
ホログラム記録方法は、 図 4に示すように、 光源 L Dが参照光 R Bを生成し、 参照光 R Bの光路に配置された回反マスク R I Mで参照光 R Bを部分的に遮り つつ、回反マスク R I Mの透光領域 T Rを通過させ、対物レンズ O Bにより収束 させて、ホログラム記録層 7を透過するように反射層 5へ照射する。記録情報に 応じて変調された信号光 S Bと、参照光 R Bとをホログラム記録層 7内で干渉さ せ回折格子を形成する。 In the hologram recording method, as shown in FIG. 4, the light source LD generates the reference light RB, and the antireflection mask RIM is partially blocked by the antireflection mask RIM arranged in the optical path of the reference light RB. The reflection layer 5 is irradiated so as to pass through the hologram recording layer 7 through the light transmission region TR, converged by the objective lens OB. The signal light SB modulated according to the recording information and the reference light RB are caused to interfere with each other in the hologram recording layer 7 to form a diffraction grating.
また、ホログラム再生方法では、 レーザ光源 L Dからの射出された発散コヒ一 レント光は、コリメータレンズ C Lで平行光束とされ参照光 R Bとして、ハーフ ミラー HMを経て対物レンズ O Bによって記録媒体 2へ集光される。ホログラム 記録層の回折格子から再生光が生成され、対物レンズ O Bを経て第 3ハーフミラ 一 HM 3で反射される。 再生光は結像レンズ MLで像センサ I S上に結像する。 このように、参照光 R Bの生成から反射層 5への照射まではホ口グラム記録方法 と同様であり、かかる照射により回折格子から再生光を生成して、対物レンズ〇 Bを介して再生光を像センサ I Sへ導き光電変換によって、 情報を再生する。 この実施形態において、記録時と同じ回反マスク R I Mの状態で再生を行えば、 通常再生となる。 In the hologram reproducing method, the divergent coherent light emitted from the laser light source LD is converted into a parallel light beam by the collimator lens CL, and is condensed as the reference light RB on the recording medium 2 by the objective lens OB via the half mirror HM. Is done. Reproduced light is generated from the diffraction grating of the hologram recording layer and is reflected by the third half mirror HM 3 through the objective lens OB. Reproduced light is imaged on the image sensor IS by the imaging lens ML. As described above, the generation of the reference beam RB to the irradiation of the reflective layer 5 is the same as that in the photogram recording method, and the reproduction beam is generated from the diffraction grating by the irradiation, and the reproduction beam is transmitted through the objective lens B. To the image sensor IS to reproduce information by photoelectric conversion. In this embodiment, normal playback is performed if playback is performed with the same anti-reverse mask R I M as during recording.
図 1 3に示すよちに、回反マスク R I Mを参照光光路に置くことに'より、対物 レンズ O Bと反射層 5の光路空間においては、対物レンズ〇Bから反射層 5へ向 かう光(行きの光)か、反射層 5から対物レンズ O Bへ向かう光(帰りの光)か、 のいずれか一方のみが存在することになる。また、回反マスク R I Mとして厳密 な回反対称性を有するものを用いた場合、記録媒体 2の被照射部において、 どち らかの光は必ず存在し、光が照射されない場所はない。 図 1 4に示すように、 入 射参照光と入射信号光間の干渉及び入射参照光と反射信号光間の干渉によるホ ログラムの対 E、或いは、反射参照光と入射信号光間の干渉及び反射参照光と反 射信号光間の干渉によるホログラム対 Fの何れかの対が、記録層 7の場所に依存 して択一的に記録されることになる。 As shown in Fig.13, the objective is selected by placing the anti-reverse mask RIM in the reference beam path. In the optical path space between the lens OB and the reflective layer 5, either the light from the objective lens B to the reflective layer 5 (bound light) or the light from the reflective layer 5 to the objective lens OB (return light) Only one of them will exist. Further, when the anti-rotation mask RIM having a strict anti-rotation symmetry is used, either light is always present in the irradiated portion of the recording medium 2, and there is no place where the light is not irradiated. As shown in Fig. 14, the hologram pair E due to interference between the incident reference light and the incident signal light and interference between the incident reference light and the reflected signal light, or interference between the reflected reference light and the incident signal light, and Depending on the location of the recording layer 7, any pair of hologram pairs F due to interference between the reflected reference light and the reflected signal light is recorded alternatively.
このように回反マスク R I Mを置くことにより、 ホログラムが 2つ (無駄に) 記録されるという問題点が解決される。 By placing the anti-rotation mask R I M in this way, the problem of recording two holograms (uselessly) is solved.
再生時にも同じように回反マスク R I Mを置けば、ホログラムを記録したとき と全く同じ参照光 R Bを照射することになるため通常再生光のみが現れ、位相共 役再生光が現れることはない。 If the anti-reflection mask RIM is placed in the same way during reproduction, the same reference light RB as that when the hologram is recorded is irradiated, so that only normal reproduction light appears, and phase-shared reproduction light does not appear.
他の実施形態では、図 4に示す回反マスク R I Mの遮光領域 S R及び透光領域 T Rを反転あるいは光軸周りに 1 8 0度回転する反転手段 I N Vを設けて、記録 時と明暗パターン(回反マスク R I Mの遮光領域 S R及び透光領域 T R)を反転 させ、 あるいは光軸周りに 1 8 0度回転させた状態で再生すれば、位相共役再生 となる。再生時に通常再生と位相共役再生を切り替えて選択することが可能であ るとともに、 2つの再生光が同時に像センサ I Sに戻ることを防止できる。 回反マスク R I Mは固定式の板状体で構成できるが、これを透過型の液晶素子 から構成して、記^時に液晶素子が遮光領域 S R及び透光領域 T Rを ¾示する状 態であるように制御することもできる。 In another embodiment, the light shielding region SR and the light transmitting region TR of the anti-rotation mask RIM shown in FIG. 4 are provided with inversion means INV that inverts or rotates 180 degrees around the optical axis, so Phase conjugation reproduction can be achieved by reversing the light-blocking region SR and the light-transmitting region TR) of the anti-mask RIM or by rotating it 180 degrees around the optical axis. During playback, it is possible to switch between normal playback and phase conjugate playback and to prevent two playback lights from returning to the image sensor IS at the same time. The anti-rotation mask RIM can be composed of a fixed plate-like body, but this is composed of a transmissive liquid crystal element, and at the time of writing, the liquid crystal element shows a light shielding region SR and a light transmissive region TR. It can also be controlled to be in a state.
図 1 5に示すように、回反マスク R I Mを記録時状態から 1 8 0度回転させた 状態(明暗を反転させた状態)では、対物レンズ〇Bと反射層 5の間の全ての場 所で、 参照光 の向きが反転している。 今まで「行きの光」 があったところに は 「帰りの光」 が、 「帰りの光」 があったところには 「行きの光」 が存在してい る。 この状態で再生を行うと、位相共役再生光のみが現れ、通常再生光が現れる ことはない。また、反転手段により回反マスク R I Mを再生時に 2つの状態で切 り替えることにより、 通常再生か位相共役再生かを選択することができる。 仮に対物レンズ O Bが理想レンズ(たとえばフーリエ変換レンズ)であれば空 間光変調器のページデータ上の一点から出た光線は、像センサ I Sの像面上の一 点に結像する。 しかし、実際の対物レンズではレンズの収差や MT F特性の影響 を受けるため、像のぼけが生じる。 これは対物レンズ O Bの開口数 NAが大きい 場合や、像高(ぺ一ジデ一夕のドットの光軸からの距離)が大きい場合にはさら に顕著である。 As shown in Fig. 15, when the anti-rotation mask RIM is rotated 180 degrees from the recording state (in which light and dark are reversed), all locations between the objective lens B and the reflective layer 5 are shown. The direction of the reference beam is reversed. Where there has been a “light for going”, there is a “light for return” and where there has been a “light for return” there is “light for going”. When reproduction is performed in this state, only phase conjugate reproduction light appears, and normal reproduction light does not appear. In addition, it is possible to select normal reproduction or phase conjugate reproduction by switching the anti-reflection mask R I M in two states during reproduction by the inversion means. If the objective lens OB is an ideal lens (for example, a Fourier transform lens), a light beam emitted from a point on the page data of the spatial light modulator forms an image on a point on the image plane of the image sensor IS. However, an actual objective lens is affected by lens aberration and MTF characteristics, resulting in image blurring. This is even more conspicuous when the numerical aperture NA of the objective lens OB is large or when the image height (distance from the optical axis of the dot on the page) is large.
空間光変調器 S L Mのパターンをホログラムとして記録する場合、空間光変調 器 S L Mのパターンがページデータに相当する。 この場合、対物レンズ O Bと反 射層 5の間で参照光 R Bと干渉させてホログラムを形成する。その再生光は、元 の場所にページデ一夕があるかのごとく出現するので、再生光の光路は記録時の 実際の対物レンズの場合と同じとなり、対物レンズ〇 Bの収差や M T Fの影響を 受けた、 像センサ I Sの上ではぼやけた像となる。 When the pattern of the spatial light modulator SLM is recorded as a hologram, the pattern of the spatial light modulator SLM corresponds to page data. In this case, a hologram is formed by interfering with the reference light RB between the objective lens OB and the reflecting layer 5. Since the reproduced light appears as if there is a page dew in the original location, the optical path of the reproduced light is the same as that of the actual objective lens during recording, and the influence of the aberration of the objective lens B and the MTF is affected. The received image is blurred on the image sensor IS.
これに対して位相共役再生では、再生光は元の信号光 S Bの光路を逆戻りする ように出現する。 とのため、対物レンズ〇Bの性能などにかかわらず元のページ データと同じ像を形成することができる。よって、使用する対物レンズ O Bの N Aが大きい場合や、空間光変調器 S L Mのパターンが大きくて像高が大きい部分 も存在するような場合、位相共役再生を用いることで、対物レンズ〇Bの性能の 制約を受けずに良好な再生像を得られる。但し、通常再生光に比べて位相共役再 生光は S N比が劣るため、良好な S N比での再生を望むのであれば通常再生光の みを使用することが好ましい。 S N比をとるか、結像性能をとるかの仕様で、通 常再生か位相共役再生かを選ぶことができる。 On the other hand, in the phase conjugate reproduction, the reproduced light appears so as to return back to the optical path of the original signal light SB. Therefore, the original page regardless of the performance of the objective lens 〇B The same image as the data can be formed. Therefore, if the NA of the objective lens OB to be used is large, or if there is a part where the spatial light modulator SLM has a large pattern and a large image height, the performance of the objective lens 0B can be improved by using phase conjugate reproduction. Good reproduction images can be obtained without any restrictions. However, since the phase conjugate reproduction light is inferior to the normal reproduction light in the SN ratio, it is preferable to use only the normal reproduction light if reproduction with a good SN ratio is desired. You can choose between normal playback and phase-conjugate playback depending on whether you want the SN ratio or imaging performance.
なお、上述の説明から明らかであるように、回反マスク R I Mの形状が厳密な 回反対称でなく、図 1 6 Aに例示したような遮光領域 S Rが透光領域 T Rより面 積が多少小さい回反対称に準ずる形状(準回反対称) であっても、媒体中におい て 「行きの参照光」 と 「帰りの参照光」 が同時に存在する領域を大幅に減ずるこ とができるので、余分なホログラムの影響を低減するという本願発明の効果が得 られる。また、図 1 6 Bに例示したような遮光領域 S Rが透光領域 T Rより面積 が多少大きい形状とした場合は、媒体中に参照光が全く存在しない領域が生ずる が、 「行きの参照光」 と 「帰りの参照光」 のいずれか一方のみ存在する状況を実 現することができ、 やはり本願発明の効果が得られる。 よって、 回反マスク R I Mの形状では厳密に遮光領域 S R及び透光領域 T Rの面積が等しいだけでなぐ それらの面積は、媒体中における入射光及び反射光の光路の制限すれば、増減さ せることができる。 As is clear from the above description, the shape of the anti-rotation mask RIM is not strictly anti-rotation-symmetric, and the shading area SR illustrated in FIG. 16A has a slightly smaller area than the translucent area TR. Even if the shape conforms to anti-rotation symmetry (quasi-anti-anti-symmetry), it is possible to greatly reduce the area where “bound reference light” and “return reference light” exist simultaneously in the medium. The effect of the present invention to reduce the influence of a simple hologram can be obtained. In addition, when the light-shielding region SR illustrated in Fig. 16B has a slightly larger area than the light-transmitting region TR, a region where no reference light exists in the medium is generated. And “returning reference beam” can be realized, and the effect of the present invention can be obtained. Therefore, in the shape of the anti-rotation mask RIM, the areas of the light-shielding region SR and the light-transmitting region TR are strictly equal, and these areas can be increased or decreased if the optical paths of incident light and reflected light in the medium are limited. Can do.
他の実施形態としては、 以下のものがある。 Other embodiments include the following.
例えば、図 1 7に示すように、光源 L Dからのレーザ光束の外周部分のみを変 調して、外周部を信号光 S B、光軸上の内周部を無変調の参照光 R Bとすること ができる。 この場合、 図 18に示すように、 空間光変調器 SLMを、 参照光 RB を無変調で通過させる光軸上に配置された透過中央領域 T C Rと、透過中央領域 T C Rの周囲に配置されかつ記録情報に応じて参照光 R Bを変調して参照光 R Bから空間的に分離された信号光 S Bを生成する透過型のマトリクス液晶装置 からなる空間光変調環状領域 SLMRRと、 から構成する。 この形態では、光軸 及びその近傍が参照光 RBとなるので、いずれかの場所に、信号光 s こ影響を 与えないように内周部だけに作用する回反マスク R IMを配置すればよい。すな わち、回反マスク R IMは、信号光 SBを遮らずに透過中央領域 TCRを通過す る参照光 RBのみを部分的に遮るように、配置される。 また、透過中央領域 TC Rは貫通開口又は透明材料から構成できる。さらに、透過中央領域 TCRは透過 型の液晶素子から構成して、記録時に液晶素子が透光状態であるように制御する。 一方、図 19のように、空間光変調器 SLMと回反マスク R IMを一体で形成 し、 他は図 17の例と同一に構成してもよい。 この場合、 図 20に示すように、 空間光変調器 SLMは、回反マスク R I Mとしての中央マスク領域 CMRと、 中 央マスク領域 CMRの周囲に配置されかつ記録情報に応じて参照光 RBを変調 して参照光 RBから空間的に分離された信号光 S Bを生成する透過型のマトリ クス液晶装置からなる空間光変調環状領域 SLMRRと、からなる。中央マスク 領域 C M Rは固定式の板状体で構成できるが、中央マスク領域 C M Rは透過型の 液晶素子から構成して、記録時に液晶素子が遮光領域 S R及び透光領域 T Rを表 示する状態であるように制御することもできる。 For example, as shown in FIG. 17, only the outer peripheral part of the laser beam from the light source LD is modulated so that the outer peripheral part is signal light SB and the inner peripheral part on the optical axis is unmodulated reference light RB. Can do. In this case, as shown in FIG. 18, the spatial light modulator SLM is arranged around the transmission central region TCR arranged on the optical axis that allows the reference light RB to pass through without modulation, and around the transmission central region TCR. A spatial light modulation annular region SLMRR composed of a transmissive matrix liquid crystal device that modulates the reference light RB according to information and generates the signal light SB spatially separated from the reference light RB. In this embodiment, since the optical axis and the vicinity thereof become the reference light RB, the anti-reflection mask RIM that acts only on the inner periphery may be disposed at any location so as not to affect the signal light s. . In other words, the anti-reflection mask RIM is arranged so as to partially block only the reference light RB passing through the transmission central region TCR without blocking the signal light SB. Further, the transmission central region TCR can be formed of a through opening or a transparent material. Further, the transmissive central region TCR is composed of a transmissive liquid crystal element, and is controlled so that the liquid crystal element is in a translucent state during recording. On the other hand, as shown in FIG. 19, the spatial light modulator SLM and the anti-rotation mask RIM may be integrally formed, and the other configuration may be the same as the example of FIG. In this case, as shown in FIG. 20, the spatial light modulator SLM is arranged around the central mask region CMR as the anti-rotation mask RIM and the central mask region CMR and modulates the reference light RB according to the recording information. And a spatial light modulation annular region SLMRR composed of a transmissive matrix liquid crystal device that generates signal light SB spatially separated from the reference light RB. The central mask area CMR can be composed of a fixed plate, but the central mask area CMR is composed of a transmissive liquid crystal element, and the liquid crystal element displays the light shielding area SR and the translucent area TR during recording. It can also be controlled as is.
図 17及び図 19の例とは逆に内周部が信号光 S B、外周部が参照光 RBとな る構成も採用できる。例えば、 図 21に示すように、光源 LDからのレーザ光束 の内周部分のみを変調して、内周部を信号光 SB、外周部を無変調の参照光 RB とすることができる。 この場合、 図 22に示すように、 空間光変調器 SLMは、 記録情報に応じて参照光 R Bを変調して通過させ信号光 S Bを生成する光軸上 に配置された透過型のマトリクス液晶装置からなる空間光変調中央領域 S LM C Rと、空間光変調中央領域 S LMC Rの周囲に配置されかつ参照光 RBを無変 調で通過させ信号光 S Bから空間的に分離する透過環状領域 T R Rと、から構成 する。回反マスク R IMは、信号光 SBを遮らずに透過環状領域 TRRを通過す る参照光 RBのみを部分的に遮るように、配置される。透過環状領域 TRRは貫 通開口又は透明材料からなる。さらに、透過環状領域 TRRは透過型の液晶素子 から構成して、記録時に液晶素子が透光状態であるように制御することもできる。 また、図 23のように、空間光変調器 SLMと回反マスク R IMを一体で形成 し、 他は図 21の例と同一に構成してもよい。 この場合、 図 24に示すように、 空間光変調器 S LMは、記録情報に応じて参照光 R Bを変調して通過させ信号光 S Bを生成する光軸上に配置された透過型のマトリクス液晶装置からなる空間 光変調中央領域 S L M C Rと、空間光変調中央領域 SLMCRの周囲に配置され た回反マスク R IMとしての環状マスク領域 RMRと、からなる。環状マスク領 域 RMRは透過型の液晶素子からなり、記録時に液晶素子が環状マスク領域 RM Rが遮光領域 S R及び透光領域 TRを表示する状態である。 Contrary to the examples of FIGS. 17 and 19, a configuration in which the inner peripheral portion is the signal light SB and the outer peripheral portion is the reference light RB can be employed. For example, as shown in Fig. 21, the laser beam from the light source LD Only the inner peripheral part of the signal can be modulated so that the inner peripheral part is the signal light SB and the outer peripheral part is the unmodulated reference light RB. In this case, as shown in FIG. 22, the spatial light modulator SLM is a transmissive matrix liquid crystal device arranged on the optical axis that modulates the reference light RB in accordance with the recording information and generates the signal light SB. Spatial light modulation central region SLM CR consisting of and a transmission annular region TRR arranged around the spatial light modulation central region S LMC R and spatially separated from the signal light SB through the reference light RB without modulation. Consists of. The anti-rotation mask RIM is arranged so as to partially block only the reference light RB passing through the transmission annular region TRR without blocking the signal light SB. The transmissive annular region TRR consists of a through-opening or a transparent material. Further, the transmissive annular region TRR can be constituted by a transmissive liquid crystal element and can be controlled so that the liquid crystal element is in a light-transmitting state during recording. Further, as shown in FIG. 23, the spatial light modulator SLM and the anti-rotation mask RIM may be integrally formed, and the other configuration may be the same as the example of FIG. In this case, as shown in FIG. 24, the spatial light modulator SLM modulates the reference light RB in accordance with the recording information and passes it to generate a transmission light matrix liquid crystal disposed on the optical axis. It consists of a spatial light modulation central region SLMCR consisting of a device and an annular mask region RMR as a reversal mask RIM arranged around the spatial light modulation central region SLMCR. The annular mask area RMR is composed of a transmissive liquid crystal element, and the liquid crystal element is in a state where the annular mask area RM R displays the light shielding area SR and the light transmitting area TR during recording.
図 25に示すように、空間光変調器 SLMや、回反マスク R IM—体型空間光 変調器 SLMの液晶装置部分は透過型の液晶素子からなり、 これらは、対向する 1対の偏光板 80 a, 80 b間のそれぞれの内面に順に形成された透明電極 81 a, 81 b及び配向膜 82 a, 82 bにて、 挟持された液晶層 83 ( 晶分子の 層)からなる。透明電極 8 1 a , 8 1 bは回反マスク R I Mの形状に応じた 1種 類以上の 1対の電極形状とする。 また、 図 2 6に示すように、 空間光変調器 S L M全体を透過型マトリクス液晶装置として、その制御回路 2 6により、所定パタ ーン表示、例えば内部の中央領域 A及びその外周に外周領域 Bにそれぞれ回反マ スク領域及びページ.データ領域などを表示するように、 構成することもできる。 再生時に通常再生と位相共役再生を切り替えるのに回反マスク R I Mを光軸 周りに 1 8 0度回転させるが、液晶素子を用いると、電気的な切り替えのみで同 様の効果が得られる。 As shown in FIG. 25, the liquid crystal device portion of the spatial light modulator SLM or anti-rotation mask RIM—body-type spatial light modulator SLM is composed of a transmissive liquid crystal element, which consists of a pair of opposing polarizing plates 80 liquid crystal layer 83 (crystal molecules) sandwiched between transparent electrodes 81 a and 81 b and alignment films 82 a and 82 b sequentially formed on the inner surfaces of a and 80 b. Layer). The transparent electrodes 8 1 a and 8 1 b have one or more pairs of electrode shapes according to the shape of the anti-rotation mask RIM. As shown in FIG. 26, the spatial light modulator SLM as a whole is a transmissive matrix liquid crystal device, and its control circuit 26 displays a predetermined pattern, for example, an inner central region A and an outer peripheral region B on its outer periphery. Each can also be configured to display an anti-reflection mask area and a page data area. To switch between normal playback and phase conjugate playback during playback, the anti-rotation mask RIM is rotated 180 degrees around the optical axis. If a liquid crystal element is used, the same effect can be obtained only by electrical switching.
液晶分子は電圧を印加した部分のみ光の偏光面を回転させる(旋光)性質があ る。 偏光面の回転量は液晶層の厚さや印加電圧の大きさによって変化する。 透明電極 8 1 a , 8 1 b間に電圧を印加した部分の偏光が 9 0度回転するよう に設定されているとする。偏光板 8 0 aを通過した光の偏光状態が、紙面に平行 な直線偏光 (A偏光と呼ぶこととする) であるとする。 Liquid crystal molecules have the property of rotating the polarization plane of light (rotation) only at the part where voltage is applied. The amount of rotation of the polarization plane varies depending on the thickness of the liquid crystal layer and the magnitude of the applied voltage. It is assumed that the polarization of the portion where voltage is applied between the transparent electrodes 8 1 a and 8 1 b is set to rotate 90 degrees. It is assumed that the polarization state of the light passing through the polarizing plate 80 a is linearly polarized light (referred to as A-polarized light) parallel to the paper surface.
偏光板 8 0 aは A偏光のみを通過させる偏光板であり、偏光板 8 0 bも同様で ある。 The polarizing plate 80 a is a polarizing plate that allows only the A polarized light to pass therethrough, and the polarizing plate 80 b is the same.
液晶層 8 3には或る電極対だけ電圧が印加してあり、この部分を通過した光だ け偏光面が 9 0度回転し、紙面に垂直な直線偏光(B偏光と呼ぶこととする) と なる。 A voltage is applied to the liquid crystal layer 83 only by a certain electrode pair, and the polarization plane is rotated by 90 degrees only for the light passing through this portion, and linearly polarized light perpendicular to the paper surface (referred to as B-polarized light). It becomes.
その後に対向する偏光板 8 0 bは、 A偏光のみを通過させるので、他の電極対 の光だけ通過し、 そのほかの光は遮断される。 Since the polarizing plate 80 b facing thereafter passes only the A-polarized light, only the light from the other electrode pair passes, and the other light is blocked.
この液晶素子全体としては、電圧を印加した部分だけ遮光される回反マスク R I Mとして作用す ¾。 ' 例えば、図 7 Cのパターンの回反マスク R IMを液晶で実現するとすれば、電 極パターンを白抜き及び斜線部分に相当する部分とし、斜線部分のみに電圧を印 加することにより、 図の斜線部分が遮光領域 S Rとなる。 The liquid crystal element as a whole acts as an anti-rotation mask RIM that shields light only from a portion to which a voltage is applied. ' For example, if the anti-reverse mask RIM of the pattern in Fig. 7C is realized with liquid crystal, the electrode pattern is made to correspond to the white and shaded portions, and voltage is applied only to the shaded portions. The shaded area is the light shielding region SR.
再生時、通常再生と、位相共役再生を切り替えるために、 この回反マスク R I M全体を 180度回転させる代わりに、白抜きの部分に電圧を印加し斜線部分に 電圧を印加しないようにすることにより、斜線部は透光状態、その他の部分が遮 光状態となり、光学的には回反マスク R IM全体を光軸を中心に 180度回した のと同じことになる。 なお、 入射する側の偏光板(この例では偏光板 80 a) は 無くてもよい。さらに、偏光板を光軸周りに 90度回転させた配置にすることに より、 電圧をかけた部分だけ透過(そのほかは遮光) とすることもできる。 この ように、物理的に回反マスク R IMを回転させることなく、電気的な切り替えの みで同様の効果が得られる。 In order to switch between normal playback and phase conjugate playback during playback, instead of rotating the anti-reverse mask RIM by 180 degrees, a voltage is applied to the white area and no voltage is applied to the shaded area. The shaded area is translucent and the other areas are light-shielded. Optically, this is the same as turning the entire anti-rotation mask RIM 180 degrees around the optical axis. The incident side polarizing plate (in this example, polarizing plate 80a) may be omitted. Furthermore, by arranging the polarizing plate to rotate 90 degrees around the optical axis, it is possible to transmit only the part to which voltage is applied (the other part is shielded). In this way, the same effect can be obtained only by electrical switching without physically rotating the anti-rotation mask RIM.
更なる他の実施形態においては、図 17〜図 24に示す実施形態(光源 LDか らのレーザ光束有効径の内外周で信号光 S B及び参照光 R Bを光軸に沿って分 けて伝搬する構成)ではなく、 図 27に示すように、光軸から見て第 1〜第 4象 限に光束を分割した回反マスク一体型空間光変調器 QSLMで生成する構成も 可能である。 図 28Aに示すように、 記録時には、 第 1、 第 3象限 Ql, Q3に て記録情報に応じて参照光 RBを変調するページデータパターンを表示する状 態で信号光 SBを生成し、 第 2、 第 4象限 Q2, Q4を参照光 RBに用いる (た だし第 2象限 Q 2は遮光状態)。 このとき、 参照光 RBに対応する第 2、 第 4象 限 Q2, Q 4が回反対称になる。 図 28 Bに示すように、再生時は第 1〜第 3象 限 Q1〜Q3を遮光して、参照光を記録時と同じ透光状態(第 4象限 Q4) とし て通常再生でき、 又は、 図 2 8 Cに示すように、 記録時と明暗が反転(第 4象限 Q 4が遮光、 第 2象限が透光の状態) とすることで位相共役再生が可能となる。 以上、本実施形態によれば、 ホログラム記録時には、信号光 S Bと干渉するの は行きの参照光か反射された参照光のいずれか一方のみであるため、余分なホロ グラムが記録されることがない。 また、再生時においては、通常再生と位相共役 再生のどちらか一方のみを行うことが出来、通常再生光と位相共役再生光が検出 器上で混在することがないため、 良好な再生を行うことが出来る。 In still another embodiment, the embodiment shown in FIGS. 17 to 24 (the signal light SB and the reference light RB are propagated separately along the optical axis at the inner and outer circumferences of the effective diameter of the laser beam from the light source LD. As shown in Fig. 27, it is possible to use a QSLM with an anti-reverse mask integrated spatial light modulator that divides the luminous flux into the first to fourth quadrants as viewed from the optical axis. As shown in FIG. 28A, during recording, signal light SB is generated in a state in which a page data pattern for modulating the reference light RB is displayed in the first and third quadrants Ql and Q3 according to the recording information. The fourth quadrant Q2 and Q4 are used as the reference beam RB (however, the second quadrant Q2 is shielded). At this time, the second and fourth quadrants Q2 and Q4 corresponding to the reference beam RB become antisymmetric. As shown in Figure 28B, during playback, the first to third quadrants Q1 to Q3 are shielded, and the reference light is in the same light transmission state (fourth quadrant Q4) as during recording. As shown in Fig. 28 C, phase conjugate reproduction is possible by reversing the brightness and darkness during recording (fourth quadrant Q4 is light-shielded and second quadrant is translucent). Become. As described above, according to the present embodiment, at the time of hologram recording, only one of the outgoing reference light and the reflected reference light interferes with the signal light SB, and therefore an extra hologram can be recorded. Absent. Also, during reproduction, only normal reproduction or phase conjugate reproduction can be performed, and normal reproduction light and phase conjugate reproduction light are not mixed on the detector, so that good reproduction can be performed. I can do it.
Claims
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| WO2008126301A1 (en) * | 2007-03-30 | 2008-10-23 | Pioneer Corporation | Hologram recorder/reproducer |
| JPWO2009025024A1 (en) * | 2007-08-20 | 2010-11-18 | 富士通株式会社 | Hologram recording device |
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| WO2004102542A1 (en) * | 2003-05-13 | 2004-11-25 | Optware Corporation | Optical information recording/reproduction device and method |
| JP2004361928A (en) * | 2003-05-13 | 2004-12-24 | Optware:Kk | Optical information recording method, optical information recording device, and optical information recording / reproducing device |
| JP2005031212A (en) * | 2003-07-08 | 2005-02-03 | Optware:Kk | Optical information reproducing apparatus and optical information storage / reproducing apparatus |
-
2006
- 2006-04-13 WO PCT/JP2006/308261 patent/WO2006118036A1/en not_active Ceased
- 2006-04-13 JP JP2007514634A patent/JPWO2006118036A1/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2000338846A (en) * | 1999-05-25 | 2000-12-08 | Sony Corp | Hologram recording / reproducing device |
| WO2004102542A1 (en) * | 2003-05-13 | 2004-11-25 | Optware Corporation | Optical information recording/reproduction device and method |
| JP2004361928A (en) * | 2003-05-13 | 2004-12-24 | Optware:Kk | Optical information recording method, optical information recording device, and optical information recording / reproducing device |
| JP2005031212A (en) * | 2003-07-08 | 2005-02-03 | Optware:Kk | Optical information reproducing apparatus and optical information storage / reproducing apparatus |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2008126301A1 (en) * | 2007-03-30 | 2008-10-23 | Pioneer Corporation | Hologram recorder/reproducer |
| JPWO2008126301A1 (en) * | 2007-03-30 | 2010-07-22 | パイオニア株式会社 | Hologram recording / reproducing device |
| JPWO2009025024A1 (en) * | 2007-08-20 | 2010-11-18 | 富士通株式会社 | Hologram recording device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPWO2006118036A1 (en) | 2008-12-18 |
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