This is a Continuation of application Ser. No. 10/433,644 filed on Oct. 9, 2003 which is a U.S. National Stage Application of International Application No. PCT/JP01/10681 filed on Dec. 6, 2001. The entire disclosures of the prior applications are hereby incorporated by reference herein in their entirety.
BACKGROUND The present invention relates to an optical information recording apparatus and method for recording information in each information recording area of a recording medium having a plurality of information recording areas through the use of holography.
In general, holographic recording for recording information in a recording medium through the use of holography is performed by superimposing light that carries image information on reference light within the recording medium and by writing a resultingly generated interference pattern into the recording medium. For reproducing the information recorded, the recording medium is irradiated with reference light such that the image information is reproduced through diffraction derived from the interference pattern.
In recent years, volume holography, or digital volume holography in particular, has been developed and is attracting attention in practical fields for ultra-high density optical recording. Volume holography is a method for writing a three-dimensional interference pattern by making positive use of a recording medium in a direction of its thickness as well, and is characterized in that it is possible to enhance the diffraction efficiency by increasing the thickness of the medium, and a greater recording capacity can be achieved by employing multiplex recording. Digital volume holography is a computer-oriented holographic recording method which uses the same recording medium and recording method as with the volume holography, whereas the image information to be recorded is limited to binary digital patterns. In the digital volume holography, analog image information such as a picture is once digitized and developed into two-dimensional digital pattern information, and then it is recorded as image information. For reproduction, this digital pattern information is read and decoded to restore the original image information for display. Consequently, even if the signal-to-noise ratio (hereinafter referred to as SN ratio) during reproduction is somewhat poor, it is possible reproduce the original information with extremely high fidelity by performing differential detection and/or error correction on the binary data encoded.
By the way, typical recording apparatuses that record information on a disk-shaped recording medium through the use of light comprise an optical head for irradiating the recording medium with light for information recording. In these recording apparatuses, the recording medium is rotated while the optical head irradiates the recording medium with the light for information recording, thereby recording information on the recording medium. In these recording apparatuses, a semiconductor laser is typically used as the light source for generating the light for information recording.
For holographic recording, as in the typical recording apparatuses described above, the recording medium can also be rotated while the recording medium is irradiated with information light and reference light so that information is recorded in a plurality of information recording areas of the recording medium in succession. In this case, as with the typical recording apparatuses, a practical semiconductor laser is desirably used as the light source of the information light and the reference light.
When existing photosensitive material for holography is used to make a recording medium for holographic recording and this recording medium is rotated while the recording medium is irradiated with the information light and the reference light that are generated by a semiconductor laser, however, there arises a problem as follows. That is, in this case, it is difficult to give exposure energy sufficient to record information in the form of an interference pattern to a single information recording area of the recording medium in a short time. To cope with this, the exposure time may be extended to give sufficient exposure energy to a single information recording area. Nevertheless, this can increase the moving distance of the information recording areas within the exposure time for a single information recording area, resulting in deterioration in information accuracy.
Here, the forgoing problem will be detailed with a concrete example. If a high-power light source such as a pulse laser is used as the light source instead of a semiconductor laser, then it is satisfactorily possible to record information on the recording medium while rotating the recording medium. Take, for example, the case where a pulse laser which has a maximum power of several kilowatts and is capable of generating pulsed light of several tens of nanoseconds is used as the light source. Here, assume the light intensity on the recording medium to be 200 W. The pulse width of the pulsed light shall be 20 ns, and the linear speed of the information recording areas 2 m/s. In this case, the moving distance of the information recording areas within the exposure time for a single information recording area is 0.04 μm, not exceeding one tenth of the wavelength of the light, so that it is possible to maintain sufficient information accuracy. The use of such a pulse laser as described above for the light source is impractical, however.
Next, turn to the case where a semiconductor laser is used as the light source. Here, assume that the light intensity on the recording medium is 20 mW and the linear speed of the information recording areas is 2 m/s. In this case, an exposure time of 200 Vs, or 10000 times as much as with the foregoing pulse laser, is required in order to give a single information recording area the same amount of exposure energy as with the pulse laser. The moving distance of the information recording areas for this exposure time reaches 400 μm, making it difficult to record information in the form of interference patterns.
SUMMARY It is an object of the invention to provide an optical information recording apparatus and method in which a practical light source can be used to record information in each information recording area of a recording medium having a plurality of information recording areas through the use of holography while moving the recording medium.
An optical information recording apparatus of the invention is an apparatus for recording information through the use of holography in each information recording area of a recording medium having a plurality of information recording areas. The apparatus comprises:
an irradiating device for irradiating the recording medium with information light and reference light such that information is recorded in the information recording areas in the form of interference patterns resulting from interference between the information light and the reference light;
a recording medium moving device for moving the recording medium; and
an irradiating position moving device for moving an irradiating position of the information light and the reference light such that the irradiating position of the information light and the reference light follows a single moving information recording area for a predetermined period.
In the optical information recording apparatus of the invention, the recording medium moving device moves the recording medium, and the irradiating device irradiates this recording medium with the information light and the reference light. The irradiating position moving device moves the irradiating position of the information light and the reference light such that the irradiating position of the information light and the reference light follows a single moving information recording area for a predetermined period. Consequently, the single information recording area keeps being irradiated with the information light and the reference light for the predetermined period. It is therefore possible to irradiate the information recording areas with the information light and the reference light for a sufficient time period to record information in the information recording areas without causing a deviation between the information recording areas and the irradiating position of the information light and the reference light.
In the optical information recording apparatus of the invention, the recording medium moving device may rotate the recording medium.
In the optical information recording apparatus of the invention, the irradiating position moving device may move the position of emission of the information light and the reference light in the irradiating device.
In the optical information recording apparatus of the invention, the recording medium may contain identification information for identifying the individual information recording areas, and the optical information recording apparatus may further comprise a detector for detecting the identification information.
In the optical information recording apparatus of the invention, the recording medium may contain positioning information for adjusting the irradiating position of the information light and the reference light with respect to the individual information recording areas, and the optical information recording apparatus may further comprise a detector for detecting the positioning information.
In the optical information recording apparatus of the invention, the irradiating device may apply the information light and the reference light to the same side of the information recording area coaxially such that they converge to become minimum in diameter at an identical position.
In the optical information recording apparatus of the invention, the irradiating device may apply the information light and the reference light to opposite sides of the information recording area coaxially such that they converge to become minimum in diameter at an identical position.
An optical information recording method of the invention is a method for recording information through the use of holography in each information recording area of a recording medium having a plurality of information recording areas. The method comprises the steps of:
moving the recording medium;
irradiating the recording medium with information light and reference light such that information is recorded in the information recording areas in the form of interference patterns resulting from interference between the information light and the reference light; and
moving an irradiating position of the information light and the reference light such that the irradiating position of the information light and the reference light follows a single moving information recording area for a predetermined period.
In the optical information recording method of the invention, the information light and the reference light are applied to the recording medium while it is moving. In the step of moving the irradiating position, the irradiating position of the information light and the reference light is moved to follow a single moving information recording area for a predetermined period. Consequently, the single information recording area keeps being irradiated with the information light and the reference light for the predetermined period. It is therefore possible to irradiate the information recording areas with the information light and the reference light for a sufficient time period to record information in the information recording areas without causing a deviation between the information recording areas and the irradiating position of the information light and the reference light.
Other objects, features and advantages of the invention will become sufficiently clear from the following description.
BRIEF DESCRIPTION OF THE DRAWINGSFIG. 1 is an explanatory diagram showing a recording medium used in a first embodiment of the invention.
FIG. 2 is a block diagram showing a configuration of an optical information recording/reproducing apparatus according to the first embodiment of the invention.
FIG. 3 is a plan view of an optical head according to the first embodiment of the invention.
FIG. 4 is an explanatory diagram illustrating the principle of information recording in the first embodiment of the invention.
FIG. 5 is an explanatory diagram illustrating the principle of information reproduction in the first embodiment of the invention.
FIG. 6 is a waveform diagram for explaining in detail the principle of information reproduction in the first embodiment of the invention.
FIG. 7 is an explanatory diagram showing the principle of information recording for the case where multiple recording by phase encoding multiplexing is performed in the first embodiment of the invention.
FIG. 8 is an explanatory diagram showing the principle of information reproduction for the case where multiple recording by phase encoding multiplexing is performed in the first embodiment of the invention.
FIG. 9 is a waveform diagram for explaining in detail the principle of information reproduction for the case where multiple recording by phase encoding multiplexing is performed in the first embodiment of the invention.
FIG. 10 is a cross-sectional view showing the optical head of the first embodiment of the invention.
FIG. 11 is an explanatory diagram for explaining an example of a method for producing focus error information in the first embodiment of the invention.
FIG. 12 is an explanatory diagram for explaining an example of a method for producing tracking error information and a method for tracking servo in the first embodiment of the invention.
FIG. 13 is an explanatory diagram for explaining an example of the method for producing tracking error information and the method for tracking servo in the first embodiment of the invention.
FIG. 14 is an explanatory diagram showing the operation of the optical head during information recording in the first embodiment of the invention.
FIG. 15 is an explanatory diagram showing the movement of the irradiating position of the information light and recording-specific reference light in the first embodiment of the invention.
FIG. 16 is an explanatory diagram showing an example of changes in the position of the objective lens and changes in the driving voltage for moving the head body in a direction tangential to the tracks in the first embodiment of the invention.
FIG. 17 is an explanatory diagram for explaining a method for adjusting the irradiating position of the information light and the recording-specific reference light to the position of a desired information recording area in the first embodiment of the invention.
FIG. 18 is an explanatory diagram showing a concrete example of variations in the length of a pit in the first embodiment of the invention.
FIG. 19 is an explanatory diagram showing a concrete example of variations in the time for a pit and the time between pits in the first embodiment of the invention.
FIG. 20 is a plan view showing a driving mechanism of an optical head of an optical information recording/reproducing apparatus according to a second embodiment of the invention.
FIG. 21 is an explanatory diagram showing essential parts of a recording/reproducing optical system of an optical information recording/reproducing apparatus according to a third embodiment of the invention.
FIG. 22 is an explanatory diagram showing another example of an optical information recording medium in the third embodiment of the invention.
FIG. 23 is an explanatory diagram showing a general configuration of the recording/reproducing optical system of the optical information recording/reproducing apparatus according to the third embodiment of the invention.
FIG. 24 is a block diagram showing a configuration of the optical information recording/reproducing apparatus according to the third embodiment of the invention.
FIG. 25 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a servo operation in the third embodiment of the invention.
FIG. 26 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a recording operation in the third embodiment of the invention.
FIG. 27 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a reproducing operation in the third embodiment of the invention.
FIG. 28 is an explanatory diagram showing a general configuration of a recording/reproducing optical system of an optical information recording/reproducing apparatus according to a fourth embodiment of the invention.
FIG. 29 is an explanatory diagram showing a state of essential parts of the recording/reproducing optical system during a recording operation using recording-specific reference light whose phase is not spatially modulated in the fourth embodiment of the invention.
FIG. 30 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a reproducing operation using reproduction-specific reference light whose phase is not spatially modulated in the fourth embodiment of the invention.
FIG. 31 is a waveform diagram for explaining in detail the principle of reproduction of information using the reproduction-specific reference light whose phase is not spatially modulated in the optical information recording/reproducing apparatus according to the fourth embodiment of the invention.
FIG. 32 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a recording operation using recording-specific reference light whose phase is spatially modulated in the fourth embodiment of the invention.
FIG. 33 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during a reproducing operation using reproduction-specific reference light whose phase is spatially modulated in the fourth embodiment of the invention.
FIG. 34 is a waveform diagram for explaining in detail the principle of reproduction of information using the reproduction-specific reference light whose phase is spatially modulated in the optical information recording/reproducing apparatus according to the fourth embodiment of the invention.
FIG. 35 is a plan view showing an optical head and a recording medium of a fifth embodiment of the invention.
FIG. 36 is a cross-sectional view showing the configuration of the optical head of the fifth embodiment of the invention.
FIG. 37 is a cross-sectional view showing the configuration of a recording medium of the fifth embodiment of the invention.
FIG. 38 is an explanatory diagram showing an example of changes in the position of the objective lens and changes in the driving voltage for moving the positions of the objective lenses in a direction tangential to the tracks in the fifth embodiment of the invention.
DETAILED DESCRIPTION OF EMBODIMENTS Hereinafter, embodiments of the invention will be described in detail with reference to the drawings.
First Embodiment First, with reference toFIG. 1, an overview will be given of arecording medium1 used in a first embodiment of the invention.FIG. 1 shows a part of a track of therecording medium1. Therecording medium1 is disk-shaped and has a plurality of tracks TR. Each of the tracks TR has a plurality ofaddress servo areas6 arranged at regular intervals. One or moreinformation recording areas7 are provided between adjacent ones of theaddress servo areas6.FIG. 1 shows an example where fourinformation recording areas7 are arranged at regular intervals between adjacent ones of theaddress servo areas6.
Information for generating a basic clock, i.e., a timing reference for various operations of an optical information recording/reproducing apparatus, information for performing focus servo using a sampled servo system, information for performing tracking servo using the sampled servo system, and address information are recorded in advance in the form of emboss pits in theaddress servo areas6. However, the information for performing focus servo is not necessarily required to be recorded in theaddress servo areas6. In that case, focus servo may be performed using an interface between an air gap layer and a reflecting film to be described later. The address information is intended for identifying the individualinformation recording areas7, and corresponds to the identification information of the invention. The information for generating a basic clock, the information for performing focus servo, and the information for performing tracking servo serve to adjust the irradiating positions of information light, recording-specific reference light, and reproduction-specific reference light with respect to theinformation recording areas7, and correspond to the positioning information of the invention.
Now, with reference toFIG. 1, an overview will be given of an optical information recording method according to the present embodiment. In the present embodiment, to record information in theinformation recording areas7 of therecording medium1, therecording medium1 is rotated (moved) in the direction shown by the symbol R inFIG. 1, for example.Address servo areas6 and theinformation recording areas7 thus move in the direction shown by the symbol R. An optical head to be described later irradiates therecording medium1 with information light and recording-specific reference light so that information is recorded in theinformation recording areas7 in the form of interference patterns resulting from interference between the information light and the recording-specific reference light. The optical head moves the irradiating position of the information light and the recording-specific reference light such that the irradiating position follows a single movinginformation recording area7 for a predetermined period. Consequently, the singleinformation recording area7 keeps being irradiated with the information light and the recording-specific reference light for the predetermined period. It is therefore possible to irradiate theinformation recording areas7 with the information light and the recording-specific reference light for a sufficient time period to record information in theinformation recording areas7 without causing a deviation between theinformation recording areas7 and the irradiating position of the information light and the recording-specific reference light.
Next, with reference toFIG. 2, description will be given of a configuration of an optical information recording/reproducing apparatus including an optical information recording apparatus according to the present embodiment. The optical information recording/reproducingapparatus10 has: aspindle81 on which therecording medium1 is mounted; aspindle motor82 for rotating thespindle81; and aspindle servo circuit83 for controlling thespindle motor82 to keep the rotation speed of therecording medium1 at a predetermined value. The optical information recording/reproducingapparatus10 further has anoptical head40 and adriving device84. Theoptical head40 is provided for irradiating therecording medium1 with information light and recording-specific reference light to thereby record information, and for irradiating therecording medium1 with reproduction-specific reference light and detecting reproduction light to thereby reproduce information recorded in therecording medium1. The drivingdevice84 allows theoptical head40 to be movable in a direction of the radius of therecording medium1.
The optical information recording/reproducingapparatus10 further has adetection circuit85, afocus servo circuit86, a trackingservo circuit87, and aslide servo circuit88. Thedetection circuit85 detects a focus error signal FE, a tracking error signal TE and a reproduction signal RF from the output signal of theoptical head40. Thefocus servo circuit86 performs focus servo by moving a head body of theoptical head40, which will be described later, in a direction perpendicular to the surface of therecording medium1 based on the focus error signal FE detected by thedetection circuit85. The trackingservo circuit87 performs tracking servo by moving the head body in a direction of the radius of therecording medium1 based on the tracking error signal TE detected by thedetection circuit85. Theslide servo circuit88 performs slide servo by controlling the drivingdevice84 to move theoptical head40 in a direction of the radius of therecording medium1 based on the tracking error signal TE and a command from a controller to be described later.
The optical information recording/reproducingapparatus10 further has asignal processing circuit89, acontroller90, and an operatingportion91. Thesignal processing circuit89 decodes data outputted by a CCD array in theoptical head40, which will be described later, to thereby reproduce data recorded in theinformation recording areas7 of therecording medium1. It also reproduces a basic clock and determines addresses from the reproduction signal RF from thedetection circuit85. Thecontroller90 controls the optical information recording/reproducingapparatus10 as a whole, and the operatingportion91 supplies various instructions to thecontroller90.
The optical information recording/reproducingapparatus10 further has aninclination detection circuit92 and aninclination correction circuit93. Theinclination detection circuit92 detects relative inclination between therecording medium1 and the head body based on the output signal of thesignal processing circuit89. Based on the output signal of thisinclination detection circuit92, theinclination correction circuit93 changes the position of the head body in such directions that the head body changes in inclination with respect to the surface of therecording medium1, and thereby corrects the relative inclination between therecording medium1 and the head body.
The optical information recording/reproducingapparatus10 further has a follow-upcontrol circuit94. The follow-upcontrol circuit94 moves the head body in a direction generally along the tracks at the time of recording information, so that the irradiating position of the information light and the recording-specific reference light is controlled to follow a single movinginformation recording area7 for a predetermined period.
Thecontroller90 receives input of the basic clock and address information outputted by thesignal processing circuit89 and controls the parts such as theoptical head40, thespindle servo circuit83, theslide servo circuit88 and the follow-upcontrol circuit94. Thespindle servo circuit83 receives input of the basic clock outputted by thesignal processing circuit89. Thecontroller90 has a CPU (central processing unit), a ROM (read only memory) and a RAM (random access memory). The CPU executes programs stored in the ROM using the RAM as a work area to perform the functions of thecontroller90.
Next, with reference toFIG. 3, description will be given of a driving mechanism of the head body of theoptical head40.FIG. 3 is a plan view of theoptical head40. InFIG. 3, the symbol TR represents a track of therecording medium1. Theoptical head40 has thehead body41 which records information on therecording medium1 and reproduces information from therecording medium1. Thehead body41 has anobjective lens11 opposing to therecording medium1. Elasticarm fixing portions140aand140bare provided at both ends of thehead body41 in a direction tangential to the track (horizontal directions inFIG. 3).Elastic arms149 made of elastic members such as rubber, a plate spring, a coil spring, and a wire are fixed at one end each to these elasticarm fixing portions140aand140b. The other ends of theelastic arms149 are fixed to anarm support portion150. Thearm support portion150 is attached to apiezoelectric actuator170 which is capable of moving thisarm support portion150 in a direction of the radius of the recording medium1 (vertical directions inFIG. 3) within a predetermined range.
Coils151,152 for focus servo and inclination adjustment, and coils155,156 for irradiating position follow-up, are attached to one end of thehead body41 along a direction of the radius of therecording medium1. Likewise, coils153,154 for focus servo and inclination adjustment, and coils157,158 for irradiating position follow-up, are attached to the other end of thehead body41 along the direction of the radius of therecording medium1.
Theoptical head40 further has:magnets161,162,163, and164 which are arranged to penetrate through thecoils151,152,153, and154, respectively; amagnet165 which is located in a position opposite to thecoils155 and156; and amagnet166 which is located in a position opposite to thecoils157 and158.
In theoptical head40, thecoils151 to154 and themagnets161 to164 can change the position of thehead body41 in a direction perpendicular to the surface of the recording medium1 (a direction perpendicular to the plane of the drawing sheet ofFIG. 3) and in such a direction that thehead body41 varies in inclination with respect to the surface of therecording medium1. Moreover, in theoptical head40, thepiezoelectric actuator170 can change the position of thehead body41 in a direction of the radius of therecording medium1. Furthermore, in theoptical head40, theelastic arms149, thecoils155 to158, and themagnets165 and166 can change the position of thehead body41 in a direction generally along the track TR. Theelastic arms149, thecoils155 to158, and themagnets165 and166 correspond to the irradiating position moving device of the invention.
Thecoils151 to154 are driven by thefocus servo circuit86 and theinclination correction circuit93 inFIG. 2. Thecoils155 to158 are driven by the follow-upcontrol circuit94 inFIG. 2. Thepiezoelectric actuator170 is driven by the trackingservo circuit87 inFIG. 2.
Next, with reference toFIG. 4, description will be given of the configuration of the recording medium for use in the present embodiment. Therecording medium1 of the present embodiment comprises a disk-shapedtransparent substrate2 made of polycarbonate or the like, and aninformation recording layer3, anair gap layer4, and a reflectingfilm5 that are arranged in this order from thetransparent substrate2, on a side of thetransparent substrate2 opposite from the light incident/exit side. Theinformation recording layer3 is a layer on which information is recorded through the use of holography, and is made of a hologram material which varies, when irradiated with light, in its optical characteristics such as refractive index, permittivity, and reflectance, depending on the intensity of the light. The available hologram material includes photopolymer HRF-600 (product name) manufactured by Dupont and photopolymer ULSH-500 (product name) manufactured by Aprils. The reflectingfilm5 is made of aluminum, for example. Incidentally, in therecording medium1, theinformation recording layer3 and the reflectingfilm5 may be arranged next to each other without theair gap layer4.
Next, description will be given of the principle of information recording in the optical information recording/reproducing apparatus according to the present embodiment. In the embodiment, information light and recording-specific reference light are generated, and theinformation recording layer3 of therecording medium1 is irradiated with the information light and the recording-specific reference light so that information is recorded in theinformation recording layer3 in the form of an interference pattern resulting from interference between the information light and the recording-specific reference light. The information light is generated by spatially modulating the phase of light based on the information to be recorded.
Hereinafter, the optical information recording method according to the present embodiment will be described in detail with reference toFIG. 4.FIG. 4 illustrates part of an example of a recording/reproducing optical system of the optical information recording/reproducing apparatus according to the embodiment. In this example, the recording/reproducing optical system has anobjective lens11 facing toward the transparent-substrate-2 side of therecording medium1, and abeam splitter12 and a phase spatiallight modulator13 that are arranged in this order from theobjective lens11, on a side of theobjective lens11 opposite from therecording medium1. Thebeam splitter12 has asemi-reflecting surface12athat is inclined at 45° in the normal direction with respect to the direction of the optical axis of theobjective lens11. The recording/reproducing optical system shown inFIG. 4 also has aphotodetector14. Thephotodetector14 is provided in a direction in which return light from therecording medium1 is reflected by thesemi-reflecting surface12aof thebeam splitter12. The phase spatiallight modulator13 has a number of pixels arranged in a matrix, and is capable of spatially modulating the phase of light by selecting the phase of outgoing light for each of the pixels. Thephotodetector14 also has a number of pixels arranged in a matrix, and is capable of detecting the intensity of received light for each of the pixels.
In the example shown inFIG. 4, the phase spatiallight modulator13 generates the information light and the recording-specific reference light. Coherent parallel light having a constant phase and intensity is incident on the phase spatiallight modulator13. For information recording, the phase spatiallight modulator13, in ahalf area13A thereof, selects the phase of the outgoing light for each pixel based on the information to be recorded, thereby modulating the phase of the light spatially to generate the information light. In theother half area13B, it renders the phase of the outgoing light identical for all the pixels to generate the recording-specific reference light.
In thearea13A, the phase spatiallight modulator13 sets the phase of the light after the modulation for each pixel, to either a first phase having a phase difference of +π/2 (rad) with respect to a predetermined reference phase, or a second phase having a phase difference of −π/2 (rad) with respect to the reference phase. The phase difference between the first phase and the second phase is π (rad). Incidentally, in thearea13A, the phase spatiallight modulator13 may set the phase of the light after the modulation at any of three or more values for each pixel. In thearea13B, the phase spatiallight modulator13 sets the phase of the outgoing light for every pixel to the first phase having a phase difference of +π/2 (rad) with respect to the predetermined reference phase. Incidentally, in thearea13B, the phase spatiallight modulator13 may set the phase of the outgoing light for every pixel to the second phase or a certain phase different from both the first phase and the second phase.
FIG. 4 shows the phases and intensities of incident light on the phase spatiallight modulator13, outgoing light from the phase spatiallight modulator13, incident light on theobjective lens11 yet to be applied to therecording medium1, and return light from therecording medium1 reflected by thesemi-reflecting surface12aof thebeam splitter12. InFIG. 4, the symbol “+” represents the first phase, and the symbol “−” the second phase.FIG. 4 also shows the maximum value of intensity as “1” and the minimum value of intensity as “0”.
In the example shown inFIG. 4, for information recording, coherent parallel light21 having a constant phase and intensity is incident on the phase spatiallight modulator13. Of the light incident on the phase spatiallight modulator13, the light that has passed through thearea13A becomes information light22A, being spatially modulated in phase based on the information to be recorded. The information light22A locally drops in intensity at the borders between first-phase pixels and second-phase pixels. Meanwhile, of the light incident on the phase spatiallight modulator13, the light that has passed through thearea13B becomes recording-specific reference light22B without being spatially modulated in phase. The information light22A and the recording-specific reference light22B are incident on thebeam splitter12. Part of them passes through thesemi-reflecting surface12a, and further through theobjective lens11 to turn into converging information light23A and converging recording-specific reference light23B, respectively, with which therecording medium1 is irradiated. The information light23A and the recording-specific reference light23B pass through theinformation recording layer3, converge to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and are reflected by the reflectingfilm5.Information light24A and recording-specific reference light24B that have been reflected by the reflectingfilm5 become divergent light to pass through theinformation recording layer3 again.
In theinformation recording layer3, the information light23A yet to be reflected by the reflectingfilm5 and the recording-specific reference light24B that has been reflected by the reflectingfilm5 interfere with each other to form an interference pattern, and the information light24A that has been reflected by the reflectingfilm5 and the recording-specific reference light23B yet to be reflected by the reflectingfilm5 interfere with each other to form an interference pattern. Then, these interference patterns are volumetrically recorded in theinformation recording layer3.
The information light24A and the recording-specific reference light24B having been reflected by the reflectingfilm5 are emitted from therecording medium1, and become parallel information light25A and parallel recording-specific reference light25B through theobjective lens11. The light25A and the light25B are incident on thebeam splitter12, and part of each of them is reflected by thesemi-reflecting surface12aand received by thephotodetector14.
Next, description will be given of the principle of information reproduction in the optical information recording/reproducing apparatus according to the present embodiment. In the embodiment, reproduction-specific reference light is generated, and theinformation recording layer3 of therecording medium1 is irradiated with this reproduction-specific reference light. Then, reproduction light that is generated from theinformation recording layer3 irradiated with the reproduction-specific reference light is collected. The reproduction light is superimposed on the reproduction-specific reference light to generate composite light, and this composite light is detected.
Hereinafter, with reference toFIG. 5, detailed description will be given of the optical information reproducing method according to the present embodiment. LikeFIG. 4,FIG. 5 illustrates part of an example of the recording/reproducing optical system of the optical information recording/reproducing apparatus according to the embodiment.
FIG. 5 shows the phases and intensities of the incident light on the phase spatiallight modulator13, the outgoing light from the phase spatiallight modulator13, the incident light on theobjective lens11 yet to be applied to therecording medium1, and the return light from therecording medium1 reflected by thesemi-reflecting surface12aof thebeam splitter12. InFIG. 5, the phases and intensities are expressed in the same manner as inFIG. 4.
In the example shown inFIG. 5, for information reproduction, coherent parallel light31 having a constant phase and intensity is incident on the phase spatiallight modulator13. For information reproduction, the phase spatiallight modulator13 sets the phase of the outgoing light for every pixel to a first phase having a phase difference of +π/2 (rad) with respect to a predetermined reference phase, thereby generating reproduction-specific reference light32. The reproduction-specific reference light32 is incident on thebeam splitter12, and part thereof passes through thesemi-reflecting surface12a, and further through theobjective lens11 to turn into converging reproduction-specific reference light33, with which the opticalinformation recording medium1 is irradiated. The reproduction-specific reference light33 passes through theinformation recording layer3, converges to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and is reflected by the reflectingfilm5. Having been reflected by the reflectingfilm5, the reproduction-specific reference light becomes divergent light to pass through theinformation recording layer3 again.
In theinformation recording layer3, the reproduction-specific reference light33 yet to be reflected by the reflectingfilm5 causes reproduction light that travels away from the reflectingfilm5. The reproduction-specific reference light that has been reflected by the reflectingfilm5 causes reproduction light that travels toward the reflectingfilm5. The reproduction light traveling away from the reflectingfilm5 is emitted as-is from therecording medium1. The reproduction light traveling toward the reflectingfilm5 is reflected by the reflectingfilm5 and emitted from therecording medium1.
Thus, at the time of reproduction, return light34 from therecording medium1 includes the reproduction light and the reproduction-specific reference light that has been reflected by the reflectingfilm5. Thereturn light34 is turned into parallel return light35 through theobjective lens11, and incident on thebeam splitter12. Part of the light is reflected by thesemi-reflecting surface12a, and received by thephotodetector14. Thereturn light35 incident on thephotodetector14 includesreproduction light36 and reproduction-specific reference light37 that has been reflected by the reflectingfilm5. Thereproduction light36 is light that is spatially modulated in phase according to the information recorded in theinformation recording layer3. For the sake of convenience,FIG. 5 shows thereproduction light36 and the reproduction-specific reference light37 separately, along with their respective phases and intensities. In reality, however, thereproduction light36 is superimposed on the reproduction-specific reference light37 to generate composite light, and this composite light is received by thephotodetector14. The composite light is light that is spatially modulated in intensity according to the information recorded. Thus, thephotodetector14 detects a two-dimensional intensity pattern of the composite light, from which the information is reproduced.
As shown inFIG. 4 andFIG. 5, the optical information recording/reproducing apparatus according to the present embodiment performs the irradiation with the information light, the recording-specific reference light and the reproduction-specific reference light and the collection of the reproduction light on the same side of theinformation recording layer3 so that the information light, the recording-specific reference light, the reproduction-specific reference light and the reproduction light are arranged coaxially. All of the information light, the recording-specific reference light and the reproduction-specific reference light converge to become minimum in diameter at the same position. InFIG. 4, the information light23A and the recording-specific reference light23B to irradiate theinformation recording layer3 with are light beams that are semicircular in cross section. Those beams are coaxial since they constitute respective halves of a light beam that is circular in cross section.
Now, with reference toFIG. 6, detailed description will be given of thereproduction light36, the reproduction-specific reference light37, and the composite light mentioned above. InFIG. 6, (a) represents the intensity of thereproduction light36, (b) the phase of thereproduction light36, (c) the intensity of the reproduction-specific reference light37, (d) the phase of the reproduction-specific reference light37, and (e) the intensity of the composite light.FIG. 6 shows an example where the phase of the information light for each pixel is set to either the first phase having a phase difference of +π/2 (rad) with respect to the reference phase, or the second phase having a phase difference of −π/2 (rad) with respect to the reference phase. Consequently, in the example shown inFIG. 6, thereproduction light36 has either the first phase or the second phase pixel by pixel as the information light does. The reproduction-specific reference light37 has the first phase for every pixel. Assuming here that thereproduction light36 and the reproduction-specific reference light37 are equal in intensity, the composite light exceeds thereproduction light36 and the reproduction-specific reference light37 in intensity at pixels where thereproduction light36 has the first phase, and the composite light theoretically becomes zero in intensity at pixels where thereproduction light36 has the second phase, as shown inFIG. 6(e).
Now, detailed description will be given of the relationship between the phase of the reproduction light and the intensity of the composite light, including situations where the phase of the information light is set at either of two values and where the phase of the information light is set at any of three or more values for recording.
The composite light is made by superimposing one of two lightwaves, the reproduction light, on the other, the reproduction-specific reference light. Thus, the intensity I of the composite light is given by the following equation (1), where a0is both the amplitude of the reproduction light and the amplitude of the reproduction-specific reference light, and δ is a phase difference between the reproduction light and the reproduction-specific reference light:
Since the phase of the reproduction-specific reference light is constant irrespective of pixel, from the foregoing equation, it can be seen that the intensity I of the composite light varies with the phase of the reproduction light. Moreover, when the phase of the information light is set at any of n values (n is an integer no less than 2) within a range of, e.g., +π/2 (rad) to −π/2 (rad), the intensity I of the composite light also takes any of the n values.
As above, according to the optical information reproducing method of the present embodiment, the two-dimensional intensity pattern of the composite light generated by superimposing the reproduction light on the reproduction-specific reference light is detected to reproduce the information recorded in theinformation recording layer3 in the form of an interference pattern resulting from the interference between the information light that is spatially modulated in phase based on the information to be recorded, and the recording-specific reference light.
By the way, in the present embodiment, recording-specific reference light and reproduction-specific reference light that are spatially modulated in phase may be used to achieve both multiple recording by phase encoding multiplexing and reproduction of the information multiple-recorded in this way. Hereinafter, with reference toFIG. 7 toFIG. 9, description will be given of the principle of information recording and the principle of information reproduction for the case where multiple recording by phase-encoding multiplex is performed.
First, with reference toFIG. 7, description will be given of the principle of information recording for the case where multiple recording by phase-encoding multiplex is performed.FIG. 7 shows part of an example of the recording/reproducing optical system of the optical information recording/reproducing apparatus according to the embodiment. The optical system shown inFIG. 7 has the same configuration as inFIG. 4.FIG. 7 illustrates the phases and intensities of incident light on the phase spatiallight modulator13, outgoing light from the phase spatiallight modulator13, incident light on theobjective lens11 yet to irradiate therecording medium1 with, and return light from therecording medium1 reflected by thesemi-reflecting surface12aof thebeam splitter12. InFIG. 7, the phases and intensities of the light are expressed in the same manner as inFIG. 4.
When recording information, coherent parallel light21 having a constant phase and intensity is incident on the phase spatiallight modulator13. Ahalf area13A of the phase spatiallight modulator13 selects the phase of outgoing light from between two values or from among three or more values for each pixel based on information to be recorded, thereby generating information light22A that is spatially modulated in phase. Here, for ease of explanation, thearea13A shall modulate the phase of the outgoing light spatially by setting the phase of the outgoing light to either a first phase having a phase difference of +π/2 (rad) with respect to a predetermined reference phase or a second phase having a phase difference of −π/2 (rad) with respect to the reference phase for each pixel. Meanwhile, theother half area13B of the phase spatiallight modulator13 selects the phase of the outgoing light from between two values or from among three or more values for each pixel, thereby generating recording-specific reference light22B that is spatially modulated in phase. Here, for ease of explanation, thearea13B shall modulate the phase of the outgoing light spatially by setting the phase of the outgoing light at any of the reference phase, the first phase, and the second phase for each pixel.
The information light22A and the recording-specific reference light22B are incident on thebeam splitter12. Part of them pass through thesemi-reflecting surface12a, and further through theobjective lens11 to turn into converging information light23A and converging recording-specific reference light23B, respectively, with which therecording medium1 is irradiated. The information light23A and the recording-specific reference light23B pass through theinformation recording layer3, converge to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and are reflected by the reflectingfilm5.Information light24A and recording-specific reference light24B that has been reflected by the reflectingfilm5 become divergent light to pass through theinformation recording layer3 again.
In theinformation recording layer3, the information light23A yet to be reflected by the reflectingfilm5 and the recording-specific reference light24B that has been reflected by the reflectingfilm5 interfere with each other to form an interference pattern, and the information light24A that has been reflected by the reflectingfilm5 and the recording-specific reference light23B yet to be reflected by the reflectingfilm5 interfere with each other to form an interference pattern. Then, these interference patterns are volumetrically recorded in theinformation recording layer3.
The information light24A and the recording-specific reference light24B having been reflected by the reflectingfilm5 are emitted from therecording medium1, and become parallel information light25A and parallel recording-specific reference light25B through theobjective lens11. The light25A and the light25B are incident on thebeam splitter12. Part of them are reflected by thesemi-reflecting surface12a, and received by thephotodetector14.
Next, with reference toFIG. 8, description will be given of the principle of information reproduction for the case where multiple recording by phase-encoding multiplex is performed.FIG. 8 shows, likeFIG. 7, part of an example of the recording/reproducing optical system in the optical information recording/reproducing apparatus according to the present embodiment.FIG. 8 illustrates the phases and intensities of incident light on the phase spatiallight modulator13, outgoing light from the phase spatiallight modulator13, incident light on theobjective lens11 yet to irradiate therecording medium1 with, and return light from therecording medium1 reflected by thesemi-reflecting surface12aof thebeam splitter12. InFIG. 8, the phases and intensities are expressed in the same manner as inFIG. 7.
When reproducing information, coherent parallel light31 having a constant phase and intensity is incident on the phase spatiallight modulator13. Thehalf area13B of the phase spatiallight modulator13 selects the phase of the outgoing light from between two values or from among three or more values for each pixel, thereby generating reproduction-specific reference light32B1that is spatially modulated in phase in the same modulation pattern as that of the recording-specific reference light22B. On the other hand, thehalf area13A of the phase spatiallight modulator13 selects the phase of the outgoing light from between two values or from among three or more values for each pixel, thereby generating reproduction-specific reference light32B2that is spatially modulated in phase in a pattern that is point-symmetric to the modulation pattern of the reproduction-specific reference light32B1about a position of optical axis of the optical system that irradiates theinformation recording layer3 with the recording-specific reference light and the reproduction-specific reference light.
The reproduction-specific reference light32B1and the reproduction-specific reference light32B2are incident on thebeam splitter12. Part of them pass through thesemi-reflecting surface12a, and further through theobjective lens11 to turn into converging reproduction-specific reference light33B1and33B2, respectively, with which therecording medium1 is irradiated. The reproduction-specific reference light33B1and the reproduction-specific reference light33B2pass through theinformation recording layer3, converge to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and are reflected by the reflectingfilm5. Having been reflected by the reflectingfilm5, the reproduction-specific reference light become divergent light to pass through theinformation recording layer3 again.
In theinformation recording layer3, the reproduction-specific reference light33B2yet to be reflected by the reflectingfilm5 causes reproduction light that travels away from the reflectingfilm5, while the reproduction-specific reference light33B2having been reflected by the reflectingfilm5 causes reproduction light that travels toward the reflectingfilm5. The reproduction light traveling away from the reflectingfilm5 is emitted as-is from therecording medium1. The reproduction light traveling toward the reflectingfilm5 is reflected by the reflectingfilm5 and emitted from therecording medium1. Both of the reproduction light are represented by reference numeral34A1.
In theinformation recording layer3, on the other hand, the reproduction-specific reference light33B1yet to be reflected by the reflectingfilm5 causes reproduction light that travels away from the reflectingfilm5, while the reproduction-specific reference light33B1having been reflected by the reflectingfilm5 causes reproduction light that travels toward the reflectingfilm5. The reproduction light traveling away from the reflectingfilm5 is emitted as-is from therecording medium1. The reproduction light traveling toward the reflecting film S is reflected by the reflectingfilm5 and emitted from therecording medium1. Both of the reproduction light are represented by reference numeral34A2.
Meanwhile, the reproduction-specific reference light33B1is reflected by the reflectingfilm5 and becomes reproduction-specific reference light34B1that travels in the same direction as the reproduction light34A1does. The reproduction-specific reference light33B2is reflected by the reflectingfilm5 and becomes reproduction-specific reference light34B2that travels in the same direction as the reproduction light34A2does.
The reproduction light34A1,34A2and the reproduction-specific reference light34B1,34B2are turned into parallel reproduction light35A1,35A2and parallel reproduction-specific reference light35B1,35B2through theobjective lens11, respectively, and are incident on thebeam splitter12. Then, part of them are reflected by thesemi-reflecting surface12aand received by thephotodetector14.
Both the reproduction light35A1and the reproduction light35A2are spatially modulated in phase as the information light for recording. The phase modulation patterns of the reproduction light35A, and the reproduction light35A2are mutually symmetrical with respect to a point.
Composite light produced by superimposing the reproduction light35A1on the reproduction-specific reference light35B, is incident on a half area of thephotodetector14. Composite light produced by superimposing the reproduction light35A2on the reproduction-specific reference light35B2is incident on the other half area of thephotodetector14. Both of the two types of composite light are spatially modulated in intensity according to the information recorded. The intensity modulation patterns of the two types of composite light are mutually symmetrical with respect to a point. Thus, thephotodetector14 can reproduce information by detecting a two-dimensional pattern of intensity of one of the two types of composite light. Here, information shall be reproduced by detecting the two-dimensional pattern of intensity of the composite light produced by superimposing the reproduction light35A1on the reproduction-specific reference light35B1.
Next, the reproduction light, the reproduction-specific reference light, and the composite light mentioned above will be described in detail with reference toFIG. 9. InFIG. 9, (a) shows the intensity of the reproduction light, (b) the phase of the reproduction light, (c) the intensity of the reproduction-specific reference light, (d) the phase of the reproduction-specific reference light, and (e) the intensity of the composite light.FIG. 9 shows an example where the phase of the information light is set at either the first phase or the second phase for each pixel, and the phases of the recording-specific reference light and the reproduction-specific reference light are set at any of the reference phase, the first phase, and the second phase for each pixel. In this case, the phase of the reproduction light for each pixel is either the first phase or the second phase like the information light. Consequently, the phase difference between the reproduction light and the reproduction-specific reference light is any of zero, ±π/2 (rad), and ±π (rad). Suppose here that the intensity of the reproduction light and the intensity of the reproduction-specific reference light are equal. In that case, as shown inFIG. 9(e), the intensity of the composite light becomes maximum at pixels where the phase difference between the reproduction light and the reproduction-specific reference light is zero, and becomes theoretically zero at pixels where the phase difference between the reproduction light and the reproduction-specific reference light is ±π (rad). At pixels where the phase difference between the reproduction light and the reproduction-specific reference light is ±π/2 (rad), the intensity becomes ½ that at a zero-phase-difference pixel. InFIG. 9(e), the intensity at the pixels where the phase difference is ±π (rad) is represented by “0”, the intensity at the pixels where the phase difference is ±π/2 (rad) is represented by “1”, and the intensity at the pixels where the phase difference is zero is represented by “2”.
In the example shown inFIG. 7 throughFIG. 9, the intensity of the composite light has three values for each pixel. Then, for example, the intensity “0” can be associated with two bits of data “00”, the intensity “1” with two bits of data “01”, and the intensity “2” with two bits of data “10” as shown inFIG. 9(e). Thus, in the example shown inFIG. 7 throughFIG. 9, the composite light can carry an increased amount of information with the same intensity and phase of the reproduction light as compared to the cases where the intensity of the composite light has two values for each pixel as shown inFIG. 4 throughFIG. 6. As a result, therecording medium1 can be enhanced in recording density.
Where the phase difference between the reproduction light and the reproduction-specific reference light is expressed as δ, the intensity I of the composite light is given by the equation (1) mentioned previously. The equation (1) shows that the intensity I of the composite light varies according to the phase difference between the reproduction light and the reproduction-specific reference light. Consequently, when the absolute value of the phase difference between the reproduction light and the reproduction-specific reference light, i.e., the absolute value of the phase difference between the information light and the reproduction-specific reference light, has n values (n is an integer no less than 2) within the range of 0 to π (rad), for example, the intensity I of the composite light also has the n values.
Meanwhile, when the information light and the recording-specific reference light that are spatially modulated in phase are used to record information on theinformation recording layer3 of therecording medium1 as described above, the phase modulation pattern of the information light is determined based on the information to be recorded and the phase modulation pattern of the recording-specific reference light to be used in recording the information. This will be described in detail with reference toFIG. 9. Since the information recorded on theinformation recording layer3 is reproduced based on the intensity pattern of the composite light, the information to be recorded is converted into data on a desired intensity pattern of the composite light as shown inFIG. 9(e). The phase modulation pattern of the recording-specific reference light is the same as the phase modulation pattern of the reproduction-specific reference light as shown inFIG. 9(d). By means of phase calculation using the data on the desired intensity pattern of the composite light as shown inFIG. 9(e) and the data on the phase modulation patterns of the reproduction-specific reference light and the recording-specific reference light as shown inFIG. 9(d), the phase modulation pattern of the information light is determined so as to be the same as or point-symmetric to the desired phase modulation pattern of the reproduction light as shown inFIG. 9(b).
Theinformation recording layer3 on which information is recorded by using the information light having the phase modulation pattern determined as described above and the recording-specific reference light may be irradiated with the reproduction-specific reference light having the phase modulation pattern as shown inFIG. 9(d), which is the same as the phase modulation pattern of the recording-specific reference light. In such a case, composite light having the intensity pattern as shown inFIG. 9(e) is obtained. The information recorded on theinformation recording layer3 is reproduced based on the intensity pattern of this composite light.
The phase modulation patterns of the recording-specific reference light and the reproduction-specific reference light may be produced from information unique to an individual who is a user. Such information unique to an individual includes a personal identification number, a fingerprint, a voiceprint, and an iris pattern. In that case, information can be reproduced only by the certain individual who recorded the information on therecording medium1.
As has been described, the use of the recording-specific reference light and the reproduction-specific reference light that are spatially modulated in phase allows both the multiple recording by phase encoding multiplexing and reproduction of the information multiple-recorded in this way.
Next, with reference toFIG. 10, description will be given of the recording/reproducing optical system provided in theoptical head40.FIG. 10 is a cross-sectional view showing theoptical head40. As shown inFIG. 10, theoptical head40 has ahead body41 that accommodates individual components to be described later. Asemiconductor laser43 is fixed to the internal bottom of thehead body41 via asupport42. A phase spatiallight modulator44 of reflection type and aphotodetector45 are also fixed thereto. Amicrolens array46 is attached to the light-receiving surface of thephotodetector45. In thehead body41, aprism block48 is provided above the phase spatiallight modulator44 and thephotodetector45. Acollimator lens47 is provided near an end of theprism block48 closer to thesemiconductor laser43. Thehead body41 has an opening at the surface facing toward therecording medium1. Anobjective lens11 is provided in this opening. A quarter-wave plate49 is provided between theobjective lens11 and theprism block48.
The phase spatiallight modulator44 has a number of pixels arranged in a matrix, and is capable of spatially modulating the phase of light by setting the phase of outgoing light for each pixel to either of two values differing by π (rad) from each other. Furthermore, the phase spatiallight modulator44 rotates the direction of polarization of the outgoing light by 90° with respect to the direction of polarization of the incident light. For example, a reflection-type liquid crystal device may be used for the phase spatiallight modulator44.
Thephotodetector45 has a number of pixels arranged in a matrix, and is capable of detecting the intensity of received light for each pixel. Themicrolens array46 includes a plurality of microlenses arranged to oppose to the light-receiving surfaces of the respective pixels of thephotodetector45.
A CCD-type solid image pick-up device or a MOS-type solid image pick-up device may be used as thephotodetector45. Alternatively, a smart light sensor in which a MOS type solid image pick-up device and a signal processing circuit are integrated on a single chip (for example, see the literature “O plus E, September 1996, No. 202, pp. 93-99”) may be used. Since this smart light sensor has a high transfer rate and high-speed operation facilities, the use of this smart light sensor allows high-speed reproduction. For example, reproduction can be performed at transfer rates on the order of Gbit/s.
Theprism block48 has a polarizationbeam splitter surface48aand a reflectingsurface48b. Of the polarizationbeam splitter surface48aand the reflectingsurface48b, the polarizationbeam splitter surface48ais located closer to thecollimator lens47. The polarizationbeam splitter surface48aand the reflectingsurface48bare both inclined at 45° in the normal direction with respect to the direction of the optical axis of thecollimator lens47, and they are arranged in parallel to each other.
The phase spatiallight modulator44 is placed below the polarizationbeam splitter surface48a, and thephotodetector45 is placed below the reflectingsurface48b. The quarter-wave plate49 and theobjective lens11 are placed above the polarizationbeam splitter surface48a. Thecollimator lens47 and theobjective lens11 may be hologram lenses.
The polarizationbeam splitter surface48aof theprism block48, as will be detailed later, achieves separation between the optical path of the information light, the recording-specific reference light, and the reproduction-specific reference light yet to pass through the quarter-wave plate49 and the optical path of the return light from therecording medium1 having passed through the quarter-wave plate49, according to the difference in directions of polarization.
Theprism block48, the phase spatiallight modulator44, and thephotodetector45 inFIG. 10 correspond to thebeam splitter12, the phase spatiallight modulator13, and thephotodetector14 inFIG. 4, respectively.
Next, description will be given of the operation of the recording/reproducing optical system in information recording. Thesemiconductor laser43 emits coherent S-polarized light. S-polarization refers to linear polarization the direction of which is perpendicular to the incidence plane (plane of the drawing sheet ofFIG. 10), whereas P-polarization to be described later refers to linear polarization the direction of which is parallel to the incidence plane.
The S-polarized laser light emitted from thesemiconductor laser43 is turned into parallel light through thecollimator lens47, incident on the polarizationbeam splitter surface48aof theprism block48, reflected by the polarizationbeam splitter surface48a, and incident on the phase spatiallight modulator44. In a half area, the outgoing light from the phase spatiallight modulator44 becomes information light that is spatially modulated in phase based on the information to be recorded. In the other half area, the outgoing light becomes recording-specific reference light having an identical phase for all the pixels or recording-specific reference light that is spatially modulated in phase. The outgoing light from the phase spatiallight modulator44 is subjected to a rotation of the direction of polarization by 90° to become P-polarized light.
Since the information light and the recording-specific reference light, which have exited the phase spatiallight modulator44, are P-polarized light, they are transmitted through the polarizationbeam splitter surface48aof theprism block48, and become circularly polarized light by passing through the quarter-wave plate49. The information light and the recording-specific reference light are condensed by theobjective lens11 to irradiate therecording medium1 with. The information light and the recording-specific reference light pass through theinformation recording layer3, converge to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and are reflected by the reflectingfilm5. Having been reflected by the reflectingfilm5, the information light and the recording-specific reference light become divergent light to pass through theinformation recording layer3 again. When the power of thesemiconductor laser43 is set at a high level suitable for recording, an interference pattern resulting from the interference between the information light and the recording-specific reference light is recorded on theinformation recording layer3.
The return light from therecording medium1 is turned into parallel light through theobjective lens11, and passes through the quarter-wave plate49 to become S-polarized light. This return light is reflected by the polarizationbeam splitter surface48aof theprism block48, further reflected by the reflectingsurface48b, and incident on thephotodetector45 through themicrolens array46.
When recording information, while the light beam from theobjective lens11 passes through theaddress servo areas6 of therecording medium1, the power of thesemiconductor laser43 is set at a low level suitable for reproduction and the phase spatiallight modulator44 emits light having an identical phase for all the pixels, without modulating the phase of the light. Basic clock, address information, focus error signals and tracking error information can be obtained based on the output of thephotodetector45 at this time.
Next, description will be given of the operation of the recording/reproducing optical system in information reproduction. In information reproduction, the power of thesemiconductor laser43 is set at a low level suitable for reproduction. The S-polarized laser light emitted from thesemiconductor laser43 is turned into parallel light through thecollimator lens47, incident on the polarizationbeam splitter surface48aof theprism block48, reflected by the polarizationbeam splitter surface48a, and incident on the phase spatiallight modulator44. The light that has exited the phase spatiallight modulator44 becomes reproduction-specific reference light having an identical phase for all the pixels, or reproduction-specific reference light that is spatially modulated in phase. The light that has exited the phase spatiallight modulator44 is subjected to a rotation of the direction of polarization by 90° to become P-polarized light.
Since the reproduction-specific reference light, which has exited the phase spatiallight modulator44, is P-polarized light, it is transmitted through the polarizationbeam splitter surface48aof theprism block48 and circularly polarized through the quarter-wave plate49. The reproduction-specific reference light is condensed by theobjective lens11 to irradiate therecording medium1 with. The reproduction-specific reference light passes through theinformation recording layer3, converges to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5, and is reflected by the reflectingfilm5. Having been reflected by the reflectingfilm5, the reproduction-specific reference light becomes divergent light to pass through theinformation recording layer3 again. The reproduction-specific reference light causes reproduction light to be generated from theinformation recording layer3.
The return light from therecording medium1 includes the reproduction light and the reproduction-specific reference light. The return light is turned into parallel light through theobjective lens11, and S-polarized through the quarter-wave plate49. The return light is reflected by the polarizationbeam splitter surface48aof theprism block48, further reflected by the reflectingsurface48b, and incident on thephotodetector45 through themicrolens array46. The information recorded on therecording medium1 can be reproduced based on the output of thephotodetector45.
When reproducing information, while the light beam from theobjective lens11 passes through theaddress servo areas6 of therecording medium1, basic clock, address information, focus error signals and tracking error information can be obtained based on the output of thephotodetector45.
The phase spatiallight modulator44 may be one that causes no rotation in the direction of polarization of light. In this case, the polarizationbeam splitter surface48aof theprism block48 inFIG. 10 is replaced with a semi-reflecting surface. Alternatively, a quarter-wave plate may be provided between theprism block48 and the phase spatiallight modulator44, so that the S-polarized light from theprism block48 is converted into circularly-polarized light through the quarter-wave plate and incident on the phase spatiallight modulator44, and so that the circularly-polarized light from the phase spatiallight modulator44 is converted into P-polarized light through the quarter-wave plate and transmitted through the polarizationbeam splitter surface48a. The phase spatial light modulator that is capable of setting the phase of the outgoing light to any of three or more values for each pixel is not limited to the one using liquid crystal. For example, it may have such configuration that micromirror devices are used to adjust the position of the reflecting surface in the traveling direction of the incident light for each pixel.
Next, with reference toFIG. 11, description will be given of an example of a method for producing focus error information in the present embodiment.FIG. 11 is an explanatory diagram showing the outline of incident light on the light-receiving surface of thephotodetector45. In the method for producing focus error information of this example, focus error information is produced based on the size of the outline of the incident light on the light-receiving surface of thephotodetector45 in the following manner. Initially, in a focused state where the light beam from theobjective lens11 converges to become minimum in diameter on the interface between theair gap layer4 and the reflectingfilm5 of therecording medium1, the incident light on the light-receiving surface of thephotodetector45 shall have the outline designated by thereference numeral60 inFIG. 11. If the position at which the light beam from theobjective lens11 has the minimum diameter shifts back from the interface between theair gap layer4 and the reflectingfilm5, the outline of the incident light on the light-receiving surface of thephotodetector45 decreases in diameter as shown by thereference numeral61 inFIG. 11. On the other hand, if the position at which the light beam from theobjective lens11 has the minimum diameter shifts forward beyond the interface between theair gap layer4 and the reflectingfilm5, the outline of the incident light on the light-receiving surface of thephotodetector45 increases in diameter as shown by thereference numeral62 inFIG. 11. Consequently, a focus error signal can be obtained by detecting a signal responsive to a change in the diameter of the outline of the incident light on the light-receiving surface of thephotodetector45, with reference to the focused state. Specifically, for example, the focus error signal can be produced based on fluctuations in the number of pixels corresponding to a bright area in the light-receiving surface of thephotodetector45 with reference to the focused state.
In present the embodiment, the position of theoptical head body41 in a direction perpendicular to therecording medium1 is adjusted based on the focus error signal so that the light beam is always in the focused state, thereby effecting focus servo. When the light beam passes through theinformation recording areas7, no focus servo is performed and the state at the passing of the previousaddress servo area6 is maintained.
Next, with reference toFIG. 12 andFIG. 13, description will be given of an example of a method for producing tracking error information and a method for tracking servo in the present embodiment. In this example, as shown inFIG. 12(a), theaddress servo areas6 of therecording medium1 have twopits71A, asingle pit71B, and asingle pit71C that are formed in this order in a traveling direction of alight beam72 along atrack70, as positioning information to be used for tracking servo. The twopits71A are arranged at a position designated by the symbol A inFIG. 12, symmetrically across thetrack70. Thepit71B is located at a position designated by the symbol B inFIG. 12, being shifted to one side with respect to thetrack70. Thepit71C is located at a position designated by the symbol C inFIG. 12, being shifted to the side opposite from thepit71B, with respect to thetrack70.
As shown inFIG. 12(a), in the case where thelight beam72 travels on thetrack70 accurately, the respective total amounts of light received by thephotodetector45 at the time when thelight beam72 passes through the positions A, B, and C are as shown inFIG. 12(b). That is, the amount of light received is greatest at the time of passing through the position A, and the amounts of light received at the time of passing through the position B and at the time of passing through the position C are the same, which are lower than the amount at the time of passing through the position A.
On the other hand, as shown inFIG. 13(a), in the case where thelight beam72 travels off thetrack70 with a deviation toward thepit71C, the respective total amounts of light received by thephotodetector45 at the time when thelight beam72 passes through the positions A, B, and C are as shown inFIG. 13(b). That is, the amount of light received is greatest at the time of passing through the position A, second greatest at the time of passing through the position C, and smallest at the time of passing through the position B. The absolute value of difference between the amounts of light received at the time of passing through the position B and at the time of passing through the position C increases with increasing amount of deviation of thelight beam72 from thetrack70.
Although not shown, when thelight beam72 travels off thetrack70 with a deviation toward thepit71B, the amount of light received is greatest at the time of passing through the position A, second greatest at the time of passing through the position B, and smallest at the time of passing through the position C. The absolute value of difference between the amounts of light received at the time of passing through the position B and at the time of passing through the position C increases with increasing amount of deviation of thelight beam72 from thetrack70.
From the foregoing, the direction and magnitude of deviation of thelight beam72 with respect to thetrack70 can be seen from a difference between the amounts of light received at the time of passing through the position B and at the time of passing through the position C. Consequently, the difference between the amounts of light received at the time of passing through the position B and at the time of passing through the position C can be used as a tracking error signal. Thepits71A serve as the reference of timing for detecting the amounts of light received at the time of passing through the position B and at the time of passing through the position C.
Specifically, the tracking servo in this example is performed in the following manner. Initially, the timing at which the total amount of light received by thephotodetector45 reaches a first peak, i.e., the timing of passing through the position A, is detected. Next, the timing of passing through the position B and the timing of passing through the position C are estimated with reference to the timing of passing through the position A. Next, the amount of light received at the time of passing through the position B and the amount of light received at the time of passing through the position C are detected at the respective estimated timing. Finally, a difference between the amounts of light received at the time of passing through the position B and at the time of passing through the position C is detected as a tracking error signal. Then, based on the tracking error signal, tracking servo is performed so that thelight beam72 follows thetrack70 all the time. However, when thelight beam72 passes through theinformation recording areas7, no tracking servo is performed and the state at the time of passing through the previousaddress servo area6 is maintained.
A method for producing the tracking error information and a method for tracking servo in the present embodiment are not limited to the foregoing ones, but a push-pull method may also be used, for example. In this case, theaddress servo areas6 are provided with a row of pits along the direction of the track, as positioning information to be used for tracking servo, and then, a variation in the shape of light incident on the light-receiving surface of thephotodetector45 is detected to produce tracking error information.
Now, with reference toFIG. 14, description will be given of the operation of theoptical head40 at the time of recording information.FIG. 14 shows how a track TR and anirradiating position101 of the information light and the recording-specific reference light move during information recording. InFIG. 14, the symbol R represents the moving direction of therecording medium1. Although for the sake of convenienceFIG. 14 shows the irradiatingposition101 so as not to fall on the track TR, in fact the irradiatingposition101 falls on the track TR.
In the present embodiment, as shown inFIG. 14(a), the irradiatingposition101 is moved off the neutral position in a direction (hereinafter referred to as leading direction) that is opposite to the moving direction R of therecording medium1 before information is recorded in aninformation recording area7 of therecording medium1. Then, the irradiatingposition101 passes through anaddress servo area6, and the information recorded in theaddress servo area6 is detected by theoptical head40.
Next, as shown inFIG. 14(b), when the irradiatingposition101 has reached the end E1 of its moving range in the leading direction, the irradiatingposition101 is then moved in the moving direction R of the recording medium1 (hereinafter referred to as lagging direction). Immediately after the start of movement of the irradiatingposition101 in the lagging direction, the moving speed of the irradiatingposition101 is lower than the moving speed of a desiredinformation recording area7 in which information is to be recorded. Hence, the irradiatingposition101 finally overlaps the desiredinformation recording area7.
As shown inFIG. 14(c), when the irradiatingposition101 overlaps the desiredinformation recording area7, the moving speed of the irradiatingposition101 is adjusted to become equal to the moving speed of theinformation recording area7. Consequently, the irradiatingposition101 is moved so as to follow the desiredinformation recording area7.
Next, as shown inFIG. 14(d), when the irradiatingposition101 has reached the end E2 of its moving range in the lagging direction, the irradiatingposition101 is then moved in the leading direction again to perform the operation shown inFIG. 14(a). In this way, the operations shown inFIG. 14(a)-(d) are repeated.
As described above, in the present embodiment, the irradiatingposition101 of the information light and the recording-specific reference light is moved such that the irradiatingposition101 follows a single movinginformation recording area7 for a predetermined period. Consequently, the singleinformation recording area7 is kept being irradiated with the information light and the recording-specific reference light for the predetermined period. Information is thereby recorded in thisinformation recording area7 in the form of an interference pattern resulting from interference between the information light and the recording-specific reference light. Hereinafter, the period for which theirradiating position101 follows theinformation recording area7 is referred to as a follow-up period, while the other period is referred to as a catch-up period.
FIG. 15 shows the above-described movement of the irradiatingposition101 on the coordinates with the absolute position on the abscissa and the time on the ordinate. As in the foregoing description, the symbols R, E1, and E2 inFIG. 15 represent the moving direction of therecording medium1, the end of the moving range of the irradiatingposition101 in the leading direction, and the end of the moving range of the irradiatingposition101 in the lagging direction. InFIG. 15, the symbol T1 represents the follow-up period, and the symbol T2 represents the catch-up period.
As shown inFIG. 15, in the present embodiment, a singleinformation recording area7 keeps being irradiated with the information light and the recording-specific reference light over the follow-up period T1. An interference pattern resulting from interference between the information light and the recording-specific reference light, i.e., an information-carrying hologram is thereby formed in theinformation recording area7. InFIG. 15, the symbols H1 to H6 represent holograms which are recorded in this order.
The movement of the irradiatingposition101 is effected by moving thehead body41 which includes theobjective lens11, or the point of emission of the information light and the recording-specific reference light, in a direction generally along the tracks. Here,FIG. 16 shows an example of changes in the position of theobjective lens11 and changes in the driving voltage of thecoils155 to158 for moving thehead body41 in the direction generally along the tracks. InFIG. 16, (a) illustrates changes in the position of theobjective lens11, and (b) illustrates changes in the driving voltage.
In the example shown inFIG. 16(a), for the follow-up period T1, theobjective lens11 moves at a constant speed that is equal to the moving speed of theinformation recording area7. During the catch-up period T2, theobjective lens11 stops temporarily at the position of the end of the moving range in the lagging direction, and then starts moving in the leading direction. Reaching the end of the moving range in the leading direction, theobjective lens11 stops temporarily at that position, and then starts moving in the lagging direction at a speed lower than the moving speed of theinformation recording area7.
In the example shown inFIG. 16(b), the driving voltage gives thehead body41 power for moving in the leading direction when it has a positive value. The driving voltage gives thehead body41 power for moving in the lagging direction when it has a negative value.
Next, with reference toFIG. 17, description will be given of a method for adjusting the irradiatingposition101 of the information light and the recording-specific reference light to the position of a desiredinformation recording area7.FIG. 17(c) shows three tracks TR1, TR2, and TR3. In each of the tracks, fourinformation recording areas7 are arranged between two adjacentaddress servo areas6. InFIG. 17(c), the positions of these fourinformation recording areas7 are designated by the symbols a, b, c, and d.
InFIG. 17, (d) and (e) show the traces of the irradiatingposition101 of the information light and the recording-specific reference light in performing recording on the tracks TR1 and TR2, respectively. InFIG. 17(d) andFIG. 17(e), the abscissa represents a relative position of the irradiatingposition101 with respect to the tracks shown inFIG. 17(c), while the ordinate represents the time. In the present embodiment, during the catch-up period T2, the irradiatingposition101 passes through anaddress servo area6 so that the information recorded in theaddress servo area6 is detected by theoptical head40. Based on the detection output of theoptical head40, thecontroller90 inFIG. 2 recognizes the addresses of theinformation recording areas7 that lie between theaddress servo area6 which theirradiating position101 has just passed through and the nextaddress servo area6. While the irradiatingposition101 passes through anaddress servo area6, a basic clock is generated based on the detection output of theoptical head40.
Thecontroller90 selects aninformation recording area7 to record information in, out of the fourinformation recording areas7 lying between two adjacentaddress servo areas6. The positions of the fourinformation recording areas7 lying between the two adjacentaddress servo areas6, or the positions a to d inFIG. 17(c), can be determined by the time that is expressed using the basic clock mentioned above. In accordance with the position of theinformation recording area7 to record information in, thecontroller90 changes the profile of the driving voltage such as the one shown inFIG. 16, thereby adjusting the irradiatingposition101 to the position of thatinformation recording area7.
In the present embodiment, as shown inFIG. 17(d) andFIG. 17(e), information recording on a predetermined track is performed as follows. Initially, while therecording medium1 makes a single turn, information is recorded in each of theinformation recording areas7 that fall on the position a ofFIG. 17 (c) on a single track. During the next turn, information is recorded in each of theinformation recording areas7 that fall on the position b ofFIG. 17 (c) on the same track. Subsequently, during the next turn, information is likewise recorded in each of theinformation recording areas7 that fall on the position c ofFIG. 17(c) on the same track. During the yet next turn, information is recorded in each of theinformation recording areas7 that fall on the position d ofFIG. 17(c) on the same track. When the recording of information on theinformation recording areas7 lying in all the positions a to d on the single track is completed, recording is performed on the next track in the same manner. InFIG. 17(d) andFIG. 17(e), the traces of the irradiatingposition101 for respective turns of therecording medium1 are shown compressed in the direction of the time axis.
By the way, in the catch-up periods T2, the relative speed of the irradiatingposition101 with respect to the recording medium1 (address servo areas6) varies in the order of an increase, constant, and decrease. In the case where the information recorded in theaddress servo areas6 is detected only in the periods where the relative speed of the irradiatingposition101 is constant, the lengths of pits to be recorded in theaddress servo areas6 and the lengths between two adjacent pits may be integer multiples of a reference length, for example. In this case, however, theaddress servo areas6 cannot be made so great in length.
If the information recorded in theaddress servo areas6 is rendered detectable not only in the periods where the relative speed of the irradiatingposition101 is constant but also in the periods where the relative speed of the irradiatingposition101 increases or decreases, theaddress servo areas6 can be made greater in length to record a greater amount of information in theaddress servo areas6. In this case, however, the time of pits and the time between pits in the detection output of theoptical head40 vary depending on the relative speed of the irradiatingposition101 even if the lengths of the pits and the lengths between two adjacent pits are constant. Some measures are thus required in order to generate accurate basic clocks and recognize the information recorded in theaddress servo areas6 with accuracy. Hereinafter, two examples will be given of such measures.
For a first measure, as shown inFIG. 17(a), the reference length to the lengths of the pits P to be recorded in theaddress servo areas6 and to the lengths between two adjacent pits P is changed in proportion to the relative speed of the irradiatingposition101. InFIG. 17(a), the center pit is a special pit indicating the center position of theaddress servo area6.
For a second measure, as shown inFIG. 17(b), the reference length to the lengths of the pits P to be recorded in theaddress servo areas6 and to the lengths between two adjacent pits P is unchanged while thesignal processing circuit89 inFIG. 2 converts the time of pits and the time between pits in the detection output of theoptical head40 into actual lengths of the pits and actual lengths between the pits.
FIG. 18 shows a concrete example of changes in the length of a pit when the foregoing first measure is adopted. InFIG. 18, the ordinate shows the relative speed of the irradiatingposition101 with respect to the recording medium1 (address servo areas6), and the abscissa shows the time. InFIG. 18, the symbols P1 to P8 represent the pits at the respective timing. The pits P1 to P8 shall be considered to have the same length in terms of signal processing. InFIG. 18, the symbol LP represents a change in the power of thesemiconductor laser43. In the first measure, the pits P1 to P8 have lengths proportional to the relative speed of the irradiatingposition101. In the detection output of theoptical head40, the pits P1 to P8 are thus of constant time. Consequently, when the first measure is adopted, the lengths of pits and the lengths between pits can be recognized from the time of the pits and the time between the pits in the detection output of theoptical head40 as is, which allows recognition of the information recorded in theaddress servo areas6.
FIG. 19 shows a concrete example of changes in the time of a pit and the time between pits when the foregoing second measure is adopted.FIG. 19 shows the case where the irradiatingposition101 passes through a pit row having pits of constant length and constant intervals, in a period where the relative speed of the irradiatingposition101 decreases. InFIG. 19, (a) shows a reproduction signal RF outputted from thedetection circuit85 inFIG. 2; and (b) shows the system clock used in the optical information recording/reproducing apparatus. In (a), a high-level period corresponds to the period of a pit, and a low level period corresponds to the period between two adjacent pits. As shown inFIG. 19(a), in the period where the relative speed of the irradiatingposition101 decreases, the time of pits and the time between pits in the reproduction signal RF increase gradually even if the lengths of the pits and the lengths between the pits are constant. Thesignal processing circuit89 inFIG. 2 obtains the information on the relative speed of the irradiatingposition101 from thecontroller90, and multiplies the time of the pits and the time between the pits in the reproduction signal RF by the relative speed of the irradiatingposition101 to determine the lengths of the pits and the lengths between the pits. The lengths of the pits and the lengths between the pits calculated in this way coincide with the actual lengths of the pits and the actual lengths between the pits. Thus, when the second measure is adopted, the lengths of the pits and the lengths between the pits obtained by calculation can be used to recognize the information recorded in theaddress servo areas6.
As has been described, in the present embodiment, the irradiating position of the information light and the recording-specific reference light is moved so as to follow a single movinginformation recording area7 for a predetermined period. As a result, the singleinformation recording area7 is kept being irradiated with the information light and the recording-specific reference light for the predetermined period. Therefore, according to the embodiment, it is possible to irradiate theinformation recording areas7 with the information light and the recording-specific reference light for a sufficient time period to record information in theinformation recording areas7 without causing a deviation between theinformation recording areas7 and the irradiating position of the information light and the recording-specific reference light. Consequently, according to the embodiment it is possible to record information in each of a plurality ofinformation recording areas7 through the use of holography with thesemiconductor laser43, which is a practical light source, while rotationally moving therecording medium1 having the plurality ofinformation recording areas7.
In the present embodiment, therecording medium1 is provided with theaddress servo areas6. Theaddress servo areas6 contain address information for identifying the individualinformation recording areas7 and positioning information for adjusting the irradiating position of the information light, the recording-specific reference light, and the reproduction-specific reference light with respect to the individualinformation recording areas7. The optical information recording/reproducing apparatus detects the address information recorded in theaddress servo areas6 and thereby identifies the individualinformation recording areas7. According to the present embodiment, it is thus easy to identify the individualinformation recording areas7. In addition, the optical information recording/reproducing apparatus detects the positioning information recorded in theaddress servo areas6, and thereby adjusts the irradiating position of the information light, the recording-specific reference light, and the reproduction-specific reference light with respect to the individualinformation recording areas7. According to the present embodiment, the irradiating position of the information light, the recording-specific reference light, and the reproduction-specific reference light can thus be easily adjusted to the individualinformation recording areas7.
In the present embodiment, for information recording, theinformation recording layer3 of therecording medium1 is irradiated with the information light that is spatially modulated in phase based on information to be recorded, and the recording-specific reference light, so that the information is recorded on theinformation recording layer3 in the form of an interference pattern resulting from interference between the information light and the recording-specific reference light. For information reproduction, theinformation recording layer3 is irradiated with the reproduction-specific reference light. Then, reproduction light thereby generated from theinformation recording layer3 is superimposed on the reproduction-specific reference light to produce composite light, and this composite light is detected to reproduce the information.
Consequently, according to the present embodiment, the reproduction light and the reproduction-specific reference light need not be separated from each other at the time of information reproduction. Then, at the time of information recording, it is not necessary that the information light and the recording-specific reference light form a predetermined angle therebetween when incident on the recording medium. In fact, in the embodiment, irradiation with the information light, the recording-specific reference light and the reproduction-specific reference light, and collection of the reproduction light are performed on the same side of theinformation recording layer3 such that the information light, the recording-specific reference light, the reproduction-specific reference light and the reproduction light are arranged coaxially. Accordingly, the present embodiment allows a compact configuration of the optical system for recording and reproduction.
In conventional methods for reproduction, the reproduction light and the reproduction-specific reference light are separated to detect the reproduction light alone. Hence, there has been a problem that the reproduced information deteriorates in S/N ratio if the reproduction-specific reference light is also incident on the photodetector for detecting the reproduction light. On the contrary, in the present embodiment, both the reproduction light and the reproduction-specific reference light are used to reproduce information, and therefore the S/N ratio of the reproduced information cannot be deteriorated by the reproduction-specific reference light. Consequently, the present embodiment can improve the S/N ratio of the reproduced information.
Moreover, according to the present embodiment, the information light, the recording-specific reference light, and the reproduction-specific reference light are all arranged coaxially and converge to become minimum in diameter at the same position. The optical system for recording and reproduction can thus be simplified in configuration.
Second Embodiment Next, description will be given of an optical information recording/reproducing apparatus according to a second embodiment of the invention.FIG. 20 is a plan view showing the driving mechanism of an optical head of the optical information recording/reproducing apparatus according to the present embodiment. The present embodiment differs from the first embodiment as to the driving mechanism of the optical head.
Theoptical head40 of the present embodiment has a fixedportion201, a firstmovable portion202, and a secondmovable portion203. The fixedportion201 is fixed to the body of the optical information recording/reproducing apparatus. Tworails221 extending in a direction of the radius of the recording medium1 (vertical direction inFIG. 20) are attached to the body of the optical information recording/reproducing apparatus. The firstmovable portion202 is supported by the tworails221 so as to be movable in a direction of the radius of therecording medium1. Theoptical head40 further haslinear motors222 for moving the firstmovable portion202 with respect to the body of the optical information recording/reproducing apparatus in a direction of the radius of therecording medium1.
Tworails231 extending in a direction tangential to the tracks (horizontal direction inFIG. 20) are attached to the firstmovable portion202. The secondmovable portion203 is supported by the tworails231 so as to be movable in a direction tangential to the tracks. Theoptical head40 further haslinear motors232 for moving the secondmovable portion203 with respect to the firstmovable portion202 in a direction tangential to the tracks.
Asupport plate204 for supporting theobjective lens11 to be movable in a direction perpendicular to the surface of the recording medium1 (a direction orthogonal to the plane of the drawing sheet ofFIG. 20) is attached to the secondmovable portion203. Theoptical head40 also has anactuator241 for moving theobjective lens11 with respect to the secondmovable portion203 in a direction perpendicular to the surface of therecording medium1.
In theoptical head40 of the present embodiment, of the recording/reproducing optical system, theobjective lens11 is attached to thesupport plate204, while most of the other parts are provided on the fixedportion201. The firstmovable portion202 and the secondmovable portion203 have a relay optical system for directing the light LB from the optical system provided on the fixedportion201 to theobjective lens11 and for directing the light incident on theobjective lens11 from therecording medium1 to the optical system provided on the fixedportion201.FIG. 20 shows amirror223 which is fixed to the firstmovable portion202 and constitutes part of the relay optical system.
According to theoptical head40 of the present embodiment, theactuator241 can change the position of theobjective lens11 in a direction perpendicular to the surface of therecording medium1, thereby allowing focus servo. In addition, according to theoptical head40, thelinear motors222 can change the position of theobjective lens11 in a direction of the radius of therecording medium1, thereby allowing access to a desired track and tracking servo. Furthermore, according to theoptical head40, thelinear motors232 can change the position of theobjective lens11 in a direction tangential to the tracks, i.e., in a direction generally along the tracks. This allows control of the irradiating position of the information light and the recording-specific reference light to follow theinformation recording areas7. Thelinear motors232 correspond to the irradiating position moving device of the invention.
Theactuator241 is driven by thefocus servo circuit86 shown inFIG. 2. Thelinear motors222 are driven by the trackingservo circuit87 and theslide servo circuit88 shown inFIG. 2. Thelinear motors232 are driven by the follow-upcontrol circuit94 shown inFIG. 2.
In the present embodiment, the drivingdevice84 shown inFIG. 2 is not provided because theoptical head40 has the function of the drivingdevice84. The present embodiment is not provided with the function of correcting the relative inclination between therecording medium1 and theoptical head40. Thus, theinclination correction circuit93 shown inFIG. 2 is not provided.
The remainder of the configuration, operations, and effects of the present embodiment are the same as those of the first embodiment.
Third Embodiment Next, description will be given of an optical information recording/reproducing apparatus according to a third embodiment of the invention.FIG. 21 is an explanatory diagram showing essential parts of a recording/reproducing optical system of the optical information recording/reproducing apparatus according to the present embodiment.
First, with reference toFIG. 21, description will given of a configuration of a recording medium according to the present embodiment. Therecording medium301 according to the present embodiment is disk-shaped and has a plurality of tracks, like therecording medium1 of the first embodiment. Each of the tracks has a plurality ofaddress servo areas306 arranged at regular intervals. One or moreinformation recording areas307 are provided between adjacent ones of theaddress servo areas306.
Therecording medium301 comprises two disk-shapedtransparent substrates302 and304 made of polycarbonate or the like, aninformation recording layer303 provided between thetransparent substrates302 and304, and aprotective layer305 provided to be adjacent to a surface of thetransparent substrate302 opposite to theinformation recording layer303.
Theinformation recording layer303 is a layer on which information is recorded through the use of holography, and is made of the same hologram material as that for theinformation recording layer3 of therecording medium1 of the first embodiment.
In therecording medium301, the surface of theprotective layer305 opposite to the transparent substrate302 (the lower surface inFIG. 21) acts as afirst surface301aon which recording-specific reference light and reproduction-specific reference light are incident and from which reproduction light exits. The surface of thetransparent substrate304 opposite to the information recording layer303 (the upper surface inFIG. 21) acts as asecond surface301bon which information light carrying information to be recorded is incident.
In theaddress servo areas306, emboss pits for expressing address information and the like are formed in the interface between thetransparent substrate302 and theprotective layer305. Focus servo may also be performed by using the interface between thetransparent substrate302 and theprotective layer305.
As shown inFIG. 22, therecording medium301 may be designed such that the emboss pits for expressing address information and the like are formed in the interface between thetransparent substrate302 and theinformation recording layer303 in theaddress servo areas306. In this case, theprotective layer305 is unnecessary.
Now, with reference toFIG. 21, description will be given of essential parts of the recording/reproducing optical system of the optical information recording/reproducing apparatus according to the present embodiment. The recording/reproducing optical system has anobjective lens321 that faces toward thetransparent substrate304 of therecording medium301, and a quarter-wave plate322 and apolarization beam splitter323 that are arranged in this order from theobjective lens321, on a side of theobjective lens321 opposite from therecording medium301. Thepolarization beam splitter323 has a polarizationbeam splitter surface323afor reflecting S-polarized light and transmitting P-polarized light. The polarizationbeam splitter surface323aforms 45° with the surface of therecording medium301. In thepolarization beam splitter323, the surface on the right side inFIG. 21 serves as an informationlight incidence surface323b. The recording/reproducing optical system further has a spatiallight modulator327 which is disposed on the optical path of light incident on the informationlight incidence surface323bof thepolarization beam splitter323. The spatiallight modulator327 has a number of pixels arranged in a matrix, and is capable of generating information light that carries information by spatially modulating the intensity of outgoing light, by selecting, for example, a light-transmitting state or a light-blocking state for each of the pixels. For example, a liquid crystal device may be used as the spatiallight modulator327.
The recording/reproducing optical system further has anobjective lens331 that faces toward theprotective layer305 of therecording medium301, and a quarter-wave plate332, apolarization beam splitter333, and aphotodetector334 that are arranged in this order from theobjective lens331, on a side of theobjective lens331 opposite from therecording medium301. Thepolarization beam splitter333 has a polarizationbeam splitter surface333afor reflecting S-polarized light and transmitting P-polarized light. The polarizationbeam splitter surface333aforms 45° with the surface of therecording medium301. In thepolarization beam splitter333, the surface on the right side inFIG. 21 serves as a referencelight incidence surface333b. The recording/reproducing optical system further has a phase spatiallight modulator338 which is disposed on the optical path of light incident on the referencelight incidence surface333bof thepolarization beam splitter333. The phase spatiallight modulator338 has a number of pixels arranged in a matrix, and is capable of spatially modulating the phase of light by selecting the phase of outgoing light from between two values or from among three or more values for each of the pixels.
Thephotodetector334 has a number of pixels arranged in a matrix, and is capable of detecting the intensity of light received by each pixel. A CCD type solid state image pick-up device, a MOS type solid state image pick-up device, or a smart optical sensor may be used for thephotodetector334.
A general configuration of the recording/reproducing optical system of the optical information recording/reproducing apparatus according to the present embodiment will now be described with reference toFIG. 23.
Initially, description will be given of the parts of the recording/reproducing optical system related to information light. The recording/reproducing optical system has theobjective lens321, the quarter-wave plate322, and thepolarization beam splitter323 described above. The recording/reproducing optical system further has aconvex lens324, apin hole325, aconvex lens326, and the spatiallight modulator327 that are arranged in this order from thepolarization beam splitter323 on the optical path of light incident on the informationlight incidence surface323bof thepolarization beam splitter323.
Theconvex lens324 and theconvex lens326 have the same focal length. The focal length shall be indicated by fs. The center of theconvex lens324, thepin hole325, the center of theconvex lens326, and the image forming plane of the spatiallight modulator327 are arranged at intervals of the focal length fs. Thus, parallel beams having passed through the spatiallight modulator327 are collected by theconvex lens326 to become minimum in diameter at the position of thepin hole325, and pass through thepin hole325. The light having passed through thepin hole325 becomes diverging light, and is incident on theconvex lens324. It then becomes parallel beams to be incident on the informationlight incidence surface323bof thepolarization beam splitter323. Animage plane351 conjugate to the image forming plane of the spatiallight modulator327 is formed between theconvex lens324 and thepolarization beam splitter323 at a distance of the focal length fs from the center of theconvex lens324.
Where f1 represents a distance between the center of thepolarization beam splitter323 and theimage plane351, f2 represents a distance between the center of thepolarization beam splitter323 and the center of theobjective lens321, and f represents the focal length of theobjective lens321, there holds f=f1+f2. The interface between thetransparent substrate302 and theprotective layer305 of therecording medium301 is located at a distance of the focal length f from the center of theobjective lens321. With such a configuration, it is possible to locate the spatiallight modulator327 at a distance from theobjective lens321, which allows greater design flexibility in the optical system.
Now, description will be given of the parts of the recording/reproducing optical system related to recording-specific reference light, reproduction-specific reference light, and reproduction light. The recording/reproducing optical system has theobjective lens331, the quarter-wave plate332, thepolarization beam splitter333, and thephotodetector334 described previously. The recording/reproducing optical system further has apolarization beam splitter335 which is disposed on the optical path of light incident on the referencelight incidence surface333bof thepolarization beam splitter333. Thepolarization beam splitter335 has a polarizationbeam splitter surface335afor reflecting S-polarized light and transmitting P-polarized light. The polarizationbeam splitter surface335alies in parallel with the polarizationbeam splitter surface333aof thepolarization beam splitter333.
The recording/reproducing optical system further has aconvex lens336, aconcave lens337, and the phase spatiallight modulator338 that are arranged in this order from thepolarization beam splitter335, below thepolarization beam splitter335 inFIG. 23. The phase spatiallight modulator338 is of reflection type. Animage plane352 conjugate to the image forming plane of the phase spatiallight modulator338 is formed between thepolarization beam splitter335 and thepolarization beam splitter333.
The distance between the center of thepolarization beam splitter333 and theimage plane352 is f1, the same as the distance between the center of thepolarization beam splitter323 and theimage plane351. The distance between the center of thepolarization beam splitter333 and the center of theobjective lens331 is f2, the same as the distance between the center of thepolarization beam splitter323 and the center of theobjective lens321. The focal length of theobjective lens331 is f, the same as the focal length of theobjective lens321. The interface between thetransparent substrate302 and theprotective layer305 of therecording medium301 is located at a distance of the focal length f from the center of theobjective lens331. With such a configuration, it is possible to locate the phase spatiallight modulator338 at a distance from theobjective lens331, which allows greater design flexibility in the optical system.
Above thepolarization beam splitter335 inFIG. 23, the recording/reproducing optical system further has amirror339 disposed to form 90° with respect to the polarizationbeam splitter surface335a, and amirror340 disposed in parallel with themirror339.
Now, description will be given of the parts of the recording/reproducing optical system common to the information light, the recording-specific reference light, and the reproduction-specific reference light. The recording/reproducing optical system has asemiconductor laser342 that emits coherent linearly polarized laser light, and acollimator lens343, amirror344, a rotation-causingoptical element345, and apolarization beam splitter346 that are arranged in this order from thesemiconductor laser342 on the optical path of the light emitted from thesemiconductor laser342. For example, a half-wave plate or an optical rotation plate is used as the rotation-causingoptical element345. Thepolarization beam splitter346 has a polarizationbeam splitter surface346afor reflecting S-polarized light and transmitting P-polarized light.
For plain representation of the essential parts of the recording/reproducing optical system shown inFIG. 23,FIG. 21 shows the spatiallight modulator327 as being located at the position of theimage plane351 and the phase spatiallight modulator338 as being transmission type and located at the position of theimage plane352.
Description will now be given of the outline of operation of the recording/reproducing optical system shown inFIG. 23. Thesemiconductor laser342 emits S-polarized linear light or P-polarized linear light. Thecollimator lens343 collimates the light emitted by thesemiconductor laser342 into parallel beams for exit therefrom. The rotation-causingoptical element345 optically rotates the light that has exited thecollimator lens343 and has been reflected by themirror344, to emit light including S-polarized components and P-polarized components.
The S-polarized components of the light having exited the rotation-causingoptical element345 are reflected by the polarizationbeam splitter surface346aof thepolarization beam splitter346 to be incident on the spatiallight modulator327. The spatiallight modulator327 spatially modulates the intensity of the light to generate information light. The information light having exited the spatiallight modulator327 passes through theconvex lens326, thepin hole325, and theconvex lens324 in succession, and is reflected by the polarizationbeam splitter surface323aof thepolarization beam splitter323 to be incident on the quarter-wave plate322. The information light having passed through the quarter-wave plate322 becomes circularly polarized light, is collected by theobjective lens321, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. The optical system consisting of theconvex lens326, thepin hole325, and theconvex lens324 may exercise spatial filtering.
On the other hand, the P-polarized components of the light having exited the rotation-causingoptical element345 are transmitted through the polarizationbeam splitter surface346aof thepolarization beam splitter346, reflected by themirrors340 and339, transmitted through the polarizationbeam splitter surface335aof thepolarization beam splitter335, pass through theconvex lens336 and theconcave lens337, and impinge on the phase spatiallight modulator338 as parallel beams. For example, the phase spatiallight modulator338 sets the phase of outgoing light to either of two values differing by π (rad) from each other for each pixel, thereby spatially modulating the phase of the light. The light modulated by the phase spatiallight modulator338 serves as recording-specific reference light or reproduction-specific reference light. Furthermore, the phase spatiallight modulator338 rotates the direction of polarization of outgoing light by 90° with respect to the direction of polarization of incident light. The light that exits the phase spatiallight modulator338 thus becomes S-polarized light. The light having exited the phase spatiallight modulator338 passes through theconcave lens337 and theconvex lens336, is reflected by the polarizationbeam splitter surface335aof thepolarization beam splitter335, and is further reflected by the polarizationbeam splitter surface333aof thepolarization beam splitter333 to be incident on the quarter-wave plate332. The light having passed through the quarter-wave plate332 becomes circularly polarized light, is collected by theobjective lens331, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305.
Return light that results when the light applied to therecording medium301 by theobjective lens331 is reflected off the interface between thetransparent substrate302 and theprotective layer305, or reproduction light that occurs from theinformation recording layer303 according to the reproduction-specific reference light applied to therecording medium301 by theobjective lens331 is collimated through theobjective lens331, passes through the quarter-wave plate332 to become P-polarized light, and passes through the polarizationbeam splitter surface333aof thepolarization beam splitter333 to be incident on thephotodetector334.
When therecording medium301 is configured as shown inFIG. 22, the light from theobjective lens321 and the light from theobjective lens331 are both applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theinformation layer303.
Next, with reference toFIG. 24, description will be given of the configuration of the optical information recording/reproducing apparatus according to the present embodiment. The optical information recording/reproducingapparatus310 has an optical headlower portion40A, an optical headupper portion40B, and a fixedportion40C instead of theoptical head40 and the drivingdevice84 in the optical information recording/reproducingapparatus10 according to the first embodiment which is shown inFIG. 2. The optical headlower portion40A is placed under therecording medium301 to irradiate therecording medium301 with recording-specific reference light or reproduction-specific reference light and to collect reproduction light. The optical headupper portion40B is placed over therecording medium301 to irradiate therecording medium301 with information light. The fixedportion40C is fixed to the body of the optical information recording/reproducingapparatus310.
Among the components of the recording/reproducing optical system shown inFIG. 23, the optical headlower portion40A contains theobjective lens331, the quarter-wave plate332, thepolarization beam splitter333, thephotodetector334, thepolarization beam splitter335, theconvex lens336, theconcave lens337, the phase spatiallight modulator338, and themirror339. Among the components of the recording/reproducing optical system shown inFIG. 23, the optical headupper portion40B contains theobjective lens321, the quarter-wave plate322, thepolarization beam splitter323, theconvex lens324, thepin hole325, theconvex lens326, and the phase spatiallight modulator327. The fixedportion40C contains thesemiconductor laser342, thecollimator lens343, themirror344, the rotation-causingoptical element345, thepolarization beam splitter346, and themirror340.
The optical headlower portion40A and the optical headupper portion40B are each driven by the same driving mechanism as that of theoptical head40 shown inFIG. 20, while maintaining an opposite positional relationship with each other with therecording medium301 in between. In the present embodiment, the drivingdevice84 shown inFIG. 2 is not provided because the optical headlower portion40A and the optical headupper portion40B each have the function of the drivingdevice84. The present embodiment is not provided with the function of correcting the relative inclinations of therecording medium301 to the optical headlower portion40A and the optical headupper portion40B. Thus, theinclination correction circuit93 shown inFIG. 2 is not provided. The circuit configuration of the optical information recording/reproducingapparatus310 is otherwise the same as that of the optical information recording/reproducingapparatus10 shown inFIG. 2.
According to the optical headlower portion40A and the optical headupper portion40B of the present embodiment, theactuator241 inFIG. 20 can change the positions of theobjective lenses321,331 in a direction perpendicular to the surface of therecording medium301, thereby allowing focus servo. Additionally, according to the optical headlower portion40A and the optical headupper portion40B, thelinear motors222 inFIG. 20 can change the positions of theobjective lenses321,331 in a direction of the radius of therecording medium301, thereby allowing access to a desired track and tracking servo. Furthermore, according to the optical headlower portion40A and the optical headupper portion40B, thelinear motors232 can change the positions of theobjective lenses321,331 in a direction tangential to the tracks, i.e., in a direction generally along the tracks. This allows control of the irradiating position of the information light and the recording-specific reference light to follow theinformation recording areas307.
Thesemiconductor laser342, the spatiallight modulator327, and the phase spatiallight modulator338 are controlled by thecontroller90 shown inFIG. 24. Thecontroller90 holds information on a plurality of modulation patterns for spatially modulating the phase of light with the phase spatiallight modulator338. The operatingportion91 can select any one of the plurality of modulation patterns. Then, thecontroller90 supplies the information on a modulation pattern selected by itself according to predetermined conditions or a modulation pattern selected by the operatingportion91 to the phase spatiallight modulator338. In accordance with the information on the modulation pattern supplied by thecontroller90, the phase spatiallight modulator338 spatially modulates the phase of light in the corresponding modulation pattern.
Servo, information recording, and information reproducing operations of the optical information recording/reproducing apparatus according to the embodiment will now be separately described in succession.
The servo operation will now be described with reference toFIG. 23 andFIG. 25.FIG. 25 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during the servo operation. During the servo operation, all the pixels of the spatiallight modulator327 are brought into a blocking state. The phase spatiallight modulator338 is set such that light passing through every pixel thereof has the same phase. The power of light emitted by thesemiconductor laser342 is set to a low level suitable for reproduction. Thecontroller90 predicts the timing at which light that has exited theobjective lens331 passes through theaddress servo areas306 based on the basic clock reproduced from the reproduction signal RF, and maintains the foregoing setting while the light that has exited theobjective lens331 passes through theaddress servo areas306.
The light emitted by thesemiconductor laser342 is collimated by thecollimator lens343 and passes through themirror344 and the rotation-causingoptical element345 to be incident on thepolarization beam splitter346. S-polarized components of the light incident on thepolarization beam splitter346 are reflected by the polarizationbeam splitter surface346aand are blocked by the spatiallight modulator327.
P-polarized components of the light incident on thepolarization beam splitter346 are transmitted through the polarizationbeam splitter surface346a, pass through themirrors340 and339, are transmitted through the polarizationbeam splitter surface335aof thepolarization beam splitter335, pass through theconvex lens336 and theconcave lens337, and are incident on the phase spatiallight modulator338. Since the phase spatiallight modulator338 rotates the direction of polarization of outgoing light by 90° with respect to the direction of polarization of incident light, the light that exits the phase spatiallight modulator338 becomes S-polarized light. The light that has exited the phase spatiallight modulator338 passes through theconcave lens337 and theconvex lens336, is reflected by the polarizationbeam splitter surface335aof thepolarization beam splitter335, and is further reflected by the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on the quarter-wave plate332. The light having passed through the quarter-wave plate332 becomes circularly polarized light, is collected by theobjective lens331, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305.
Return light that is generated when the light applied to therecording medium301 by theobjective lens331 is reflected off the interface between thetransparent substrate302 and theprotective layer305 is collimated through theobjective lens331, passes through the quarter-wave plate332 to become P-polarized light, and passes through the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on thephotodetector334. Based on the output of thephotodetector334, the detection circuit385 generates a focus error signal FE, a tracking error signal TE, and a reproduction signal RF. Focus servo and tracking servo are performed, the basic clock is reproduced, and addresses are determined based on these signals.
For the above-described setting for the servo operation, the configuration of the optical headlower portion40A is similar to that of the optical head for recording and reproduction on a typical optical disk. Thus, the optical information recording/reproducing apparatus of the embodiment allows recording and reproduction using a typical optical disk.
An information recording operation will now be described with reference toFIG. 23 andFIG. 26.FIG. 26 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during the recording operation. During the recording operation, the spatiallight modulator327 spatially modulates the intensity of light passing therethrough by selecting a transmitting state (hereinafter also referred to as ON) or a blocking state (hereinafter also referred to as OFF) for each pixel according to the information to be recorded, to thereby generate information light. The phase spatiallight modulator338 spatially modulates the phase of light passing therethrough by selectively giving the light a phase difference of either 0 (rad) or π (rad) from a predetermined reference phase for each pixel according to a predetermined modulation pattern, to thereby generate recording-specific reference light having a spatially modulated phase.
Thecontroller90 supplies the information on the modulation pattern selected by itself in accordance with predetermined conditions or the modulation pattern selected by the operatingportion91 to the phase spatiallight modulator338, and the phase spatiallight modulator338 spatially modulates the phase of light passing therethrough in accordance with the information on the modulation pattern supplied by thecontroller90.
The power of light emitted by thesemiconductor laser342 is set to reach high levels on a pulse basis suitable for recording. Under the control of thecontroller90, while the light that has exited theobjective lenses321 and331 passes through an area other than theaddress servo areas306, neither focus servo nor tracking servo is performed.
The light emitted by thesemiconductor laser342 is collimated by thecollimator lens343 and passes through themirror344 and the rotation-causingoptical element345 to be incident on thepolarization beam splitter346. S-polarized components of the light incident on thepolarization beam splitter346 are reflected by the polarizationbeam splitter surface346aand pass through the spatiallight modulator327, at which time the light is spatially modulated in intensity in accordance with the information to be recorded, to become information light. This information light passes through theconvex lens326, thepin hole325, and theconvex lens324 in succession, and is reflected by the polarizationbeam splitter surface323aof thepolarization beam splitter323 to impinge on the quarter-wave plate322. The information light having passed through the quarter-wave plate322 becomes circularly polarized light, is collected by theobjective lens321, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. As shown inFIG. 26, the information light passes through theinformation recording layer303 in therecording medium301 while converging.
P-polarized components of the light incident on thepolarization beam splitter346 are transmitted through the polarizationbeam splitter surface346a, pass through themirrors340 and339, are transmitted through the polarizationbeam splitter surface335aof thepolarization beam splitter335, pass through theconvex lens336 and theconcave lens337, and impinge on the phase spatiallight modulator338 to become recording-specific reference light, being spatially modulated in phase. Since the recording-specific reference light exiting from the phase spatiallight modulator338 becomes S-polarized light, it passes through theconcave lens337 and theconvex lens336, is reflected by the polarizationbeam splitter surface335aof thepolarization beam splitter335, and is further reflected by the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on the quarter-wave plate332. The recording-specific reference light having passed through the quarter-wave plate332 becomes circularly polarized light, is collected by theobjective lens331, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. As shown inFIG. 26, the recording-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
In this way, for recording, the information light and the recording-specific reference light are coaxially applied to opposite sides of theinformation recording layer303 while converging to become minimum in diameter at the same position (on the interface between thetransparent substrate302 and the protective layer305). The information light and the recording-specific reference light interfere with each other to form an interference pattern in theinformation recording layer303. When the power of the light emitted by thesemiconductor laser342 has reached a high level for recording, the interference pattern is volumetrically recorded in theinformation recording layer303 to form a reflection-type (Lippmann-type) hologram.
According to the present embodiment, a plurality of pieces of information can be recorded in an identical location of theinformation recording layer303 on a multiplex basis through phase-encoding multiplexing by changing the modulation pattern of the phase of the recording-specific reference light for each piece of the information to be recorded.
In the embodiment, a method called shift multiplexing may also be used to record a plurality of pieces of data on a multiplex basis. Shift multiplexing is a method for recording a plurality of pieces of information on a multiplex basis by forming a plurality of hologram forming regions corresponding to the respective pieces of information in theinformation recording layer303 such that the hologram forming regions are slightly shifted from each other and overlap each other in a horizontal direction.
The multiplex recording through phase-encoding multiplexing or the multiplex recording through shift multiplexing may be used alone, or both of them may be used in combination.
An information reproducing operation will now be described with reference toFIG. 23 andFIG. 27.FIG. 27 is an explanatory diagram showing a state of the essential parts of the recording/reproducing optical system during the reproducing operation. During the reproducing operation, all pixels of the spatiallight modulator327 are brought into a blocking state. The phase spatiallight modulator338 spatially modulates the phase of light passing therethrough by selectively giving the light a phase difference of either 0 (rad) or π (rad) from a predetermined reference phase for each pixel according to a predetermined modulation pattern, to thereby generate reproduction-specific reference light having a spatially modulated phase.
Thecontroller90 supplies the information on the modulation pattern selected by itself in accordance with predetermined conditions or the modulation pattern selected by the operatingportion91 to the phase spatiallight modulator338, and the phase spatiallight modulator338 spatially modulates the phase of light passing therethrough in accordance with the information on the modulation pattern supplied by thecontroller90.
The power of the light emitted by thesemiconductor laser342 is set to a low level suitable for reproduction. Under the control of thecontroller90, while the light that has exited theobjective lenses321 and331 passes through an area other than theaddress servo areas306, neither focus servo nor tracking servo is performed.
The light emitted by thesemiconductor laser342 is collimated by thecollimator lens343 and passes through themirror344 and the rotation-causingoptical element345 to be incident on thepolarization beam splitter346. S-polarized components of the light incident on thepolarization beam splitter346 are reflected by the polarizationbeam splitter surface346aand blocked by the spatiallight modulator327.
P-polarized components of the light incident on thepolarization beam splitter346 are transmitted through the polarizationbeam splitter surface346a, pass through themirrors340 and339, are transmitted through the polarizationbeam splitter surface335aof thepolarization beam splitter335, pass through theconvex lens336 and theconcave lens337, and are incident on the phase spatiallight modulator338 to become reproduction-specific reference light, being spatially modulated in phase. Since the reproduction-specific reference light exiting from the phase spatiallight modulator338 becomes S-polarized light, it passes through theconcave lens337 and theconvex lens336, is reflected by the polarizationbeam splitter surface335aof thepolarization beam splitter335, and is further reflected by the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on the quarter-wave plate332. The reproduction-specific reference light having passed through the quarter-wave plate332 becomes circularly polarized light, is collected by theobjective lens331, and is applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. As shown inFIG. 27, the reproduction-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
Upon application of the reproduction-specific reference light, reproduction light that corresponds to the information light used for recording is generated in theinformation recording layer303. The reproduction light travels toward thetransparent substrate302 while converging, becomes minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305, and exits therecording medium301 while diverging. Then, the light is collimated through theobjective lens331, passes through the quarter-wave plate332 to become P-polarized light, and passes through the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on thephotodetector334.
On thephotodetector334 is formed an image of the ON/OFF pattern caused by the spatiallight modulator327 in the recording operation, so that information is reproduced by detecting this pattern. When a plurality of pieces of information are recorded in theinformation recording layer303 on a multiplex basis by changing modulation patterns of the recording-specific reference light, among the plurality of pieces of information, the one corresponding to the modulation pattern of the reproduction-specific reference light is only reproduced.
In this way, for reproduction, the reproduction-specific reference light is applied to therecording medium301 to converge to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. The application of the reproduction-specific reference light and the collection of the reproduction light are performed on the incidence side for the recording-specific reference light on therecording medium301. The reproduction-specific reference light and the reproduction light are arranged coaxially.
As has been described, in the present embodiment, the optical headupper portion40B and the optical headlower portion40A move the irradiating position of the information light and the recording-specific reference light such that the irradiating position of the information light and the recording-specific reference light follows a single movinginformation recording area307 for a predetermined period. As a result, the singleinformation recording area307 is kept being irradiated with the information light and the recording-specific reference light for the predetermined period.
Moreover, according to the present embodiment, the information light, the recording-specific reference light, and the reproduction-specific reference light are all arranged coaxially and converge to become minimum in diameter at the same position. The optical system for recording and reproduction can thus be simplified in configuration.
According to the embodiment, the information light can carry information using the entire cross section of the beam thereof. Likewise, the reproduction light can also carry information using the entire cross section of the beam thereof.
From the foregoing, the embodiment makes it possible to record and reproduce information through the use of holography and to simplify the configuration of the optical system for recording and reproduction without causing a reduction in the amount of information.
In the embodiment, therecording medium301 is provided with positioning areas (address servo areas306) in which information for alignment of the information light, the recording-specific reference light, and the reproduction-specific reference light is recorded. The recording/reproducing optical system applies the information light, the recording-specific reference light, and the reproduction-specific reference light to therecording medium301, letting them converge to become minimum in diameter at the position where the positioning areas are provided. The positioning areas are irradiated with light that converges, like the recording-specific reference light and the reproduction-specific reference light, to become minimum in diameter at the position where the positioning areas are provided, and return light from the positioning areas is detected. It is thereby possible to position the information light, the recording-specific reference light, and the reproduction-specific reference light by using the information recorded in the positioning areas. Thus, the embodiment allows precise positioning of the information light, the recording-specific reference light, and the reproduction-specific reference light with respect to therecording medium301 without complicating the configuration of the recording/reproducing optical system.
Furthermore, in the embodiment, because the positioning areas are located on the incidence side for the recording-specific reference light with respect to theinformation recording layer303, return light from the positioning areas will not pass through theinformation recording layer303. This prevents the light used for positioning from being disturbed by theinformation recording layer303, and it is thus possible to prevent deterioration in the reproduction accuracy of the information for positioning.
The remainder of the configuration, operations, and effects of the present embodiment are the same as those of the first or second embodiment.
Fourth Embodiment Now, description will be given of an optical information recording/reproducing apparatus according to a fourth embodiment of the invention.FIG. 28 is an explanatory diagram showing a general configuration of a recording/reproducing optical system of the optical information recording/reproducing apparatus according to the present embodiment.
In the present embodiment, information light is generated by spatially modulating the phase of light based on the information to be recorded. The recording/reproducing optical system of the embodiment has a phase spatiallight modulator347 instead of the spatiallight modulator327 inFIG. 23. Besides, ashutter348 for selecting a light-transmitting state or a light-blocking state is provided between the phase spatiallight modulator347 and thepolarization beam splitter346. The phase spatiallight modulator347 has a number of pixels arranged in a matrix, and is capable of spatially modulating the phase of light by selecting the phase of outgoing light from between two values or from among three or more values for each of the pixels. For example, a liquid crystal device may be used for the phase spatiallight modulator347. Theshutter348 may also be a liquid crystal device.
Servo, information recording, and information reproducing operations of the optical information recording/reproducing apparatus according to the embodiment will now be separately described in succession.
The servo operation will now be described. During the servo operation, theshutter348 is brought into a blocking state. The remainder of the servo operation is the same as in the third embodiment.
Now, with reference toFIG. 29, a recording operation will be described for situations where information is recorded using information light whose phase is spatially modulated and recording-specific reference light whose phase is not spatially modulated.FIG. 29 is an explanatory diagram showing the state of essential parts of the recording/reproducing optical system during the recording operation. During the recording operation, theshutter348 is brought into a transmitting state. The phase spatiallight modulator347 spatially modulates the phase of light by selecting the phase of outgoing light from between two values or from among three or more values for each pixel according to the information to be recorded. Here, for ease of explanation, the phase spatiallight modulator347 shall spatially modulate the phase of the light by setting the phase of the outgoing light to either a first phase having a phase difference of +π/2 (rad) from a predetermined reference phase or a second phase having a phase difference of −π/2 (rad) from the reference phase for each pixel. The phase difference between the first phase and the second phase is π (rad). In this way, information light having a spatially modulated phase is generated. The information light locally drops in intensity at the borders between first-phase pixels and second-phase pixels.
As in the third embodiment, the information light is collected by theobjective lens321 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the information light passes through theinformation recording layer303 in therecording medium301 while converging.
Here, the phase spatiallight modulator338 generates recording-specific reference light by setting the phase of outgoing light to the first phase having a phase difference of +π/2 (rad) from the predetermined reference phase for every pixel, without spatially modulating the phase of the light. The phase spatiallight modulator338 may set the phase of the outgoing light for every pixel to the second phase or a certain phase different from both the first phase and the second phase.
InFIG. 29, the symbol “+” represents the first phase, and the symbol “−” the second phase.FIG. 29 also shows the maximum value of intensity as “1”, and the minimum value of intensity as “0”.
As in the third embodiment, the recording-specific reference light is collected by theobjective lens331 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the recording-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
As in the third embodiment, the information light and the recording-specific reference light interfere with each other to form an interference pattern in theinformation recording layer303. When the power of the light emitted by thesemiconductor laser342 has reached a high level suitable for recording, the interference pattern is volumetrically recorded in theinformation recording layer303 to form a reflection-type (Lippmann-type) hologram.
Now, with reference toFIG. 30, an operation for reproducing information that is recorded using the information light whose phase is spatially modulated and the recording-specific reference light whose phase is not spatially modulated.FIG. 30 is an explanatory diagram showing the state of the essential parts of the recording/reproducing optical system during the reproducing operation. During the reproducing operation, theshutter348 is brought into a blocking state. The phase spatiallight modulator338 generates reproduction-specific reference light by setting the phase of outgoing light to the first phase having a phase difference of +π/2 (rad) from the predetermined reference phase for every pixel, without spatially modulating the phase of the light. InFIG. 30, the phases and intensities are indicated in the same manner as inFIG. 29.
As in the third embodiment, the reproduction-specific reference light is collected by theobjective lens331 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the reproduction-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
Upon application of the reproduction-specific reference light, reproduction light that corresponds to the information light used for recording is generated in theinformation recording layer303. The reproduction light has a spatially modulated phase, as is the case with the information light used for recording. The reproduction light travels toward thetransparent substrate302 while converging, becomes minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305, and exits therecording medium301 while diverging. Then, the light is collimated through theobjective lens331, passes through the quarter-wave plate332 and the polarizationbeam splitter surface333aof thepolarization beam splitter333, and is incident on thephotodetector334.
Part of the reproduction-specific reference light applied to therecording medium301 is reflected off the interface between thetransparent substrate302 and theprotective layer305, and exits therecording medium301 while diverging. It is then collimated through theobjective lens331, and passes through the quarter-wave plate332 and the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on thephotodetector334.
In reality, the reproduction light is superimposed on the reproduction-specific reference light that is reflected off the interface between thetransparent substrate302 and theprotective layer305 to generate composite light, and this composite light is received by thephotodetector334. The composite light has an intensity that is spatially modulated according to the information recorded. Thus, thephotodetector334 detects a two-dimensional intensity pattern of the composite light, from which the information is reproduced.
Now, with reference toFIG. 31, detailed description will be given of the reproduction light, the reproduction-specific reference light, and the composite light used for reproduction mentioned above. InFIG. 31, (a) shows the intensity of the reproduction light, (b) shows the phase of the reproduction light, (c) shows the intensity of the reproduction-specific reference light, (d) shows the phase of the reproduction-specific reference light, and (e) shows the intensity of the composite light.FIG. 31 shows an example where the phase of the information light for each pixel is set to either the first phase having a phase difference of +π/2 (rad) from the reference phase, or the second phase having a phase difference of −π/2 (rad) from the reference phase. Consequently, in the example shown inFIG. 31, the reproduction light has either the first phase or the second phase pixel by pixel as the information light does. The reproduction-specific reference light has the first phase for every pixel. Assuming here that the reproduction light and the reproduction-specific reference light are equal in intensity, the composite light exceeds the reproduction light and the reproduction-specific reference light in intensity at pixels where the reproduction light has the first phase, and the composite light theoretically becomes zero in intensity at pixels where the reproduction light has the second phase, as shown inFIG. 31(e).
Now, with reference toFIG. 32, a recording operation will be described for situations where information is recorded using information light whose phase is spatially modulated and recording-specific reference light whose phase is spatially modulated.FIG. 32 is an explanatory diagram showing the state of the essential parts of the recording/reproducing optical system during the recording operation. During the recording operation, theshutter348 is brought into a transmitting state. The phase spatiallight modulator347 spatially modulates the phase of light by selecting the phase of outgoing light from between two values or from among three or more values each pixel according to the information to be recorded. Here, for ease of explanation, the phase spatiallight modulator347 shall spatially modulate the phase of the light by setting the phase of the outgoing light to either the first phase or the second phase for each pixel. In this way, information light having a spatially modulated phase is generated.
As in the third embodiment, the information light is collected by theobjective lens321 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the information light passes through theinformation recording layer303 in therecording medium301 while converging.
The phase spatiallight modulator338 spatially modulates the phase of light by selecting the phase of outgoing light from between two values or from among three or more values for each pixel. Here, the phase spatiallight modulator338 shall spatially modulate the phase of the light by setting, for each pixel, the phase of the outgoing light to any one of a predetermined reference phase, a first phase having a phase difference of +π/2 (rad) from the reference phase, and a second phase having a phase difference of −π/2 (rad) from the reference phase. InFIG. 32, the reference phase is represented by the symbol “0”. InFIG. 32, the phases and intensities are otherwise indicated in the same manner as inFIG. 29. The recording-specific reference light locally drops in intensity at portions where the phase changes.
As in the third embodiment, the recording-specific reference light is collected by theobjective lens331 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the recording-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
As in the third embodiment, the information light and the recording-specific reference light interfere with each other to form an interference pattern in theinformation recording layer303. When the power of the light emitted by thesemiconductor laser342 has reached a high level suitable for recording, the interference pattern is volumetrically recorded in theinformation recording layer303 to form a reflection-type (Lippmann-type) hologram.
Now, with reference toFIG. 33, an operation for reproducing information that is recorded using the information light whose phase is spatially modulated and the recording-specific reference light whose phase is spatially modulated.FIG. 33 is an explanatory diagram showing the state of the essential parts of the recording/reproducing optical system during the reproducing operation. During the reproducing operation, theshutter348 is brought into a blocking state. As is the case with the recording operation, the phase spatiallight modulator338 spatially modulates the phase of outgoing light to generate reproduction-specific reference light having a spatially modulated phase. InFIG. 33, the phases and intensities are indicated in the same manner as inFIG. 32.
As in the third embodiment, the reproduction-specific reference light is collected by theobjective lens331 and applied to therecording medium301 while converging to become minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305. Then, the reproduction-specific reference light passes through theinformation recording layer303 in therecording medium301 while diverging.
Upon application of the reproduction-specific reference light, reproduction light that corresponds to the information light used for recording is generated in theinformation recording layer303. The reproduction light has a spatially modulated phase, as the information light used for recording does. The reproduction light travels toward thetransparent substrate302 while converging, becomes minimum in diameter on the interface between thetransparent substrate302 and theprotective layer305, and exits therecording medium301 while diverging. Then, the light is collimated through theobjective lens331, and passes through the quarter-wave plate332 and the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on thephotodetector334.
Part of the reproduction-specific reference light applied to therecording medium301 is reflected off the interface between thetransparent substrate302 and theprotective layer305, and exits therecording medium301 while diverging. It is then collimated through theobjective lens331, and passes through the quarter-wave plate332 and the polarizationbeam splitter surface333aof thepolarization beam splitter333 to impinge on thephotodetector334.
In reality, the reproduction light is superimposed on the reproduction-specific reference light that is reflected off the interface between thetransparent substrate302 and theprotective layer305 to generate composite light, and this composite light is received by thephotodetector334. The composite light has an intensity which is spatially modulated according to the information recorded. Thus, thephotodetector334 detects a two-dimensional intensity pattern of the composite light, from which the information is reproduced.
Now, with reference toFIG. 34, detailed description will be given of the reproduction light, the reproduction-specific reference light, and the composite light used for reproduction mentioned above. InFIG. 34, (a) shows the intensity of the reproduction light, (b) shows the phase of the reproduction light, (c) shows the intensity of the reproduction-specific reference light, (d) shows the phase of the reproduction-specific reference light, and (e) shows the intensity of the composite light.FIG. 34 show an example where the phase of the information light is set at either the first phase or the second phase for each pixel, and the phases of the recording-specific reference light and the reproduction-specific reference light are set at any one of the reference phase, the first phase, and the second phase for each pixel. In this case, the phase of the reproduction light for each pixel is either the first phase or the second phase, as is the case with the information light. Consequently, the phase difference between the reproduction light and the reproduction-specific reference light is any of zero, +π/2 (rad), and ±π (rad). Suppose here that the intensity of the reproduction light and the intensity of the reproduction-specific reference light are equal. In that case, as shown inFIG. 34(e), the intensity of the composite light becomes maximum at pixels where the phase difference between the reproduction light and the reproduction-specific reference light is zero, and becomes theoretically zero at pixels where the phase difference between the reproduction light and the reproduction-specific reference light is ±π (rad). At pixels where the phase difference between the reproduction light and the reproduction-specific reference light is ±π/2 (rad), the intensity becomes ½ that at a zero-phase-difference pixel. InFIG. 34(e), the intensity at the pixels where the phase difference is ±π (rad) is represented by “0”, the intensity at the pixels where the phase difference is ±π/2 (rad) is represented by “1”, and the intensity at the pixels where the phase difference is zero is represented by “2”.
In the example shown inFIG. 32 toFIG. 34, the intensity of the composite light at each pixel has three values. Then, for example, the intensity “0” can be associated with two bits of data “00”, the intensity “1” with two bits of data “01”, and the intensity “2” with two bits of data “10” as shown inFIG. 34(e). Thus, in the example shown inFIG. 32 toFIG. 34, the composite light can carry an increased amount of information with the same intensity and phase of the reproduction light as compared to the cases where the intensity of the composite light at each pixel has two values as shown inFIG. 29 toFIG. 31. As a result, therecording medium301 can be enhanced in recording density.
As described in the foregoing, in the present embodiment, to record information, theinformation recording layer303 of therecording medium301 is irradiated with the information light that is spatially modulated in phase based on information to be recorded and the recording-specific reference light, so that the information is recorded in theinformation recording layer303 in the form of an interference pattern resulting from interference between the information light and the recording-specific reference light. Then, to reproduce the information, theinformation recording layer303 is irradiated with the reproduction-specific reference light. Reproduction light thereby generated from theinformation recording layer303 is superimposed on the reproduction-specific reference light to produce composite light, and this composite light is detected to thereby reproduce the information.
Consequently, according to the present embodiment, the reproduction light and the reproduction-specific reference light need not be separated from each other when reproducing information. Thus, when recording information, it is not necessary that the information light and the recording-specific reference light form a predetermined angle therebetween when incident on the recording medium. The embodiment therefore allows a compact configuration of the optical system for recording and reproduction.
In the conventional methods for reproduction, the reproduction light and the reproduction-specific reference light are separated to detect the reproduction light alone. Hence, there has been a problem that the reproduced information deteriorates in S/N ratio if the reproduction-specific reference light is also incident on the photodetector for detecting the reproduction light. On the contrary, in the present embodiment, since the reproduction light and the reproduction-specific reference light are both used to reproduce information, the reproduction-specific reference light will not deteriorate the S/N ratio of the reproduced information. Consequently, the present embodiment makes it possible to improve the S/N ratio of the reproduced information.
The remainder of the configuration, operations, and effects of the present embodiment are the same as those of the third embodiment.
Fifth Embodiment Next, description will be given of an optical information recording/reproducing apparatus according to a fifth embodiment of the invention. As with the fourth embodiment, the present embodiment is designed such that information light is generated by modulating the phase of light spatially based on the information to be recorded. It differs from the fourth embodiment, however, as to the driving mechanism of the optical head and the configuration of the recording/reproducing optical system.
FIG. 35 is a plan view showing the optical head and a recording medium of the present embodiment.FIG. 36 is a cross-sectional view showing the configuration of the optical head of the present embodiment.FIG. 37 is a cross-sectional view showing the configuration of the recording medium of the present embodiment.
As shown inFIG. 35 andFIG. 36, the optical information recording/reproducing apparatus according to the present embodiment has anoptical head440 and adriving device484 instead of theoptical head40 and the drivingdevice84 in the optical information recording/reproducingapparatus10 according to the first embodiment which is shown inFIG. 2. The present embodiment is not provided with the function of correcting the relative inclinations of arecording medium401 to theoptical head440. Thus, theinclination correction circuit93 shown inFIG. 2 is not provided. The circuit configuration of the optical information recording/reproducing apparatus according to the embodiment is otherwise the same as that of the optical information recording/reproducingapparatus10 shown inFIG. 2.
Theoptical head440 has a firstmovable portion441 and a secondmovable portion442. The firstmovable portion441 is moved by the drivingdevice484 in a direction of the radius of therecording medium401 of the present embodiment. The secondmovable portion442 has alower arm portion442A to be placed under therecording medium401, anupper arm portion442B to be placed over therecording medium401, and acoupling portion442C for coupling thelower arm portion442A and theupper arm portion442B at a position outside the outer periphery of therecording medium401. The extremities of thelower arm portion442A and theupper arm portion442B are located at opposite positions across therecording medium401.
Thecoupling portion442C is rotatably coupled to the firstmovable portion441 viaball bearings443. Twocoils444 for irradiating-position follow-up are attached to an end of thecoupling portion442C opposite from thelower arm portion442A and theupper arm portion442B. In the firstmovable portion441, twomagnets445 are placed at opposite positions across each of thecoils444. In theoptical head440, the secondmovable portion442 can be rotated with respect to the firstmovable portion441 by means of thecoils444 and themagnets445 so as to change the positions of the extremities of thelower arm portion442A and theupper arm portion442B in directions generally along the tracks of therecording medium401.
Next, with reference toFIG. 36, description will be given of the configuration of the recording/reproducing optical system provided inside the secondmovable portion442. The recording/reproducing optical system has a recording/reproducing semiconductor laser411 and aservo semiconductor laser412 which are fixed to an inside end of thecoupling portion442C opposite from thelower arm portion442A and theupper arm portion442B. The recording/reproducing optical system further has acollimator lens413, adichroic mirror414, a phase spatiallight modulator415 of transmission type, apolarization beam splitter416, arelay lens system417, a quarter-wave plate418, and amirror419 that are arranged in this order from theservo semiconductor laser412 on the optical path of light emitted from thesemiconductor laser412. Thedichroic mirror414 has a reflecting surface which reflects light of predetermined wavelengths and transmits light of other wavelengths. This reflecting surface reflects the light emitted from the recording/reproducing semiconductor laser411, and transmits the light emitted from theservo semiconductor laser412. Thepolarization beam splitter416 has a polarization beam splitter surface which reflects or transmits light depending on the direction of polarization of the light.
The recording/reproducing optical system further has anobjective lens420 which is disposed in the extremity of thelower arm portion442A and faces the bottom surface of therecording medium401, and anactuator421 which moves theobjective lens420 in a direction perpendicular to the surface of therecording medium401. Themirror419 reflects light that is incident from the quarter-wave plate418, and guides the light to theobjective lens420. The recording/reproducing optical system further has aphotodetector422 for receiving light that is incident on thepolarization beam splitter416 from therelay lens system417 and reflected by the polarization beam splitter surface thereof.
The recording/reproducing optical system further has a collimator lens423, a half-wave plate424, apolarization beam splitter425, and amirror426 that are arranged in this order from the recording/reproducing semiconductor laser411 on the optical path of the light emitted from the semiconductor laser411. Thepolarization beam splitter425 has a polarization beam splitter surface. Themirror426 reflects light incident from thepolarization beam splitter425, and guides the light to the reflecting surface of thedichroic mirror414.
The recording/reproducing optical system further has apolarization beam splitter427 disposed on the optical path of light that is incident on thepolarization beam splitter425 from the half-wave plate424 and reflected by the polarization beam splitter surface thereof. The recording/reproducing optical system further has ashutter428, a half-wave plate429, a phase spatiallight modulator430 of transmission type, apolarization beam splitter431, arelay lens system432, a quarter-wave plate433, and amirror434 that are arranged in this order from thepolarization beam splitter427 on the optical path of light that is incident from thepolarization beam splitter425 on thepolarization beam splitter427 and reflected by the polarization beam splitter surface thereof. Thepolarization beam splitter431 has a polarization beam splitter surface.
The recording/reproducing optical system further has anobjective lens435 which is disposed in the extremity of theupper arm portion442B and faces the top surface of therecording medium401, and anactuator436 which moves theobjective lens435 in a direction perpendicular to the surface of therecording medium401. Themirror434 reflects light that is incident from the quarter-wave plate433, and guides the light to theobjective lens436. The recording/reproducing optical system further has aphotodetector437 for receiving light that is incident on thepolarization beam splitter431 from therelay lens system432 and reflected by the polarization beam splitter surface thereof.
Next, with reference toFIG. 37, description will given of the configuration of therecording medium401 of the present embodiment. Therecording medium401 is disk-shaped and has a plurality of tracks, like therecording medium1 of the first embodiment. Each of the tracks has a plurality of address servo areas arranged at regular intervals. One or more information recording areas are provided between adjacent ones of the address servo areas.
Therecording medium401 comprises two disk-shapedtransparent substrates402 and404 made of polycarbonate or the like, aspacer406 for separating thesetransparent substrates402 and404 at a predetermined distance, aninformation recording layer403 provided between thetransparent substrates402 and404, and atransparent substrate405 bonded to a surface of thetransparent substrate404 opposite from theinformation recording layer403 via abonding layer407.
Theinformation recording layer403 is a layer in which information is recorded through the use of holography, and is made of a hologram material having sensitivity to light of a predetermined wavelength range. The recording/reproducing semiconductor laser411 emits light having a wavelength to which the hologram material constituting theinformation recording layer403 has sensitivity. Theservo semiconductor laser412 emits light having a wavelength that falls outside the wavelength range to which the hologram material constituting theinformation recording layer403 has sensitivity. Possible combinations of wavelength of the light emitted from the recording/reproducing semiconductor laser411 and the wavelength of the light emitted from theservo semiconductor laser412 include a combination of 650 nm and 780 nm, a combination of 523 nm and 650 nm, and a combination of 405 nm and 650 nm.
In the address servo areas, emboss pits for expressing address information and the like are formed at a surface of thetransparent substrate405 closer to thetransparent substrate404. Focus servo may also be performed by using the surface of thetransparent substrate405 closer to thetransparent substrate404.
In therecording medium401, the total optical thickness of thetransparent substrate402, theinformation recording layer403, thetransparent substrate404, and thebonding layer407 is equal to the optical thickness of thetransparent substrate405.
In therecording medium401, the surface of thetransparent substrate405 opposite from the transparent substrate404 (the bottom surface inFIG. 37) serves as the surface on which recording-specific reference light and reproduction-specific reference light are incident and from which reproduction light is emitted. The surface of thetransparent substrate402 opposite from the information recording layer403 (the top surface inFIG. 37) serves as the surface on which information light that carries information to be recorded is incident.
Servo, information recording, and information reproducing operations of theoptical head440 in the present embodiment will now be separately described in succession. Initially, description will be given of the servo operation. During the servo operation, theservo semiconductor laser412 emits light, whereas the recording/reproducing semiconductor laser411 will not emit light. Theservo semiconductor laser412 emits P-polarized light. The light emitted from thesemiconductor laser412 is collimated by thecollimator lens413, is transmitted through the reflecting surface of thedichroic mirror414, passes through the phase spatiallight modulator415, is transmitted through the polarization beam splitter surface of thepolarization beam splitter416, passes through therelay lens system417, and passes through the quarter-wave plate418 to become circularly-polarized light. This light is reflected by themirror419 to impinge on theobjective lens420, and is collected by theobjective lens420. Then, the light is applied to therecording medium401 while converging to become minimum in diameter on the surface of thetransparent substrate405 closer to thetransparent substrate404.
The light applied to therecording medium401 from theobjective lens420 is reflected by the surface of thetransparent substrate405 closer to thetransparent substrate404 to cause return light. The return light is collimated through theobjective lens420, reflected by themirror419, and passes through the quarter-wave plate418 to become S-polarized light. This light passes through therelay lens system417 and is reflected by the polarization beam splitter surface of thepolarization beam splitter416 to impinge on thephotodetector422. Based on the output of thephotodetector422, a focus error signal on theobjective lens420 is obtained by the same method as that described in conjunction withFIG. 11, for example. Based on this focus error signal, theactuator421 adjusts the position of theobjective lens420 to effect focus servo on theobjective lens420.
The light that has been applied to therecording medium401 from theobjective lens420 and has passed through therecording medium401 is collimated through theobjective lens435, reflected by themirror434, and passes through the quarter-wave plate433 to become S-polarized light. This light passes through therelay lens system432 and is reflected by the polarization beam splitter surface of thepolarization beam splitter431 to impinge on thephotodetector437. Based on the output of thephotodetector437, a focus error signal on theobjective lens435 is obtained by the same method as that described in conjunction withFIG. 11, for example. Based on this focus error signal, theactuator436 adjusts the position of theobjective lens435 to effect focus servo on theobjective lens435.
Based on the output of at least either one of thephotodetectors422 and437, a tracking error signal is obtained by the same method as that described in conjunction withFIG. 12 andFIG. 13, for example. In addition, based on the output of at least either one of thephotodetectors422 and437, a basic clock is generated and addresses are recognized.
Next, description will be given of an information recording operation. At the time of recording, the recording/reproducing semiconductor laser411 emits light, whereas theservo semiconductor laser412 will not emit light. During the recording operation, theshutter428 is brought into a transmitting state. The phase spatiallight modulator430 selects the phase of outgoing light from between two values or from among three or more values for each pixel based on the information to be recorded, thereby modulating the phase of the light spatially to generate information light. The phase spatiallight modulator415 selects the phase of outgoing light from between two values or from among three or more values for each pixel in accordance with a predetermined modulation pattern, thereby modulating the phase of the light spatially to generate recording-specific reference light.
Thecontroller90 supplies the information on the modulation pattern selected by itself in accordance with predetermined conditions or the modulation pattern selected by the operatingportion91 to the phase spatiallight modulator415, and the phase spatiallight modulator415 spatially modulates the phase of light passing therethrough in accordance with the information on the modulation pattern supplied by thecontroller90. The power of the light emitted by the recording/reproducing semiconductor laser411 is set to reach high levels on a pulse basis suitable for recording. Under the control of thecontroller90, while the light that has exited theobjective lenses420 and435 passes through an area other than the address servo areas, neither focus servo nor tracking servo is performed.
The recording/reproducing semiconductor laser411 emits P-polarized or S-polarized light. The light emitted from the semiconductor laser411 passes through the half-wave plate424 to become light that contains a P-polarized component and an S-polarized component. The light of the P-polarized component from the half-wave plate424 is transmitted through the polarization beam splitter surface of thepolarization beam splitter425, reflected by themirror426, and reflected by the reflecting surface of thedichroic mirror414. This light passes through the phase spatiallight modulator415 to become recording-specific reference light. This recording-specific reference light is transmitted through the polarization beam splitter surface of thepolarization beam splitter416, passes through therelay lens system417, and passes through the quarter-wave plate418 to become circularly-polarized light. This recording-specific reference light is reflected by themirror419 to impinge on theobjective lens420, and is collected by theobjective lens420. Then, the light is applied to therecording medium401 while converging to become minimum in diameter on the surface of thetransparent substrate405 closer to thetransparent substrate404. The recording-specific reference light passes through theinformation recording layer403 in therecording medium401 while diverging.
Meanwhile, the light of the S-polarized component from the half-wave plate424 is reflected by the polarization beam splitter surface of thepolarization beam splitter425, and further reflected by the polarization beam splitter surface of thepolarization beam splitter427. Then, it passes through theshutter428 and through the half-wave plate429 to become P-polarized light. This light passes through the phase spatiallight modulator430 to become information light. This information light is transmitted through the polarization beam splitter surface of thepolarization beam splitter431, passes through therelay lens system432, and passes through the quarter-wave plate433 to become circularly-polarized light. This information light is reflected by themirror434 to impinge on theobjective lens435, and is collected by theobjective lens435. Then, the light is applied to therecording medium401 while converging to become minimum in diameter on the surface of thetransparent substrate405 closer to thetransparent substrate404. The information light passes through theinformation recording layer403 in therecording medium401 while converging.
In the present embodiment, the optical length of the optical path that leads from the recording/reproducing semiconductor laser411 to theobjective lens420 is equal to the optical length of the optical path that leads from the recording/reproducing semiconductor laser411 to theobjective lens435.
The information light and the recording-specific reference light interfere with each other to form an interference pattern in theinformation recording layer403. When the power of the light emitted by the semiconductor laser411 has reached a high level suitable for recording, the interference pattern is volumetrically recorded in theinformation recording layer403 to form a reflection-type (Lippmann-type) hologram.
Next, description will be given of an information reproducing operation. At the time of reproduction, the recording/reproducing semiconductor laser411 emits light, whereas theservo semiconductor laser412 will not emit light. During the reproducing operation, theshutter428 is brought into a blocking state. The phase spatiallight modulator415 selects the phase of outgoing light from between two values or from among three or more values for each pixel in accordance with a predetermined modulation pattern, thereby modulating the phase of the light spatially to generate reproduction-specific reference light. The reproduction-specific reference light follows the same path as with the recording-specific reference light, and is applied to therecording medium401 while converging to become minimum in diameter on the surface of thetransparent substrate405 closer to thetransparent substrate404. The reproduction-specific reference light passes through theinformation recording layer403 in therecording medium401 while diverging.
Upon application of the reproduction-specific reference light, reproduction light that corresponds to the information light used for recording is generated in theinformation recording layer403. This reproduction light has a spatially modulated phase, as with the information light used for recording. The reproduction light travels toward thetransparent substrate405 while converging, becomes minimum in diameter on the surface of thetransparent substrate405 closer to thetransparent substrate404, and exits therecording medium401 while diverging. Then, the light is collimated through theobjective lens420, reflected by themirror419, and passes through the quarter-wave plate418 to become S-polarized light. This reproduction light passes through therelay lens system417, and is reflected by the polarization beam splitter surface of thepolarization beam splitter416 to impinge on thephotodetector422.
Part of the reproduction-specific reference light applied to therecording medium401 is reflected by the surface of thetransparent substrate405 closer to thetransparent substrate404, and exits therecording medium401 while diverging. Then, the light is collimated through theobjective lens420, reflected by themirror419, and passes through the quarter-wave plate418 to become S-polarized light. This reproduction light passes through therelay lens system417, and is reflected by the polarization beam splitter surface of thepolarization beam splitter416 to impinge on thephotodetector422.
In reality, the reproduction light is superimposed on the reproduction-specific reference light that is reflected by the surface of thetransparent substrate405 closer to thetransparent substrate404 to generate composite light, and this composite light is received by thephotodetector422. The composite light has an intensity that is spatially modulated according to the information recorded. Thus, thephotodetector422 detects a two-dimensional intensity pattern of the composite light, from which the information is reproduced.
The principles of information recording and reproduction in the present embodiment are the same as those of the fourth embodiment.
In the present embodiment, theactuators421 and436 can change the positions of theobjective lenses420 and435 in a direction perpendicular to the surface of therecording medium401, thereby effecting focus servo. In addition, in the present embodiment, the drivingdevice484 shown inFIG. 35 can move the entireoptical head440 in a direction of the radius of therecording medium401 to change the positions of theobjective lenses420 and435 in the direction of the radius of therecording medium401. This allows access to desired tracks and tracking servo. Furthermore, in the present embodiment, the secondmovable portion442 is rotatably moved by thecoils444 and themagnets445 with respect to the firstmovable portion441, so that the positions of theobjective lenses420 and435 are changed in a direction generally along the tracks. This allows such control that the irradiating position of the information light and the recording-specific reference light follows the information recording areas. In this control, as with the first embodiment, such driving voltages as shown inFIG. 16(b) may be supplied to thecoils444 to change the positions of theobjective lenses420 and435 as inFIG. 16(a). The positions of theobjective lenses420 and435 may also be changed by a simpler method as described below.
Here, with reference toFIG. 38, description will be given of the simpler method for changing the positions of theobjective lenses420 and435.FIG. 38 shows an example of changes in the positions of theobjective lenses420,435 and changes in the driving voltage of thecoils444. InFIG. 38, (a) shows changes in the positions of theobjective lenses420 and435, and (b) shows changes in the driving voltage. In this method, as shown inFIG. 38(a), the positions of theobjective lenses420 and435 are put into simple harmonic motion about a neutral position. Then, in this method, the period where the moving speed of the positions of theobjective lenses420 and435 becomes nearly equal to the moving speed of the information recording areas in therecording medium401 shall be referred to as a follow-up period T1. The other period shall be referred to as a catch-up period T2.
The positions of theobjective lenses420 and435 can be changed as shown inFIG. 38(a) by using the driving voltage that traces a sine wave as shown inFIG. 38(b). Such a driving voltage can be generated easily by configuring an oscillating circuit and a resonant circuit. When a plurality of information recording areas are provided between two adjacent address servo areas, an information recording area for the positions of theobjective lenses420 and435 to follow up is selectable by controlling the phase of the driving voltage.
The simplified control method shown inFIG. 38 may also be used in the first to fourth embodiments.
The remainder of the configuration, operations, and effects of the present embodiment are the same as those of the fourth embodiment.
The present invention is not limited to the foregoing embodiments but may be modified in various ways. For example, the invention is applicable not only to the apparatuses that record information on a rotating disk-shaped recording medium, but to ones that record information on such a recording medium as card-shaped one which moves linearly.
In the foregoing embodiments, the address information and the like are recorded in advance in the form of emboss pits in the address servo areas of the recording medium. However, the address information and the like may be recorded in the following manner without providing the emboss pits in advance. In this case, the information recording layer is irradiated with high-power laser light selectively at a portion closer to one of its surfaces. The portion is thereby selectively changed in refractive index so that address information and the like are recorded for formatting.
As has been described, in the optical information recording apparatus or method of the invention, the irradiating position of the information light and the reference light is moved so as to follow a single moving information recording area for a predetermined period. As a result, the single information recording area is kept being irradiated with the information light and the reference light for the predetermined period. Therefore, according to the invention, it is possible to irradiate the information recording areas with the information light and the reference light for a sufficient time period to record information in the information recording areas without causing a deviation between the information recording areas and the irradiating position of the information light and the reference light. Consequently, according to the invention, it is possible to record information in each information recording area of a recording medium having a plurality of information recording areas through the use of holography with a practical light source, while moving the recording medium.
The optical information recording apparatus of the invention may comprise a detector for detecting identification information for identifying the individual information recording areas. In this case, it becomes easy to identify the individual information recording areas.
The optical information recording apparatus of the invention may comprise a detector for detecting positioning information for adjusting the irradiating position of the information light and the reference light with respect to the individual information recording areas. In this case, it becomes easy to adjust the irradiating position of the information light and the reference light with respect to the individual information recording areas.
In the optical information recording apparatus of the invention, the information light and the reference light may be applied to the same side of the information recording area coaxially so as to converge to become minimum in diameter at an identical position. In this case, the optical system for recording can be simplified in configuration.
In the optical information recording apparatus of the invention, the information light and the reference light may be applied to opposite sides of the information recording area coaxially so as to converge to become minimum in diameter at an identical position. In this case, the optical system for recording can be simplified in configuration.
It is apparent from the foregoing description that the invention may be carried out in various modes and may be modified in various ways. It is therefore to be understood that within the scope of equivalence of the appended claims the invention may be practiced in modes other than the foregoing best modes.