WO2007052639A1 - Optical pickup device, irradiating method, information recording device and information reproducing device, and computer program - Google Patents

Optical pickup device, irradiating method, information recording device and information reproducing device, and computer program Download PDF

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Publication number
WO2007052639A1
WO2007052639A1 PCT/JP2006/321718 JP2006321718W WO2007052639A1 WO 2007052639 A1 WO2007052639 A1 WO 2007052639A1 JP 2006321718 W JP2006321718 W JP 2006321718W WO 2007052639 A1 WO2007052639 A1 WO 2007052639A1
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WO
WIPO (PCT)
Prior art keywords
filter
light
light intensity
control means
transmission amount
Prior art date
Application number
PCT/JP2006/321718
Other languages
French (fr)
Japanese (ja)
Inventor
Naoharu Yanagawa
Akira Shirota
Original Assignee
Pioneer Corporation
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Pioneer Corporation filed Critical Pioneer Corporation
Priority to JP2007542748A priority Critical patent/JPWO2007052639A1/en
Publication of WO2007052639A1 publication Critical patent/WO2007052639A1/en

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Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/135Means for guiding the beam from the source to the record carrier or from the record carrier to the detector
    • G11B7/1365Separate or integrated refractive elements, e.g. wave plates
    • G11B7/1369Active plates, e.g. liquid crystal panels or electrostrictive elements
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
    • G11B7/126Circuits, methods or arrangements for laser control or stabilisation
    • G11B7/1263Power control during transducing, e.g. by monitoring

Definitions

  • Optical pickup device irradiation method, information recording device, information reproducing device, and computer program
  • the present invention relates to an optical pickup device used for recording and reproducing data on an information recording medium such as an optical disc, a method of irradiating emitted light in the optical pickup device, an information recording device and an information reproducing device including the optical pickup device,
  • the present invention also relates to a computer program that causes a computer to operate as such an information recording device or information reproducing device.
  • an optical disc such as DVD-R or DVD-RW has a constant temperature on the optical disc when the total amount of laser light irradiated per unit time exceeds a predetermined threshold.
  • a predetermined threshold When the value exceeds the value, thermal decomposition or phase change of the dye occurs, whereby various data are recorded.
  • the rotational speed of the optical disk is increased in order to increase the recording speed, data cannot be recorded unless the amount of laser beam energy (ie, laser beam power) applied to the optical disk is increased. Therefore, in order to improve the recording speed, it is essential to increase the power of the laser beam output from the light source.
  • a drive power of about 800 mA is used to output laser light with a power of about 300 mW. It is necessary to supply the current to the laser drive circuit force laser element. In order to further improve the recording speed, it is necessary to output laser light with a power greater than 300 mW, for example, and it is necessary to supply a large drive current of 800 mA or more to the laser element from the laser drive circuit, for example. Also come out.
  • the pulse width of the laser beam also decreases, for example, D
  • VD 16x speed recording it is necessary to output a strict square wave laser beam with a pulse width on the order of Ins to 30 ns.
  • the present invention has been made in view of the above-described conventional problems, for example, an optical pickup device capable of performing a suitable recording operation while suppressing heat dissipation, and a method for irradiating emitted light. It is an object of the present invention to provide an information recording device, an information reproducing device, and a computer program.
  • the optical pickup device of the present invention includes a light source for irradiating the recording surface of the information recording medium with the emitted light, a light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape, A filter disposed on the optical path of the outgoing light and configured to change a transmission amount of the incident outgoing light; and a filter control unit configured to control the filter so as to change the transmission amount of the outgoing light.
  • the emitted light emitted from the light source including the laser element or the like is irradiated onto the recording surface of the information recording medium.
  • the intensity of the emitted light is controlled by the operation of light intensity control means including a laser drive circuit.
  • the emitted light is emitted from the light source with the first light intensity that is relatively strong (or relatively large) capable of forming a light source.
  • the recording mark formed on the recording surface of the information recording medium, or the recording pit is not destroyed or erased.
  • the emitted light is emitted from the light source at a second light intensity that is relatively weak (or relatively small).
  • the light intensity of the emitted light is controlled by the operation of the light intensity control means so that the light intensity of the emitted light changes in a substantially sinusoidal waveform.
  • “change to a substantially sine wave shape” is intended to indicate a state in which the light intensity changes more slowly than when the light intensity is changed in a strict square wave shape. That is, it is intended to indicate a state in which the light intensity is increased relatively slowly and decreased relatively slowly by the operation of the light intensity control means.
  • the filter can increase or decrease the transmission amount of the outgoing light incident on the filter. How much outgoing light is transmitted is controlled by the operation of the filter control means. That is, the transmission amount of the filter is controlled by the operation of the filter control means.
  • the filter control means changes the transmission amount of the filter so that the transmission amount of the filter changes in a substantially square wave shape.
  • the emitted light emitted with the light intensity changing to a substantially sinusoidal shape passes through the filter, and the light intensity changing to the square wave shape is obtained.
  • the recording surface of the information recording medium is irradiated. In other words, it is not necessary to change the light intensity of the emitted light into a strict square wave shape when the emitted light is irradiated from the light source. For this reason, the light intensity changing means can change the light intensity of the emitted light while suppressing the amount of heat generation.
  • the operation of the filter and the filter control means causes the emitted light to have a light intensity that changes to a square wave shape. Irradiates the recording surface. For this reason, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be suitably recorded.
  • the optical pickup device of the present invention it is preferable to suppress heat dissipation and A recording operation can be performed.
  • the filter control unit controls the filter so as to change a transmission amount of the filter according to data recorded on the information recording medium.
  • the emitted light is irradiated onto the recording surface of the information recording medium with the light intensity that changes to a square wave shape according to the data to be recorded. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, it is possible to perform a suitable recording operation while suppressing heat dissipation.
  • the filter control means changes the transmission amount of the filter according to a strategy pulse corresponding to data recorded on the information recording medium. Control the filter.
  • the emitted light is irradiated onto the recording surface of the information recording medium with a light intensity that changes to a square wave shape.
  • the light emitted from the light source is usually emitted with a light intensity that changes to a square wave shape according to the strategy pulse.
  • the light is emitted with a light intensity that changes to a square wave shape according to the strategy pulse.
  • the amount of transmission of the filter is changed so that the incident light passes through the filter.
  • the light source force is emitted in the same manner as when the emitted light is emitted with the light intensity changing to the square wave shape.
  • the emitted light is applied to the recording surface of the information recording medium with a light intensity that changes to a square wave shape. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
  • the strategy pulse includes a first pulse having a predetermined first amplitude and a first pulse smaller than the first amplitude. At least a second pulse having two amplitudes, wherein the filter control means increases the transmission amount of the filter in response to the first pulse than the transmission amount of the filter in response to the second pulse. Control the filter to Make it.
  • the transmission amount of the filter can be changed according to the amplitude of the strategy pulse. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
  • the light intensity control means controls the light source so as to change the light intensity of the emitted light according to data recorded on the information recording medium. Control.
  • the light source emits the emitted light having a light intensity that changes in a substantially sinusoidal shape according to the recorded data.
  • the light intensity control means changes the light intensity of the emitted light according to a strategy pulse corresponding to data recorded on the information recording medium.
  • the light source is controlled.
  • the emitted light having the light intensity that changes in a substantially sinusoidal shape in accordance with the strategy pulse is irradiated with the light source power.
  • the emitted light is usually emitted with a light intensity that changes to a square wave shape according to the strategy pulse.
  • the light intensity changes to a substantially sine wave shape according to the strategy pulse.
  • Outgoing light is emitted from the light source.
  • the strategy pulse is smaller than the first pulse having a predetermined first amplitude and the first amplitude.
  • At least a second pulse having a second amplitude, and the light intensity control means has a light intensity of the emitted light according to the first pulse, and the light intensity of the emitted light according to the second pulse.
  • You may comprise so that the said light source may be controlled so that it may become larger than intensity
  • the phase of the rise in the increase or decrease in the light intensity of the emitted light that is, the period during which the light intensity increases
  • the rise in the change in the transmission amount of the filter that is, the transmission of the filter. It is possible to synchronize with the phase of the period during which the amount increases.
  • the phase of the fall that is, the period during which the light intensity decreases
  • the transmission quantity of the filter decreases
  • Phase can be synchronized. It is possible to reduce or eliminate the situation where unnecessary blocking or unnecessary transmission of emitted light in the filter occurs.
  • the optical pickup device further includes a monitoring unit that monitors the light intensity of the emitted light that has passed through the filter, and the synchronization unit integrates the monitored light intensity.
  • the phase may be synchronized by comparing the value with a predetermined reference value.
  • the synchronization unit is V (t + At) — It may be configured to synchronize the phase so that V (t) takes 0 or the maximum value! /.
  • the outgoing light after passing through the filter changes to a square wave shape
  • the outgoing light after passing through the filter has its pulse in the ON state or its pulse in the OFF state.
  • the operation of comparing the integrated value of the monitored light intensity with the reference value is the monitoring This is equivalent to the operation for determining whether the integrated value of the light intensity is 0 or a maximum value.
  • the filter includes a light absorption layer whose absorption wavelength varies depending on a value of an applied voltage, and an electrode that applies the voltage to the light absorption layer.
  • the filter control means controls the filter so as to change a transmission amount of the filter by changing a value of the voltage applied to the electrode.
  • the transmission amount of the filter can be increased or decreased by changing the voltage applied to the light absorption layer.
  • the filter applies a liquid crystal layer including a liquid crystal element whose molecular arrangement changes depending on a value of an applied voltage, and the voltage to the liquid crystal layer.
  • the filter control means controls the filter so as to change the transmission amount of the filter by changing the value of the voltage applied to the electrode.
  • the transmission amount of the filter can be increased or decreased by changing the voltage applied to the liquid crystal layer.
  • the filter is disposed with a predetermined angle with respect to the optical path of the emitted light.
  • An irradiation method of the present invention comprises an optical pickup comprising: a light source that irradiates a recording surface of an information recording medium with emitted light; and a filter that is disposed on an optical path of the emitted light and changes a transmission amount of the incident emitted light.
  • a method of irradiating the emitted light in an apparatus wherein a light intensity control step of controlling the light source so as to change a light intensity of the emitted light into a substantially sinusoidal shape, and changing a transmission amount of the emitted light.
  • a filter control step for controlling the filter for controlling the filter.
  • the irradiation method can also take various forms.
  • An information recording apparatus of the present invention includes a light source that irradiates a recording surface of an information recording medium with emitted light, and a light intensity control unit that controls the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape.
  • a filter that is disposed on the optical path of the emitted light and that changes a transmission amount of the incident outgoing light, a filter control unit that controls the filter to change the transmission amount of the outgoing light, and the information Recording means for recording data on a recording medium. That is, an information recording apparatus of the present invention includes the above-described optical pickup apparatus of the present invention (including various aspects thereof) and recording means for recording data on the information recording medium.
  • the information recording apparatus of the present invention it is possible to record data on the information recording medium while enjoying the same benefits as the benefits of the above-described optical pickup device of the present invention.
  • the information recording apparatus of the present invention can also adopt various aspects.
  • An information reproducing apparatus of the present invention includes a light source that irradiates a recording surface of an information recording medium with emitted light, and a light intensity control unit that controls the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape.
  • a filter that is disposed on the optical path of the emitted light and that changes a transmission amount of the incident outgoing light, a filter control unit that controls the filter to change the transmission amount of the outgoing light, and the information Playback means for playing back data recorded on the recording medium. That is, an information recording apparatus according to the present invention includes the above-described optical pickup apparatus according to the present invention (including various aspects thereof) and reproducing means for reproducing data recorded on the information recording medium.
  • the information reproducing apparatus of the present invention can also adopt various aspects.
  • a first computer program of the present invention is a recording control computer program for controlling a computer provided with the above-described information recording apparatus of the present invention (including various aspects thereof), It functions as at least a part of the light intensity control means and the filter control means.
  • a second computer program of the present invention is a computer program for reproduction control for controlling a computer provided with the above-described information reproduction apparatus of the present invention (including various aspects thereof), A computer is caused to function as at least part of the light intensity control means and the filter control means.
  • each computer program if the computer program is read from a recording medium such as a ROM, CD-ROM, DVD-ROM, or hard disk storing the computer program and then executed by the computer.
  • a recording medium such as a ROM, CD-ROM, DVD-ROM, or hard disk storing the computer program and then executed by the computer.
  • the computer program is downloaded to a computer via communication means and then executed, the above-described information recording apparatus or information reproducing apparatus of the present invention can be realized relatively easily.
  • each computer program of the present invention can also adopt various aspects.
  • a first computer program product in a computer-readable medium is obtained by a computer provided with the above-described information recording apparatus (including various aspects thereof) of the present invention.
  • Executable program instructions are clearly embodied, and the converter functions as at least a part of the light intensity control means and the filter control means.
  • a second computer program product in a computer-readable medium is obtained by a computer provided with the above-described information reproducing apparatus of the present invention (including various aspects thereof).
  • Executable program instructions are clearly embodied, and the converter functions as at least a part of the light intensity control means and the filter control means.
  • a record such as a ROM, a CD-ROM, a DVD-ROM, or a hard disk for storing the computer program product.
  • the computer program product is read from a medium into a computer, or if the computer program product, which is a transmission wave, for example, is downloaded to a computer via communication means, the information recording apparatus or information reproducing apparatus of the present invention described above Can be implemented relatively easily.
  • the computer program product may also be configured with computer-readable code (or computer-readable instructions) that functions as the information recording apparatus or information reproducing apparatus of the present invention described above.
  • the optical pickup device of the present invention includes a light source, a light intensity control means, a filter, and a filter control means. Therefore, a suitable recording operation and reproduction operation can be performed while suppressing heat dissipation.
  • the irradiation method of the present invention includes a light intensity control step and a filter control step. Therefore, it is possible to perform a suitable recording operation and reproducing operation while suppressing heat dissipation.
  • the information recording apparatus of the present invention includes a light source, a light intensity control means, a filter, a filter control means, and a recording means. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
  • the light source, the light intensity control means, the filter, the filter control means, and the reproduction means are provided. Therefore, a suitable reproduction operation can be performed while suppressing heat dissipation.
  • FIG. 1 is a block diagram conceptually showing the basic structure of an information recording / reproducing apparatus in a first example.
  • FIG. 2 is a sectional view conceptually showing a first specific example of the filter.
  • FIG. 3 is a sectional view conceptually showing a second specific example of the filter.
  • FIG. 4 is a sectional view conceptually showing a third specific example of the filter.
  • FIG. 5 Waveform of recording strategy according to recording signal (recording data), light intensity of light beam emitted from laser diode, transmission amount of filter, and light intensity of light beam irradiated to optical disk, respectively It is a graph which shows notably the mode of the change along a time-axis.
  • FIG. 6 is a waveform diagram showing overshoot and undershoot of a light beam.
  • FIG. 7 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the second example.
  • FIG. 8 When the timing of changing the transmission amount of the filter is not shifted, the light intensity of the light beam emitted from the laser diode, the transmission amount of the filter, and the light intensity of the light beam emitted to the optical disc are It is a graph which shows notionally the mode of change along a time axis.
  • FIG. 9 The light intensity of the light beam emitted from the laser diode, the transmission quantity of the filter, and the light intensity of the light beam emitted to the optical disk when the timing of changing the transmission quantity of the filter is shifted. , Is a graph conceptually showing the state of change along the time axis
  • FIG. 1 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the first example.
  • the information recording / reproducing apparatus 1 includes an optical pickup 10, a photo detector (PD) amplifier 21, a reproducing circuit 22, a CPU 24, and a recording A circuit 25, a laser drive circuit 26, a filter element drive circuit 27, and a spindle motor 28 are provided.
  • PD photo detector
  • the optical pickup 10 is used to irradiate the optical disc 50 with a light beam and to record and reproduce data on the optical disc 50.
  • the optical pickup 10 includes a laser diode 11, a filter 13, a beam splitter 14, an objective lens 15, a condenser lens 16, and a photodetector 17.
  • the laser diode 11 constitutes a specific example of the “light source” in the present invention. Based on the drive signal supplied from the laser drive circuit 26, the laser diode 11 emits one type or plural types of light beams having different wavelengths. Irradiate. For example, when data is recorded and reproduced on a DVD constituting a specific example of the optical disk 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 660 nm. For example, when data is recorded and reproduced on a CD constituting a specific example of the optical disc 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 780 nm. For example, when recording and reproducing data on a Blu-ray Disc constituting a specific example of the optical disc 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 405 nm.
  • the filter 13 has a configuration capable of changing the transmission amount of the light beam incident on the filter 13 (that is, the transmittance for the light beam incident on the filter 13) under the control of the filter element drive circuit 27. is doing.
  • the specific configuration of the filter 13 will be described in detail later (see FIGS. 2 to 4).
  • the beam splitter 14 reflects 90% of the light beam, which is also incident on the side force of the laser diode 11, to the optical disk 50 and transmits 10%, and is incident from the optical disk 50 side.
  • the light beam (that is, the light reflected from the optical disk 50) is transmitted 100% as it is.
  • the objective lens 15 emits an incident light beam and irradiates the recording surface of the optical disc 50.
  • the condensing lens 16 condenses the light beam transmitted through the beam splitter 14 as it is (that is, the light beam reflected from the optical disk 50) and irradiates the light receiving surface of the photodetector 17 with the light beam. .
  • the photodetector 17 is configured by, for example, a photodiode, receives the light beam emitted from the condenser lens 16, and sends a detection signal corresponding to the power of the received light beam to the photodetector amplifier 21. Output.
  • the photodetector amplifier 21 generates an RF signal from the detection signal output from the photodetector 17 and outputs the RF signal to the reproduction circuit 22.
  • the reproduction circuit 22 constitutes one specific example of the "reproduction means" in the present invention.
  • the RF signal output from the photodetector amplifier 21 is demodulated, decoded, or error-corrected. Or a decoding process or the like to generate a reproduction signal.
  • the reproduction circuit 22 outputs the generated reproduction signal to an external display, a speaker or the like, and as a result, it is reproduced as data power recorded on the optical disc 50, for example, video content, audio content, or other content.
  • the CPU 24 is connected to each component of the information recording / reproducing apparatus 1 via a bus, and controls the entire information recording / reproducing apparatus 1 by giving an instruction to each component.
  • software or firmware for the CPU 24 to operate is stored in a memory in the information recording / reproducing apparatus 1.
  • the recording circuit 25 constitutes one specific example of “recording means” in the present invention, and corrects errors with respect to recording data input from the outside as data for recording on the optical disk 50.
  • a recording signal is generated by performing code addition processing, modulation processing, encryption processing, encoding processing, and the like.
  • the generated recording signal is output to the laser drive circuit 26.
  • the laser drive circuit 26 constitutes a specific example of the “light intensity control means” of the present invention under the control of the CPU 24, and a drive signal for controlling the operation of the laser diode 11 is transmitted to the laser diode. Output to 11.
  • the laser drive circuit 26 uses a predetermined power as a write light or a power (hereinafter referred to as a power value output from the CPU 24). And a recording signal that is irradiated with a light beam while being modulated in accordance with the recording signal output from the recording circuit 25, and outputs it to the laser diode 11.
  • the laser drive circuit 26 uses a predetermined power as reading light or a power corresponding to a power value output from the CPU 24 (hereinafter referred to as “reproduction power”). T)) Generate a drive signal that is irradiated with the light beam and output it to the laser diode 11.
  • the filter element drive circuit 27 constitutes a specific example of the “filter control means” of the present invention under the control of the CPU 24, and controls the change in the transmission amount of the light beam incident on the filter 13. It is configured to be possible.
  • the spindle motor 28 rotates and stops the optical disc 50, and operates when accessing the optical disc 50. More specifically, the spindle motor 28 is configured to rotate and stop the optical disc 50 at a predetermined speed while receiving spindle servo from a servo unit (not shown) or the like.
  • the light beam emitted from the laser diode 11 is incident on the filter 13.
  • the light beam irradiated from the laser diode 11 is controlled by the filter 13 and then reflected by the beam splitter 14, enters the objective lens 15, and is condensed on the optical disk 50.
  • the light beam is collected on the optical disk 50 in this way, the light beam is reflected by the optical disk 50 and then enters the beam splitter 14 again through the objective lens 15, so that the beam splitter 14 Transparent. Thereafter, the light enters the condensing lens 16 and is condensed on the photodetector 17 by the condensing lens 16 mm.
  • a light reception signal is output from the photodetector 17 to the photodetector amplifier 21, and an RF signal is output from the photodetector amplifier 21 to the reproduction circuit 22.
  • the CPU 24 controls the reproduction circuit 22 to reproduce the data corresponding to the RF signal when reproducing the data recorded on the optical disc 50,
  • the reproduction circuit 22 outputs the data to the outside.
  • the CPU 24 determines the output timing of the drive signal corresponding to the address acquisition and data to be recorded on the optical disc 50 based on this RF signal, for example.
  • FIG. 2 is a sectional view conceptually showing a first specific example of the filter 13
  • FIG. 3 is a sectional view conceptually showing a second specific example of the filter 13
  • FIG. FIG. 5 is a sectional view conceptually showing a third specific example of the filter 13.
  • the filter 13 can be configured using a material called an EC (Electrochromic) material, for example.
  • This EC material is a material that causes the electochromism phenomenon in which the absorption wavelength reversibly changes depending on the applied voltage. Transparent state force is absorbed by the applied voltage, and changes to a state in which each color is exhibited by absorbing only light of a predetermined frequency. It has the characteristics to There are two types of EC materials, inorganic and organic. Examples of inorganic EC materials include W03 (tungsten trioxide) and MoO 3 (molybdenum trioxide) using electroabsorption reaction.
  • Power Sword EC colored by reduction
  • Prussian blue KxFeyFez (CN) 6
  • Nianod EC colored by acid
  • organic EL materials are organic EL
  • functional polymers such as polyphenacillin that are used as (Electro Luminescent) materials.
  • the first specific example of the filter 13 (hereinafter referred to as "filter 13a") is made of a highly permeable base material such as Si02 (acid-silicon).
  • a substrate 101 is provided.
  • a transparent electrode 102 is formed on the substrate 101, and an EC layer 103 is formed on the transparent electrode 102 by film formation by a sol-gel method, a pulling method, vapor deposition, or the like, followed by baking.
  • a transparent electrode 104 is further laminated on the EC layer 103. As a result, the EC layer 103 is sandwiched between the transparent electrode 102 and the transparent electrode 104.
  • the transparent electrode 102 and the transparent illumination 104 are respectively connected to the filter element drive circuit.
  • the filter element drive circuit 27 is connected to a power source provided in the path 27, and the filter element drive circuit 27 applies a predetermined voltage between the transparent electrode 102 and the transparent electrode 104 to thereby absorb light in the EC layer 103. (For example, the absorption wavelength) is reversibly changed. That is, the transmission amount of the light beam incident on the filter 13a is reversibly changed.
  • the filter 13a Since the absorbance in the EC material varies depending on the material to be used, when specifically designing the filter 13a, the filter 13a allows the light beam irradiated from the laser diode 11 to pass through the filter 13a. It is preferable to determine the thickness of the EC layer 103, the EC material used for the EC layer 103, the magnitude of the voltage applied to the EC layer 103, etc., depending on how much it is reduced.
  • a second specific example of the filter 13 (hereinafter referred to as “filter 13b”) includes two transparent substrates 111 and 114. And an EC layer 113 composed of an organic EC material member is filled between the transparent substrate 111 and the transparent substrate 114. On the opposing surfaces of the transparent substrate 111 and the transparent substrate 114, a transparent electrode 112 and a transparent electrode 115 are formed. Each of the transparent electrode 112 and the transparent electrode 115 is connected to a power source provided in the filter element drive circuit 27, and the filter element drive circuit 27 is provided between the transparent electrode 112 and the transparent electrode 115.
  • the light absorption characteristics in the EC layer 113 are reversibly changed. That is, the transmission amount of the light beam incident on the filter 13b is reversibly changed.
  • the filter 13 can also be configured using a liquid crystal material such as a cholestic liquid crystal.
  • the transmittance of the cholestic liquid crystal can be changed according to the applied voltage and temperature.
  • a liquid crystal material such as a cholestic liquid crystal.
  • the transmittance of the cholestic liquid crystal can be changed according to the applied voltage and temperature.
  • FIG. 4 in the third specific example of the filter 13 (hereinafter referred to as “filter 13c”), two transparent substrates 121 and 124 are bonded together with a gap between them.
  • a liquid crystal layer 123 composed of a liquid crystal material is filled between the transparent substrate 121 and the transparent substrate 124.
  • a transparent electrode 122 and a transparent electrode 125 are formed on the opposing surfaces of the transparent substrate 121 and the transparent substrate 124, respectively. Has been.
  • Each of the transparent electrode 122 and the transparent electrode 125 is connected to a power source provided in the filter element drive circuit 27, and the filter element drive circuit 27 is provided between the transparent electrode 122 and the transparent electrode 125.
  • the liquid crystal layer 123 is constituted, and the alignment characteristics of the liquid crystal molecules contained in the liquid crystal material are reversibly changed. That is, the transmission amount of the light beam incident on the filter 13c is reversibly changed. Even in this case, it is necessary to appropriately design the thickness, applied voltage value, etc. of the liquid crystal layer 123 because the EC layer 103 also includes the above-described inorganic EC material force and the EC layer 113 that also includes the organic EC material force. It is the same.
  • inorganic EC material organic EC material
  • liquid crystal material such as stick liquid crystal, a photopolymer, a photorefractive liquid crystal, an isomerized material, or a fluorescent dye is used.
  • the filter 13 described above can also be configured.
  • the filter 13 described above is preferably made of a material that can change the amount of transmission in the order of picoseconds or in the order of femtoseconds. In other words, it is possible to switch from a low transmission level to a high !, state, or a high transmission level !, from a low state to a state, on the order of picoseconds or femtoseconds. It is preferable to configure the filter 13 using a material. However, the filter 13 may be configured using a material capable of switching from a low transmission amount to a high state or from a high transmission amount to a low state on the order of nanoseconds. ,.
  • FIG. 5 shows the waveform of the recording strategy according to the recording signal (recording data), the light intensity of the light beam emitted from the laser diode 11, the transmission amount of the filter 13, and the light beam emitted to the optical disc 50.
  • FIG. 6 is a graph conceptually showing how the light intensity changes along the time axis, and FIG. 6 is a waveform diagram conceptually showing the overshoot and undershoot of the light beam.
  • the light beam whose light intensity changes with the waveform shown in FIG. Assuming that data is required to be recorded on the optical disc 50 Proceed with the explanation.
  • the light beam can be irradiated with a light intensity that changes with the waveform shown in Fig. 5 (a), and the light beam is applied according to a strategy pulse having a waveform substantially similar to the waveform shown in Fig. 5 (a).
  • the explanation will be made assuming that it is necessary to irradiate.
  • the laser drive circuit 26 drives the laser diode 11 so as to irradiate an optical beam that changes with the light intensity shown in FIG. 5 (b). More specifically, the laser drive circuit 26 has the exact square wave shape shown in FIG. 5 (a) while the timing or phase of the rise and fall of the waveform shown in FIG. The laser diode 11 is driven so that the light intensity of the light beam changes in such a manner that it rises more slowly than the waveform and falls more slowly. More specifically, the laser drive circuit 26 drives the laser diode 11 so that the light intensity changes in a substantially sinusoidal waveform shown in FIG. During a period in which the amplitude of the waveform shown in FIG.
  • the laser drive circuit 26 drives the laser diode 11 so that the light intensity of the light beam becomes relatively large.
  • the laser drive circuit 26 drives the laser diode 11 so that the light intensity of the light beam becomes relatively small.
  • the filter control circuit 27 causes the transmission amount to change with the same or substantially the same waveform as that shown in FIG. 5A.
  • a predetermined voltage is applied to the filter 13. More specifically, the filter control circuit 27 adjusts the voltage applied to the filter 13 so as to change with the waveform shown in FIG. 5 (a).
  • the transmission amount of the filter 13 is controlled. That is, during a period when the amplitude of the waveform shown in FIG. 5A is relatively large, the filter element drive circuit 27 applies a predetermined voltage to the filter 13 so that the transmission amount of the filter 13 is relatively large. To do. On the other hand, during a period in which the amplitude of the waveform shown in FIG. 5A is relatively small, the filter element drive circuit 27 applies a predetermined voltage to the filter 13 so that the transmission amount of the filter 13 is relatively small. .
  • the light beam irradiated from the laser diode 11 so that the light intensity changes in the waveform shown in FIG. 5 (b) passes through the filter 13 whose transmission amount changes in the waveform shown in FIG. 5 (c).
  • the optical intensity is changed with the waveform shown in FIG. Is done.
  • the laser drive circuit 26 needs to drive the laser diode 11 so as to change the light intensity in the form of a strict square wave shown in FIG. 5 (a). It ’s gone. More specifically, the laser diode is changed so as to change the light intensity in the shape of a square wave in which the light intensity suddenly or instantaneously increases tl and the light intensity sharply or instantaneously decreases. There is no need to drive. As a result, the laser diode 11 may be driven so as to change the light intensity in a substantially sinusoidal shape in which the light intensity increases relatively slowly and the light intensity decreases relatively slowly.
  • the laser drive circuit 26 does not need to drive the laser diode 11 so as to irradiate a square-wave light beam having a relatively short pulse width (that is, high-speed and suddenly ONZOFF).
  • the diode 11 can be driven suitably.
  • the amount of heat generated when the laser drive circuit 26 drives the laser diode 11 can be relatively reduced.
  • the optical disk 50 can be irradiated with the same light beam as when the laser diode 11 is driven so as to change the light intensity with a strict square wave. As a result, data can be suitably recorded on the optical disc 50.
  • the filter 13 By using the filter 13, it is possible to optically change the light intensity of the light beam, so compared with the case where the laser drive circuit 26 changes the light intensity of the light beam.
  • the waveform of the light beam can be controlled with higher accuracy.
  • the transmission amount is low, the state is high !, the state is switched, or the transmission amount is high !, the state is low, the state is switched on the order of picoseconds or is femtoseconds.
  • the optical disk 50 can be suitably irradiated with a light beam having a pulse width that is extremely short even if the recording speed increases in the future.
  • the pulse width of the optical beam becomes shorter and shorter.
  • the waveform of the optical beam can be controlled by using the filter 13, so that the burden of the laser drive circuit 26 is reduced. Does not increase so rapidly. Therefore, the amount of increase in the amount of heat generated by the laser drive circuit 26 can be suppressed as compared with the amount of decrease in the pulse width due to the increase in recording speed.
  • a filter that has a transmittance of "0" above a certain power or a transmittance of "0" above a certain power is used. It is preferable to remove shoots and undershoots.
  • an optical amplifier, a light control glass, or the like can be used.
  • the laser drive circuit 26 drives the laser diode 11 so as to irradiate a light beam whose light intensity changes to a substantially sinusoidal shape. Even if the laser diode 11 is driven so as to irradiate a light beam having a constant light intensity, the above-mentioned various benefits can be enjoyed accordingly. In other words, even if the laser diode 11 is driven so as to irradiate the light beam with a DC level light intensity, the above-described various benefits can be enjoyed accordingly.
  • a light beam reflected by the filter 13 can be generated in addition to the light beam transmitted or absorbed.
  • the filter 13 is installed at an angle with the incident axis of the light beam as a normal line, the light beam reflected on the filter 13 may stray on the optical axis. Therefore, it is preferable to install the filter 13 at a predetermined angle ⁇ with respect to the incident axis of the light beam so that no reflected light is generated on the optical axis in the filter 13! /.
  • FIG. 7 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the second example.
  • FIG. 8 is a diagram in the case where the timing for changing the transmission amount of the filter 13 is not shifted.
  • a graph conceptually showing how the light intensity of the light beam emitted from the laser diode 11, the transmission amount of the filter 13, and the light intensity of the light beam emitted to the optical disc 50 change along the time axis.
  • the information recording / reproducing apparatus 2 includes an optical pickup 10a, a photo detector (PD) amplifier 21, a reproducing circuit 22, a CPU 24, and a recording device.
  • a circuit 25 a laser drive circuit 26, a filter element drive circuit 27, a spindle motor 28, an integration circuit 31, a reference value storage circuit 32, a comparator 33, and a phase compensation servo circuit 34 are provided.
  • the optical pickup 10a includes a laser diode 11, a front monitor (FM) 12, a filter 13, a beam splitter 14, and an objective lens 15.
  • the condenser lens 16 and the photo detector 17 are provided.
  • the front monitor 12 constitutes a specific example of the “monitoring means” of the present invention.
  • the front monitor 12 includes a light receiving sensor and the like, and the power of the light beam emitted from the laser diode 11 (ie, light This is the light intensity value or energy amount of the beam. The value according to the amount of received light) can be measured. The measured power is output to the integrating circuit 31.
  • the integrating circuit 31 is configured to be able to integrate the power of the light beam measured by the front monitor 12.
  • the power of the light beam integrated in the integration circuit 31 indicates a DC component of the light intensity of the light beam and is output to the comparator 33.
  • the reference value storage circuit 32 is configured to be able to output to the comparator 33 a reference value that is referred to when compared with the power of the light beam integrated in the integrating circuit.
  • a reference value “0” or “Vmax” indicating the maximum value of the light intensity of the light beam is stored, and these reference values are output to the comparator 33.
  • the comparator 33 compares the integrated value of the power of the light beam output from the integration circuit 31 with the reference value output from the reference value storage circuit 32, and the comparison result is input to the phase compensation servo circuit 34. Output.
  • the phase compensation servo circuit 34 adjusts the timing (or phase) for changing the transmission amount of the filter 13 based on the comparison result in the comparator 33. More specifically, if the V (t + A t) -V (t) force matches the reference value “0” or “Vmax”, the timing for changing the transmission amount of the filter 13 is not changed. On the other hand, if V (t + At) -V (t) does not match the reference value "0” or “Vmax”, V (t + At) — V (t) force reference value " The timing for changing the transmission amount of the filter 13 is changed so as to coincide with “0” or “Vmax”. The change in the timing of changing the amount of transmission of the filter 13 depends on how much difference there is between the V (t + At) -V (t) force reference value "0" or “Vmax”. And are preferred.
  • the rising and falling phases (or the tendency of increase / decrease or the optical beam in the change of the light intensity of the light beam).
  • ONZOFF timing) and the rising and falling phases of the change in the transmission amount of the filter 13 (or the tendency of increase / decrease or the ON / OFF timing of the change in the transmission amount of the filter 13). ! / Thanks can be matched.
  • the rise and fall of the change in the light intensity of the light beam is suppressed. There may be a case where the phase and the rising and falling phases in the change in the transmission amount of the filter 13 are shifted. In this case, the light intensity of the light beam actually irradiated onto the optical disc 50 changes with an inappropriate waveform lacking a part of the square wave as shown in FIG. 8 (b).
  • the second embodiment by changing the timing of changing the transmission amount of the filter 13, as shown in Fig. 9 (a), the rise and rise in the change in the light intensity of the light beam.
  • the falling phase and the phase of the rising and falling force S in the change in the transmission amount of the filter 13 can be aligned or matched.
  • the light intensity of the light beam actually irradiated onto the optical disc 50 changes in an appropriate square wave shape as shown in FIG. 9 (b).
  • the reliability of data recording on the optical disc 50 can be relatively improved in consideration of the above-described various benefits.
  • the CPU 24, the laser drive circuit 26, the filter element drive circuit 27, the integration circuit 31, the reference value storage circuit 32, the comparator 33, and the phase compensation servo may be configured so as to be integrated with the optical pickup 10 and further included in the laser diode 11. Needless to say.
  • the optical disc 50 and the recorder or player related to the optical disc 50 as an example of the information recording device or the information reproducing device have been described as an example of the information recording medium.
  • the present invention is not limited to a player, and can be applied to other high-density recording or various information recording media compatible with a high transfer rate, as well as the recorder or player.
  • the present invention is not limited to the embodiments described above, but the entire claims and specification.
  • the optical pickup device, the irradiation method, the information recording device, the information reproducing device, and the computer program that can be changed as appropriate without departing from the gist or idea of the invention that can be read. It is included in the scope.
  • the optical pickup device, the irradiation method, the information recording device and the information reproducing device, and the computer program according to the present invention can be used for an optical pickup device used for recording and reproducing data on an information recording medium such as an optical disk.
  • the present invention can be used for an information recording device and an information reproducing device including an optical pickup device. Further, the present invention can also be used for information recording devices and information reproducing devices that are mounted on or connectable to various computer devices for consumer use or business use.

Abstract

An optical pickup device (10) comprising a light source (11) for irradiating the recording surface of an information recording medium (100) with an output light, a light intensity controlling means (26) for controlling the light source so as to change the light intensity of the output light into an almost sinusoidal form, a filter (13) disposed on the light path of the output light to change the transmission amount of an incident output light, and a filter controlling means (27) for controlling the filter so as to change the transmission amount of the output light.

Description

明 細 書  Specification
光ピックアップ装置、照射方法、情報記録装置及び情報再生装置、並び にコンピュータプログラム  Optical pickup device, irradiation method, information recording device, information reproducing device, and computer program
技術分野  Technical field
[0001] 本発明は、光ディスク等の情報記録媒体に対するデータの記録及び再生に用いる 光ピックアップ装置、光ピックアップ装置における出射光の照射方法、該光ピックアツ プ装置を備える情報記録装置及び情報再生装置、並びにコンピュータをこのような 情報記録装置又は情報再生装置として動作させるコンピュータプログラムに関する。 背景技術  [0001] The present invention relates to an optical pickup device used for recording and reproducing data on an information recording medium such as an optical disc, a method of irradiating emitted light in the optical pickup device, an information recording device and an information reproducing device including the optical pickup device, The present invention also relates to a computer program that causes a computer to operate as such an information recording device or information reproducing device. Background art
[0002] 従来から CD (Compact Disc)や DVD (Digital Versatile Disc)等の光ディスクに対 するデータの記録及び再生を行う情報記録再生装置にお 、ては、ユーザの利便性 を向上させ、或いは、他製品との差別ィ匕を図る観点から DVD—R等の光ディスクに 対するデータの記録スピードの向上が図られている。  [0002] Conventionally, in an information recording / reproducing apparatus for recording and reproducing data on an optical disc such as a CD (Compact Disc) or a DVD (Digital Versatile Disc), the convenience of the user is improved, or From the standpoint of discriminating from other products, the recording speed of data on optical discs such as DVD-R has been improved.
[0003] ここで、 DVD— R或いは DVD— RW等の光ディスクは、或る単位時間あたりに照射 されるレーザ光のエネルギー総量が所定の閾値を越えた場合、或いは、光ディスク 上における温度が一定の値以上になった場合に色素の熱分解或いは相変化を生じ 、これにより各種データが記録される構成となっている。このため、記録スピードを向 上させるべく光ディスクの回転速度を上昇させると光ディスクに照射されるレーザ光の エネルギー量 (即ち、レーザ光のパワー)を増加させなければデータを記録させること ができなくなる。従って、記録スピードの向上を実現するためには、光源から出力され るレーザ光のパワーを増加させることが不可欠となる。  [0003] Here, an optical disc such as DVD-R or DVD-RW has a constant temperature on the optical disc when the total amount of laser light irradiated per unit time exceeds a predetermined threshold. When the value exceeds the value, thermal decomposition or phase change of the dye occurs, whereby various data are recorded. For this reason, if the rotational speed of the optical disk is increased in order to increase the recording speed, data cannot be recorded unless the amount of laser beam energy (ie, laser beam power) applied to the optical disk is increased. Therefore, in order to improve the recording speed, it is essential to increase the power of the laser beam output from the light source.
発明の開示  Disclosure of the invention
発明が解決しょうとする課題  Problems to be solved by the invention
[0004] し力しながら、光源から出力されるレーザ光のパワーを増加させるためには、レーザ 光を出力するレーザ素子を駆動するためのレーザドライブ回路の駆動電流を大幅に 増加させる必要がある。例えば、光ディスクの一具体例である DVDであれば、例えば 300mW程度のパワーでレーザ光を出力するために、例えば 800mA程度の駆動電 流をレーザドライブ回路力 レーザ素子に供給する必要がある。更なる記録スピード の向上を実現するためには、例えば 300mWよりも大きなパワーでレーザ光を出力す ることも必要とされ、例えば 800mA以上の大きな駆動電流をレーザドライブ回路から レーザ素子に供給する必要も出てくる。 However, in order to increase the power of the laser beam output from the light source, it is necessary to significantly increase the drive current of the laser drive circuit for driving the laser element that outputs the laser beam. . For example, in the case of a DVD which is a specific example of an optical disk, for example, a drive power of about 800 mA is used to output laser light with a power of about 300 mW. It is necessary to supply the current to the laser drive circuit force laser element. In order to further improve the recording speed, it is necessary to output laser light with a power greater than 300 mW, for example, and it is necessary to supply a large drive current of 800 mA or more to the laser element from the laser drive circuit, for example. Also come out.
[0005] 更に、記録スピードの増加に伴って、レーザ光のパルス幅も減少しており、例えば D[0005] Further, as the recording speed increases, the pulse width of the laser beam also decreases, for example, D
VDの 16倍速記録であれば、概ね Insから 30nsのオーダーのパルス幅を有する厳 密な方形波形状のレーザ光を出力する必要がある。 For VD 16x speed recording, it is necessary to output a strict square wave laser beam with a pulse width on the order of Ins to 30 ns.
[0006] し力しながら、例えば 800mAを超えるような大きな駆動電流を用いて概ね Ins程度 の短 、パルス幅を有する厳密な方形波形状のレーザ光を出力することは、現在のレ 一ザドライブ回路の動作としては困難であると 、う技術的な問題点を有して 、る。更 には、例えば 800mAを超えるような大きな駆動電流を用いて概ね Ins程度の短いパ ルス幅を有する厳密な方形波形状のレーザ光を出力する場合には、レーザドライブ 回路の発熱量も大幅に増カロしてしまうという技術的な問題点を有している。 [0006] However, it is possible to output a laser beam with a strict square wave shape having a short pulse width of about Ins by using a large drive current exceeding 800 mA, for example. If the operation of the circuit is difficult, it has technical problems. Furthermore, when a laser beam with a strict square wave shape with a short pulse width of approximately Ins is output using a large drive current exceeding 800 mA, for example, the amount of heat generated by the laser drive circuit is also greatly increased. It has the technical problem of increasing the amount of calories.
[0007] 本発明は、例えば上述した従来の問題点に鑑みなされたものであり、例えば放熱を 抑制しながら好適な記録動作等を行うことを可能とならしめる光ピックアップ装置、出 射光の照射方法、情報記録装置及び情報再生装置、並びにコンピュータプログラム を提供することを課題とする。 The present invention has been made in view of the above-described conventional problems, for example, an optical pickup device capable of performing a suitable recording operation while suppressing heat dissipation, and a method for irradiating emitted light. It is an object of the present invention to provide an information recording device, an information reproducing device, and a computer program.
課題を解決するための手段  Means for solving the problem
[0008] (光ピックアップ装置)  [0008] (Optical pickup device)
本発明の光ピックアップ装置は、情報記録媒体の記録面に出射光を照射する光源 と、前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光 強度制御手段と、前記出射光の光路上に配置され、入射される前記出射光の透過 量を変更するフィルタと、前記出射光の透過量を変更するように前記フィルタを制御 するフィルタ制御手段とを備える。  The optical pickup device of the present invention includes a light source for irradiating the recording surface of the information recording medium with the emitted light, a light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape, A filter disposed on the optical path of the outgoing light and configured to change a transmission amount of the incident outgoing light; and a filter control unit configured to control the filter so as to change the transmission amount of the outgoing light.
[0009] 本発明の光ピックアップ装置によれば、レーザ素子等を含む光源から出射される出 射光が情報記録媒体の記録面に照射される。出射光は、レーザドライブ回路等を含 む光強度制御手段の動作により、その光強度が制御される。例えば、情報記録媒体 にデータを記録する際には、情報記録媒体の記録面に記録マークな 、しは記録ピッ トを形成できる相対的に強い (或いは、相対的に大きい)第 1の光強度で、光源から 出射光が出射される。或いは、例えば情報記録媒体に記録されているデータを再生 する際には、情報記録媒体の記録面に形成されて 、る記録マークな 、しは記録ピッ トを破壊な 、しは消去しな 、程度の相対的に弱 、(或いは、相対的に小さ 、)第 2の 光強度で、光源から出射光が出射される。 According to the optical pickup device of the present invention, the emitted light emitted from the light source including the laser element or the like is irradiated onto the recording surface of the information recording medium. The intensity of the emitted light is controlled by the operation of light intensity control means including a laser drive circuit. For example, when recording data on an information recording medium, there is no recording mark or recording pitch on the recording surface of the information recording medium. The emitted light is emitted from the light source with the first light intensity that is relatively strong (or relatively large) capable of forming a light source. Or, for example, when reproducing data recorded on an information recording medium, the recording mark formed on the recording surface of the information recording medium, or the recording pit is not destroyed or erased. The emitted light is emitted from the light source at a second light intensity that is relatively weak (or relatively small).
[0010] 本発明では特に、光強度制御手段の動作により、出射光の光強度が略正弦波形 状に変化するように、出射光の光強度が制御される。ここに「略正弦波形状に変化さ せる」とは、厳密な方形波の形状で光強度を変化させる場合と比較して、光強度が緩 やかに変化させる状態を示す趣旨である。即ち、光強度制御手段の動作により、光 強度を相対的に緩やかに増加させ且つ相対的に緩やかに減少させる状態を示す趣 旨である。 In the present invention, in particular, the light intensity of the emitted light is controlled by the operation of the light intensity control means so that the light intensity of the emitted light changes in a substantially sinusoidal waveform. Here, “change to a substantially sine wave shape” is intended to indicate a state in which the light intensity changes more slowly than when the light intensity is changed in a strict square wave shape. That is, it is intended to indicate a state in which the light intensity is increased relatively slowly and decreased relatively slowly by the operation of the light intensity control means.
[0011] そして、光源から出射された出射光は、フィルタに入射した後に、情報記録媒体の 記録面に照射される。フィルタは、当該フィルタに入射する出射光の透過量を増減さ せることができる。どれだけの出射光を透過させるかは、フィルタ制御手段の動作によ り制御される。即ち、フィルタの透過量は、フィルタ制御手段の動作により制御される 。本発明では、フィルタ制御手段は、フィルタの透過量が略方形波状に変化するよう に、フィルタの透過量を変更する。  [0011] Then, the emitted light emitted from the light source is incident on the recording surface of the information recording medium after entering the filter. The filter can increase or decrease the transmission amount of the outgoing light incident on the filter. How much outgoing light is transmitted is controlled by the operation of the filter control means. That is, the transmission amount of the filter is controlled by the operation of the filter control means. In the present invention, the filter control means changes the transmission amount of the filter so that the transmission amount of the filter changes in a substantially square wave shape.
[0012] まとめると、本発明に係る光ピックアップ装置によれば、略正弦波形状に変化する 光強度で出射された出射光が、フィルタを透過することによって、方形波形状に変化 する光強度で情報記録媒体の記録面に照射される。言い換えれば、光源から出射 光を照射する時点で出射光の光強度を厳密な方形波形状に変化させる必要はない 。このため、光強度変化手段は、発熱量を抑えつつ出射光の光強度を変化させるこ とができる。そして、略正弦波形状の変化する光強度で出射光が光源力 出射され たとしても、フィルタ及びフィルタ制御手段の動作により、出射光は、方形波形状に変 化する光強度で情報記録媒体の記録面に照射される。このため、情報記録媒体の 記録面に好適な記録マークないしは記録ピットを形成することができ、その結果、好 適にデータを記録することができる。  In summary, according to the optical pickup device of the present invention, the emitted light emitted with the light intensity changing to a substantially sinusoidal shape passes through the filter, and the light intensity changing to the square wave shape is obtained. The recording surface of the information recording medium is irradiated. In other words, it is not necessary to change the light intensity of the emitted light into a strict square wave shape when the emitted light is irradiated from the light source. For this reason, the light intensity changing means can change the light intensity of the emitted light while suppressing the amount of heat generation. Even if the emitted light is emitted from the light source with a light intensity that changes in a substantially sinusoidal shape, the operation of the filter and the filter control means causes the emitted light to have a light intensity that changes to a square wave shape. Irradiates the recording surface. For this reason, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be suitably recorded.
[0013] 以上の結果、本発明の光ピックアップ装置によれば、放熱を抑制しながら、好適な 記録動作を行うことができる。 As a result of the above, according to the optical pickup device of the present invention, it is preferable to suppress heat dissipation and A recording operation can be performed.
[0014] 本発明の光ピックアップ装置の一の態様は、前記フィルタ制御手段は、前記情報記 録媒体に記録されるデータに応じて前記フィルタの透過量を変更するように前記フィ ルタを制御する。  In one aspect of the optical pickup device of the present invention, the filter control unit controls the filter so as to change a transmission amount of the filter according to data recorded on the information recording medium. .
[0015] この態様によれば、記録されるデータに応じて、出射光は、方形波形状に変化する 光強度で情報記録媒体の記録面に照射される。このため、情報記録媒体の記録面 に好適な記録マークないしは記録ピットを形成することができ、その結果、好適にデ ータを記録することができる。従って、放熱を抑制しながら、好適な記録動作を行うこ とがでさる。  [0015] According to this aspect, the emitted light is irradiated onto the recording surface of the information recording medium with the light intensity that changes to a square wave shape according to the data to be recorded. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, it is possible to perform a suitable recording operation while suppressing heat dissipation.
[0016] 本発明の光ピックアップ装置の他の態様は、前記フィルタ制御手段は、前記情報記 録媒体に記録されるデータに応じたストラテジパルスに応じて前記フィルタの透過量 を変更するように前記フィルタを制御する。  In another aspect of the optical pickup device of the present invention, the filter control means changes the transmission amount of the filter according to a strategy pulse corresponding to data recorded on the information recording medium. Control the filter.
[0017] この態様によれば、ストラテジパルスに応じて、出射光は、方形波形状に変化する 光強度で情報記録媒体の記録面に照射される。言い換えれば、通常は、ストラテジ パルスに応じて方形波形状に変化する光強度で光源力 出射光が出射されるが、こ の態様では、ストラテジパルスに応じて方形波形状に変化する光強度で出射光がフ ィルタを透過するように、フィルタの透過量が変更される。このため、光源から出射光 を照射する時点で出射光の光強度を厳密な方形波形状で変化させなくとも、方形波 形状に変化する光強度で光源力 出射光が出射される場合と同様に、出射光は、方 形波形状に変化する光強度で情報記録媒体の記録面に照射される。このため、情 報記録媒体の記録面に好適な記録マークないしは記録ピットを形成することができ、 その結果、好適にデータを記録することができる。従って、放熱を抑制しながら、好適 な記録動作を行うことができる。  According to this aspect, in accordance with the strategy pulse, the emitted light is irradiated onto the recording surface of the information recording medium with a light intensity that changes to a square wave shape. In other words, the light emitted from the light source is usually emitted with a light intensity that changes to a square wave shape according to the strategy pulse. In this aspect, the light is emitted with a light intensity that changes to a square wave shape according to the strategy pulse. The amount of transmission of the filter is changed so that the incident light passes through the filter. For this reason, even if the light intensity of the emitted light is not changed in a strict square wave shape when the emitted light is irradiated from the light source, the light source force is emitted in the same manner as when the emitted light is emitted with the light intensity changing to the square wave shape. The emitted light is applied to the recording surface of the information recording medium with a light intensity that changes to a square wave shape. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
[0018] 上述の如くストラテジパルスに応じてフィルタの透過量を変更する光ピックアップ装 置の態様では、前記ストラテジパルスは、所定の第 1振幅を有する第 1パルスと前記 第 1振幅よりも小さい第 2振幅を有する第 2パルスとを少なくとも含んでおり、前記フィ ルタ制御手段は、前記第 1パルスに応じた前記フィルタの透過量が、前記第 2パルス に応じた前記フィルタの透過量よりも増加するように前記フィルタを制御するように構 成してちょい。 [0018] In the aspect of the optical pickup device that changes the transmission amount of the filter in accordance with the strategy pulse as described above, the strategy pulse includes a first pulse having a predetermined first amplitude and a first pulse smaller than the first amplitude. At least a second pulse having two amplitudes, wherein the filter control means increases the transmission amount of the filter in response to the first pulse than the transmission amount of the filter in response to the second pulse. Control the filter to Make it.
[0019] このように構成すれば、ストラテジパルスに応じて、好適にフィルタの透過量を変更 することができる。具体的には、ストラテジパルスの振幅に応じて、フィルタの透過量 を変更することができる。このため、情報記録媒体の記録面に好適な記録マークない しは記録ピットを形成することができ、その結果、好適にデータを記録することができ る。従って、放熱を抑制しながら、好適な記録動作を行うことができる。  With this configuration, it is possible to suitably change the transmission amount of the filter according to the strategy pulse. Specifically, the transmission amount of the filter can be changed according to the amplitude of the strategy pulse. Therefore, a suitable recording mark or recording pit can be formed on the recording surface of the information recording medium, and as a result, data can be recorded suitably. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
[0020] 本発明の光ピックアップ装置の他の態様は、前記光強度制御手段は、前記情報記 録媒体に記録されるデータに応じて前記出射光の光強度を変化させるように前記光 源を制御する。  In another aspect of the optical pickup device of the present invention, the light intensity control means controls the light source so as to change the light intensity of the emitted light according to data recorded on the information recording medium. Control.
[0021] この態様によれば、記録されるデータに応じて、略正弦波形状に変化する光強度 の出射光が光源から照射される。  [0021] According to this aspect, the light source emits the emitted light having a light intensity that changes in a substantially sinusoidal shape according to the recorded data.
[0022] 本発明の光ピックアップ装置の他の態様は、前記光強度制御手段は、前記情報記 録媒体に記録されるデータに応じたストラテジパルスに応じて前記出射光の光強度 を変化させるように前記光源を制御する。  In another aspect of the optical pickup device of the present invention, the light intensity control means changes the light intensity of the emitted light according to a strategy pulse corresponding to data recorded on the information recording medium. The light source is controlled.
[0023] この態様によれば、ストラテジパルスに応じて、略正弦波形状に変化する光強度の 出射光が光源力 照射される。言い換えれば、通常は、ストラテジパルスに応じて方 形波形状に変化する光強度で光源力も出射光が出射されるが、この態様では、ストラ テジパルスに応じて略正弦波形状に変化する光強度で光源から出射光が出射され る。  [0023] According to this aspect, the emitted light having the light intensity that changes in a substantially sinusoidal shape in accordance with the strategy pulse is irradiated with the light source power. In other words, the emitted light is usually emitted with a light intensity that changes to a square wave shape according to the strategy pulse. In this aspect, the light intensity changes to a substantially sine wave shape according to the strategy pulse. Outgoing light is emitted from the light source.
[0024] 上述の如くストラテジパルスに応じて出射光の光強度を変化させる光ピックアップ装 置の態様では、前記ストラテジパルスは、所定の第 1振幅を有する第 1パルスと前記 第 1振幅よりも小さい第 2振幅を有する第 2パルスとを少なくとも含んでおり、前記光強 度制御手段は、前記第 1パルスに応じた前記出射光の光強度が、前記第 2パルスに 応じた前記出射光の光強度よりも大きくなるように前記光源を制御するように構成し てもよい。  [0024] In the aspect of the optical pickup device that changes the light intensity of the emitted light according to the strategy pulse as described above, the strategy pulse is smaller than the first pulse having a predetermined first amplitude and the first amplitude. At least a second pulse having a second amplitude, and the light intensity control means has a light intensity of the emitted light according to the first pulse, and the light intensity of the emitted light according to the second pulse. You may comprise so that the said light source may be controlled so that it may become larger than intensity | strength.
[0025] このように構成すれば、光源から出射される出射光の光強度は、ストラテジパルスに 応じて方形波形状に変化しなくとも、方形波形状と概ね同様の傾向で変化する略正 弦波形状に変化する。 [0026] 本発明の光ピックアップ装置の他の態様は、前記出射光の光強度の増減における 立ち上がり及び立ち下がりの夫々の位相と、前記フィルタの透過量の変更における 立ち上がり及び立ち下がりの夫々の位相とを同期させる同期手段を更に備える。 [0025] With this configuration, even if the light intensity of the emitted light emitted from the light source does not change to a square wave shape according to the strategy pulse, it is a substantially sine string that changes with a tendency similar to that of the square wave shape. It changes to a wave shape. [0026] Another aspect of the optical pickup device of the present invention is that each phase of rise and fall in the increase and decrease of the light intensity of the emitted light and each phase of rise and fall in the change of the transmission amount of the filter And a synchronizing means for synchronizing the.
[0027] この態様によれば、出射光の光強度の増減における立ち上がり(即ち、光強度が増 加していく期間)の位相と、フィルタの透過量の変更における立ち上がり(即ち、フィ ルタの透過量が増加していく期間)の位相とを同期させることができる。また、出射光 の光強度の増減における立ち下がり(即ち、光強度が減少していく期間)の位相と、 フィルタの透過量の変更における立ち下がり(即ち、フィルタの透過量が減少していく 機関)の位相とを同期させることができる。フィルタにおける出射光の不必要な遮断や 不必要な透過が生ずる事態を減少ないしはなくすことができる。  [0027] According to this aspect, the phase of the rise in the increase or decrease in the light intensity of the emitted light (that is, the period during which the light intensity increases) and the rise in the change in the transmission amount of the filter (that is, the transmission of the filter). It is possible to synchronize with the phase of the period during which the amount increases. In addition, the phase of the fall (that is, the period during which the light intensity decreases) in the increase and decrease of the light intensity of the emitted light and the fall (that is, the transmission quantity of the filter decreases) in the change in the transmission amount of the filter. ) Phase can be synchronized. It is possible to reduce or eliminate the situation where unnecessary blocking or unnecessary transmission of emitted light in the filter occurs.
[0028] 上述の如く同期手段を更に備える光ピックアップ装置の態様では、前記フィルタを 透過した前記出射光の光強度をモニタリングするモニタリング手段を更に備え、前記 同期手段は、モニタリングされた光強度の積分値と所定の基準値とを比較することで 、前記位相を同期させるように構成してもよい。  [0028] In the aspect of the optical pickup device further including the synchronization unit as described above, the optical pickup device further includes a monitoring unit that monitors the light intensity of the emitted light that has passed through the filter, and the synchronization unit integrates the monitored light intensity. The phase may be synchronized by comparing the value with a predetermined reference value.
[0029] このように構成すれば、モニタリングされた光強度の積分値と基準値とを比較するこ とで、出射光の光強度の増減における立ち上がり及び立ち下がりの夫々の位相と、フ ィルタの透過量の変更における立ち上がり及び立ち下がりの夫々の位相とを、比較 的容易に同期させることができる。  [0029] With this configuration, by comparing the monitored integrated value of the light intensity with the reference value, each phase of rising and falling in the increase and decrease of the light intensity of the emitted light, and the filter It is possible to relatively easily synchronize the rising and falling phases in changing the transmission amount.
[0030] 上述の如くモニタリング手段を更に備える光ピックアップ装置の態様では、時間 tに おける前記出射光の光強度の積分値を V (t)とすると、前記同期手段は、 V(t+ A t) — V (t)が 0又は最大値をとるように前記位相を同期させるように構成してもよ!/、。  [0030] In the aspect of the optical pickup device further including the monitoring unit as described above, if the integrated value of the light intensity of the emitted light at time t is V (t), the synchronization unit is V (t + At) — It may be configured to synchronize the phase so that V (t) takes 0 or the maximum value! /.
[0031] フィルタを透過した後の出射光の光強度は、方形波形状に変化するため、フィルタ を透過した後の出射光は、そのパルスが ON状態にあるか又はそのパルスが OFF状 態にあるかの 2つの状態となりえる。従って、このように構成すれば、相前後する時間 帯にモニタリングされた光強度の積分値を比較することで、出射光の光強度の増減 における立ち上がり及び立ち下がりの夫々の位相と、フィルタの透過量の変更におけ る立ち上がり及び立ち下がりの夫々の位相とを、比較的容易に同期させることができ る。尚、モニタリングされた光強度の積分値を基準値と比較する動作は、モニタリング される光強度の積分値が 0又は最大値をとる力否かを判定する動作と同等である。 [0031] Since the light intensity of the outgoing light after passing through the filter changes to a square wave shape, the outgoing light after passing through the filter has its pulse in the ON state or its pulse in the OFF state. There can be two states. Therefore, with this configuration, by comparing the integrated values of the light intensity monitored in successive time zones, the rising and falling phases in the increase and decrease of the light intensity of the emitted light, and the transmission of the filter It is possible to relatively easily synchronize the rising and falling phases in changing the quantity. The operation of comparing the integrated value of the monitored light intensity with the reference value is the monitoring This is equivalent to the operation for determining whether the integrated value of the light intensity is 0 or a maximum value.
[0032] 本発明の光ピックアップ装置の他の態様は、前記フィルタは、印加される電圧の値 により吸収波長が変化する吸光層と、前記吸光層に対して前記電圧を印加する電極 とを備えており、前記フィルタ制御手段は、前記電極に対して印加する前記電圧の値 を変更することで、前記フィルタの透過量を変更するように前記フィルタを制御する。 [0032] In another aspect of the optical pickup device of the present invention, the filter includes a light absorption layer whose absorption wavelength varies depending on a value of an applied voltage, and an electrode that applies the voltage to the light absorption layer. The filter control means controls the filter so as to change a transmission amount of the filter by changing a value of the voltage applied to the electrode.
[0033] この態様によれば、吸光層に印加される電圧を変更することで、フィルタの透過量 を増減させることができる。 [0033] According to this aspect, the transmission amount of the filter can be increased or decreased by changing the voltage applied to the light absorption layer.
[0034] 本発明の光ピックアップ装置の他の態様は、前記フィルタは、印加される電圧の値 により分子配列が変化する液晶素子を含む液晶層と、前記液晶層に対して前記電 圧を印加する電極とを備えており、前記フィルタ制御手段は、前記電極に対して印加 する前記電圧の値を変更することで、前記フィルタの透過量を変更するように前記フ ィルタを制御する。 [0034] In another aspect of the optical pickup device of the present invention, the filter applies a liquid crystal layer including a liquid crystal element whose molecular arrangement changes depending on a value of an applied voltage, and the voltage to the liquid crystal layer. The filter control means controls the filter so as to change the transmission amount of the filter by changing the value of the voltage applied to the electrode.
[0035] この態様によれば、液晶層に印加される電圧を変更することで、フィルタの透過量 を増減させることができる。  According to this aspect, the transmission amount of the filter can be increased or decreased by changing the voltage applied to the liquid crystal layer.
[0036] 本発明の光ピックアップ装置の他の態様は、前記フィルタは、前記出射光の光路に 対して予め定められた角度を持って配置されて 、る。  In another aspect of the optical pickup device of the present invention, the filter is disposed with a predetermined angle with respect to the optical path of the emitted light.
[0037] この態様によれば、フィルタに入射する出射光力 フィルタ内で反射されることで生 成され得る迷光の生成要因を好適に排除することができる。  [0037] According to this aspect, it is possible to suitably eliminate stray light generation factors that can be generated by being reflected in the output light power filter incident on the filter.
[0038] (照射方法)  [0038] (Irradiation method)
本発明の照射方法は、情報記録媒体の記録面に出射光を照射する光源と、前記 出射光の光路上に配置され、入射される前記出射光の透過量を変更するフィルタと を備える光ピックアップ装置における前記出射光の照射方法であって、前記出射光 の光強度を略正弦波形状に変化させるように前記光源を制御する光強度制御工程 と、前記出射光の透過量を変更するように前記フィルタを制御するフィルタ制御工程 とを備える。  An irradiation method of the present invention comprises an optical pickup comprising: a light source that irradiates a recording surface of an information recording medium with emitted light; and a filter that is disposed on an optical path of the emitted light and changes a transmission amount of the incident emitted light. A method of irradiating the emitted light in an apparatus, wherein a light intensity control step of controlling the light source so as to change a light intensity of the emitted light into a substantially sinusoidal shape, and changing a transmission amount of the emitted light. A filter control step for controlling the filter.
[0039] 本発明の照射方法によれば、上述した本発明の光ピックアップ装置が享受する利 益と同様の利益を享受することができる。  [0039] According to the irradiation method of the present invention, it is possible to receive the same benefits as the benefits of the optical pickup device of the present invention described above.
[0040] 尚、上述した本発明の光ピックアップ装置における各種態様に対応して、本発明の 照射方法も各種態様を採ることが可能である。 [0040] Incidentally, in response to the various aspects of the optical pickup device of the present invention described above, The irradiation method can also take various forms.
[0041] (情報記録装置)  [0041] (Information recording device)
本発明の情報記録装置は、情報記録媒体の記録面に出射光を照射する光源と、 前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御手段と、前記出射光の光路上に配置され、入射される前記出射光の透過量 を変更するフィルタと、前記出射光の透過量を変更するように前記フィルタを制御す るフィルタ制御手段と、前記情報記録媒体にデータを記録する記録手段とを備える。 即ち、本発明の情報記録装置は、上述した本発明の光ピックアップ装置 (但し、その 各種態様を含む)と、前記情報記録媒体にデータを記録する記録手段とを備える。  An information recording apparatus of the present invention includes a light source that irradiates a recording surface of an information recording medium with emitted light, and a light intensity control unit that controls the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape. A filter that is disposed on the optical path of the emitted light and that changes a transmission amount of the incident outgoing light, a filter control unit that controls the filter to change the transmission amount of the outgoing light, and the information Recording means for recording data on a recording medium. That is, an information recording apparatus of the present invention includes the above-described optical pickup apparatus of the present invention (including various aspects thereof) and recording means for recording data on the information recording medium.
[0042] 本発明の情報記録装置によれば、上述した本発明の光ピックアップ装置が享受す る利益と同様の利益を享受しつつ、情報記録媒体にデータを記録することができる。  According to the information recording apparatus of the present invention, it is possible to record data on the information recording medium while enjoying the same benefits as the benefits of the above-described optical pickup device of the present invention.
[0043] 尚、上述した本発明の光ピックアップ装置における各種態様に対応して、本発明の 情報記録装置も各種態様を採ることが可能である。  Incidentally, in response to the various aspects of the optical pickup apparatus of the present invention described above, the information recording apparatus of the present invention can also adopt various aspects.
[0044] (情報再生装置)  [0044] (Information Reproducing Device)
本発明の情報再生装置は、情報記録媒体の記録面に出射光を照射する光源と、 前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御手段と、前記出射光の光路上に配置され、入射される前記出射光の透過量 を変更するフィルタと、前記出射光の透過量を変更するように前記フィルタを制御す るフィルタ制御手段と、前記情報記録媒体に記録されたデータを再生する再生手段 とを備える。即ち、本発明の情報記録装置は、上述した本発明の光ピックアップ装置 (但し、その各種態様を含む)と、前記情報記録媒体に記録されたデータを再生する 再生手段とを備える。  An information reproducing apparatus of the present invention includes a light source that irradiates a recording surface of an information recording medium with emitted light, and a light intensity control unit that controls the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape. A filter that is disposed on the optical path of the emitted light and that changes a transmission amount of the incident outgoing light, a filter control unit that controls the filter to change the transmission amount of the outgoing light, and the information Playback means for playing back data recorded on the recording medium. That is, an information recording apparatus according to the present invention includes the above-described optical pickup apparatus according to the present invention (including various aspects thereof) and reproducing means for reproducing data recorded on the information recording medium.
[0045] 本発明の情報再生装置によれば、上述した本発明の光ピックアップ装置が享受す る利益と同様の利益を享受しつつ、情報記録媒体に記録されたデータを再生するこ とがでさる。  According to the information reproducing apparatus of the present invention, it is possible to reproduce the data recorded on the information recording medium while enjoying the same benefits as those enjoyed by the optical pickup device of the present invention described above. Monkey.
[0046] 尚、上述した本発明の光ピックアップ装置における各種態様に対応して、本発明の 情報再生装置も各種態様を採ることが可能である。  Incidentally, in response to the various aspects of the optical pickup apparatus of the present invention described above, the information reproducing apparatus of the present invention can also adopt various aspects.
[0047] (コンピュータプログラム) 本発明の第 1コンピュータプログラムは、上述した本発明の情報記録装置 (但し、そ の各種態様を含む)〖こ備えられたコンピュータを制御する記録制御用のコンピュータ プログラムであって、該コンピュータを、前記光強度制御手段及び前記フィルタ制御 手段の少なくとも一部として機能させる。 [0047] (Computer program) A first computer program of the present invention is a recording control computer program for controlling a computer provided with the above-described information recording apparatus of the present invention (including various aspects thereof), It functions as at least a part of the light intensity control means and the filter control means.
[0048] 本発明の第 2コンピュータプログラムは、上述した本発明の情報再生装置 (但し、そ の各種態様を含む)〖こ備えられたコンピュータを制御する再生制御用のコンピュータ プログラムであって、該コンピュータを、前記光強度制御手段及び前記フィルタ制御 手段の少なくとも一部として機能させる。  [0048] A second computer program of the present invention is a computer program for reproduction control for controlling a computer provided with the above-described information reproduction apparatus of the present invention (including various aspects thereof), A computer is caused to function as at least part of the light intensity control means and the filter control means.
[0049] 本発明に係る各コンピュータプログラムによれば、当該コンピュータプログラムを格 納する ROM、 CD-ROM, DVD-ROM,ハードディスク等の記録媒体から、当該 コンピュータプログラムをコンピュータに読み込んで実行させれば、或いは、当該コン ピュータプログラムを、通信手段を介してコンピュータにダウンロードさせた後に実行 させれば、上述した本発明の情報記録装置又は情報再生装置を比較的簡単に実現 できる。 [0049] According to each computer program according to the present invention, if the computer program is read from a recording medium such as a ROM, CD-ROM, DVD-ROM, or hard disk storing the computer program and then executed by the computer. Alternatively, if the computer program is downloaded to a computer via communication means and then executed, the above-described information recording apparatus or information reproducing apparatus of the present invention can be realized relatively easily.
[0050] 尚、上述した本発明の情報記録装置又は情報再生装置における各種態様に対応 して、本発明の各コンピュータプログラムも各種態様を採ることが可能である。  [0050] Incidentally, in response to the various aspects of the information recording apparatus or information reproducing apparatus of the present invention described above, each computer program of the present invention can also adopt various aspects.
[0051] 上記課題を解決するために、コンピュータ読取可能な媒体内の第 1コンピュータプ ログラム製品は、上述した本発明の情報記録装置 (但し、その各種態様を含む)〖こ備 えられたコンピュータにより実行可會なプログラム命令を明白に具現ィ匕し、該コンビュ ータを、前記光強度制御手段及び前記フィルタ制御手段の少なくとも一部として機能 させる。  [0051] In order to solve the above problems, a first computer program product in a computer-readable medium is obtained by a computer provided with the above-described information recording apparatus (including various aspects thereof) of the present invention. Executable program instructions are clearly embodied, and the converter functions as at least a part of the light intensity control means and the filter control means.
[0052] 上記課題を解決するために、コンピュータ読取可能な媒体内の第 2コンピュータプ ログラム製品は、上述した本発明の情報再生装置 (但し、その各種態様を含む)〖こ備 えられたコンピュータにより実行可會なプログラム命令を明白に具現ィ匕し、該コンビュ ータを、前記光強度制御手段及び前記フィルタ制御手段の少なくとも一部として機能 させる。  [0052] In order to solve the above problems, a second computer program product in a computer-readable medium is obtained by a computer provided with the above-described information reproducing apparatus of the present invention (including various aspects thereof). Executable program instructions are clearly embodied, and the converter functions as at least a part of the light intensity control means and the filter control means.
[0053] 本発明の第 1又は第 2コンピュータプログラム製品によれば、当該コンピュータプロ グラム製品を格納する ROM、 CD-ROM, DVD-ROM,ハードディスク等の記録 媒体から、当該コンピュータプログラム製品をコンピュータに読み込めば、或いは、例 えば伝送波である当該コンピュータプログラム製品を、通信手段を介してコンピュータ にダウンロードすれば、上述した本発明の情報記録装置又は情報再生装置を比較 的容易に実施可能となる。更に具体的には、当該コンピュータプログラム製品は、上 述した本発明の情報記録装置又は情報再生装置として機能させるコンピュータ読取 可能なコード (或 、はコンピュータ読取可能な命令)力も構成されてよ 、。 [0053] According to the first or second computer program product of the present invention, a record such as a ROM, a CD-ROM, a DVD-ROM, or a hard disk for storing the computer program product. If the computer program product is read from a medium into a computer, or if the computer program product, which is a transmission wave, for example, is downloaded to a computer via communication means, the information recording apparatus or information reproducing apparatus of the present invention described above Can be implemented relatively easily. More specifically, the computer program product may also be configured with computer-readable code (or computer-readable instructions) that functions as the information recording apparatus or information reproducing apparatus of the present invention described above.
[0054] 本発明のこのような作用及び他の利得は次に説明する実施例から更に明らかにさ れよう。  [0054] These effects and other advantages of the present invention will become more apparent from the embodiments described below.
[0055] 以上説明したように、本発明の光ピックアップ装置によれば、光源と、光強度制御手 段と、フィルタと、フィルタ制御手段とを備える。従って、放熱を抑制しながら好適な記 録動作及び再生動作を行うことができる。  [0055] As described above, the optical pickup device of the present invention includes a light source, a light intensity control means, a filter, and a filter control means. Therefore, a suitable recording operation and reproduction operation can be performed while suppressing heat dissipation.
[0056] 本発明の照射方法によれば、光強度制御工程と、フィルタ制御工程とを備える。従 つて、放熱を抑制しながら好適な記録動作及び再生動作を行うことができる。 [0056] The irradiation method of the present invention includes a light intensity control step and a filter control step. Therefore, it is possible to perform a suitable recording operation and reproducing operation while suppressing heat dissipation.
[0057] 本発明の情報記録装置によれば、光源と、光強度制御手段と、フィルタと、フィルタ 制御手段と、記録手段とを備える。従って、放熱を抑制しながら、好適な記録動作を 行うことができる。 [0057] The information recording apparatus of the present invention includes a light source, a light intensity control means, a filter, a filter control means, and a recording means. Therefore, a suitable recording operation can be performed while suppressing heat dissipation.
[0058] 本発明の情報再生装置によれば、光源と、光強度制御手段と、フィルタと、フィルタ 制御手段と、再生手段とを備える。従って、放熱を抑制しながら、好適な再生動作を 行うことができる。  [0058] According to the information reproducing apparatus of the present invention, the light source, the light intensity control means, the filter, the filter control means, and the reproduction means are provided. Therefore, a suitable reproduction operation can be performed while suppressing heat dissipation.
図面の簡単な説明  Brief Description of Drawings
[0059] [図 1]第 1実施例に係る情報記録再生装置の基本構成を概念的に示すブロック図で ある。  FIG. 1 is a block diagram conceptually showing the basic structure of an information recording / reproducing apparatus in a first example.
[図 2]フィルタの第 1の具体例を概念的に示す断面図である。  FIG. 2 is a sectional view conceptually showing a first specific example of the filter.
[図 3]フィルタの第 2の具体例を概念的に示す断面図である。  FIG. 3 is a sectional view conceptually showing a second specific example of the filter.
[図 4]フィルタの第 3の具体例を概念的に示す断面図である。  FIG. 4 is a sectional view conceptually showing a third specific example of the filter.
[図 5]記録信号 (記録データ)に応じた記録ストラテジの波形、レーザダイオードから 照射される光ビームの光強度、フィルタの透過量、及び光ディスクに照射される光ビ 一ムの光強度の夫々の、時間軸に沿った変化の様子を概念的に示すグラフである。 [図 6]光ビームのオーバーシュート及びアンダーシュートを示す波形図である。 [Fig. 5] Waveform of recording strategy according to recording signal (recording data), light intensity of light beam emitted from laser diode, transmission amount of filter, and light intensity of light beam irradiated to optical disk, respectively It is a graph which shows notably the mode of the change along a time-axis. FIG. 6 is a waveform diagram showing overshoot and undershoot of a light beam.
圆 7]第 2実施例に係る情報記録再生装置の基本構成を概念的に示すブロック図で ある。  [7] FIG. 7 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the second example.
[図 8]フィルタの透過量を変化させるタイミングをずらさな ヽ場合の、レーザダイオード から照射される光ビームの光強度、フィルタの透過量、及び光ディスクに照射される 光ビームの光強度の夫々の、時間軸に沿った変化の様子を概念的に示すグラフで ある。  [FIG. 8] When the timing of changing the transmission amount of the filter is not shifted, the light intensity of the light beam emitted from the laser diode, the transmission amount of the filter, and the light intensity of the light beam emitted to the optical disc are It is a graph which shows notionally the mode of change along a time axis.
[図 9]フィルタの透過量を変化させるタイミングをずらした場合の、レーザダイオードか ら照射される光ビームの光強度、フィルタの透過量、及び光ディスクに照射される光 ビームの光強度の夫々の、時間軸に沿った変化の様子を概念的に示すグラフである 符号の説明  [FIG. 9] The light intensity of the light beam emitted from the laser diode, the transmission quantity of the filter, and the light intensity of the light beam emitted to the optical disk when the timing of changing the transmission quantity of the filter is shifted. , Is a graph conceptually showing the state of change along the time axis
[0060] 1、2 情報記録再生装置 [0060] 1, 2 Information recording / reproducing apparatus
10、 10a 光ピックアップ  10, 10a optical pickup
11 レーザダイオード  11 Laser diode
12 フロントモニタ  12 Front monitor
13 フイノレタ  13 Huinoleta
24 CPU  24 CPU
26 レーザドライブ  26 Laser drive
27 フィルタ素子ドライブ回路  27 Filter element drive circuit
31 積分回路  31 Integration circuit
32 参照値格納回路  32 Reference value storage circuit
33 コンノ レータ  33 Contortor
34 位相補償サーボ回路  34 Phase compensation servo circuit
50 光ディスク  50 optical disc
発明を実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION
[0061] 以下、本発明を実施するための最良の形態について実施例毎に順に図面に基づ いて説明する。尚、以下の実施例では、本発明の光ピックアップ装置に係る実施例を 備える、 CDや DVDや Blu— my Disc等の各種光ディスクに対するデータの記録及 び再生を行うことができる情報記録再生装置について説明を進める。 Hereinafter, the best mode for carrying out the present invention will be described in each embodiment in order with reference to the drawings. In the following embodiments, the embodiments relating to the optical pickup device of the present invention are described. We will explain the information recording / playback device that can record and play back data on various optical disks such as CD, DVD, Blu-my Disc, etc.
[0062] (1) 第 1実施例 [0062] (1) First Example
(1 - 1) 情報記録再生装置の基本構成  (1-1) Basic configuration of information recording / reproducing device
初めに、図 1を参照して、第 1実施例に係る情報記録再生装置の基本構成につい て説明を進める。ここに、図 1は、第 1実施例に係る情報記録再生装置の基本構成を 概念的に示すブロック図である。  First, the basic configuration of the information recording / reproducing apparatus in the first example will be described with reference to FIG. FIG. 1 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the first example.
[0063] 図 1に示すように、第 1実施例に係る情報記録再生装置 1は、光ピックアップ 10と、 フォトディテクタ(PD: Photo Detector)用アンプ 21と、再生回路 22と、 CPU24と、記 録回路 25と、レーザドライブ回路 26と、フィルタ素子ドライブ回路 27と、スピンドルモ ータ 28とを備える。 As shown in FIG. 1, the information recording / reproducing apparatus 1 according to the first embodiment includes an optical pickup 10, a photo detector (PD) amplifier 21, a reproducing circuit 22, a CPU 24, and a recording A circuit 25, a laser drive circuit 26, a filter element drive circuit 27, and a spindle motor 28 are provided.
[0064] 光ピックアップ 10は、光ディスク 50に対して光ビームを照射し、光ディスク 50に対 するデータの記録及び再生を行うために用いられる。力かる機能を実現するため、光 ピックアップ 10は、レーザダイオード 11と、フィルタ 13と、ビームスプリッタ 14と、対物 レンズ 15と、集光レンズ 16と、フォトディテクタ 17とを備えている。  The optical pickup 10 is used to irradiate the optical disc 50 with a light beam and to record and reproduce data on the optical disc 50. In order to realize a powerful function, the optical pickup 10 includes a laser diode 11, a filter 13, a beam splitter 14, an objective lens 15, a condenser lens 16, and a photodetector 17.
[0065] レーザダイオード 11は、本発明における「光源」の一具体例を構成しており、レーザ ドライブ回路 26から供給される駆動信号に基づき、一種類の又は複数種類の異なる 波長の光ビームを照射する。例えば、光ディスク 50の一具体例を構成する DVDに対 してデータの記録及び再生を行う際には、レーザダイオード 11は、概ね 660nmの波 長を有する光ビームを照射する。例えば、光ディスク 50の一具体例を構成する CDに 対してデータの記録及び再生を行う際には、レーザダイオード 11は、概ね 780nmの 波長を有する光ビームを照射する。例えば、光ディスク 50の一具体例を構成する Blu -ray Discに対してデータの記録及び再生を行う際には、レーザダイオード 11は、 概ね 405nmの波長を有する光ビームを照射する。  The laser diode 11 constitutes a specific example of the “light source” in the present invention. Based on the drive signal supplied from the laser drive circuit 26, the laser diode 11 emits one type or plural types of light beams having different wavelengths. Irradiate. For example, when data is recorded and reproduced on a DVD constituting a specific example of the optical disk 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 660 nm. For example, when data is recorded and reproduced on a CD constituting a specific example of the optical disc 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 780 nm. For example, when recording and reproducing data on a Blu-ray Disc constituting a specific example of the optical disc 50, the laser diode 11 irradiates a light beam having a wavelength of approximately 405 nm.
[0066] フィルタ 13は、フィルタ素子ドライブ回路 27による制御の下、該フィルタ 13に入射 する光ビームの透過量 (即ち、該フィルタ 13に入射する光ビームに対する透過率)を 変更可能な構成を有している。尚、このフィルタ 13の具体的な構成については、後 に詳述する(図 2から図 4参照)。 [0067] ビームスプリッタ 14は、レーザダイオード 11の側力も入射する光ビームを、光デイス ク 50に向力 ように 90%だけ反射して且つ 10%だけ透過すると共に、光ディスク 50 の側から入射する光ビーム (即ち、光ビームの光ディスク 50からの反射光)をそのまま 100%透過する。 The filter 13 has a configuration capable of changing the transmission amount of the light beam incident on the filter 13 (that is, the transmittance for the light beam incident on the filter 13) under the control of the filter element drive circuit 27. is doing. The specific configuration of the filter 13 will be described in detail later (see FIGS. 2 to 4). [0067] The beam splitter 14 reflects 90% of the light beam, which is also incident on the side force of the laser diode 11, to the optical disk 50 and transmits 10%, and is incident from the optical disk 50 side. The light beam (that is, the light reflected from the optical disk 50) is transmitted 100% as it is.
[0068] 対物レンズ 15は、入射する光ビーム^^光して、光ディスク 50の記録面上に照射 する。  The objective lens 15 emits an incident light beam and irradiates the recording surface of the optical disc 50.
[0069] 集光レンズ 16は、ビームスプリッタ 14においてそのまま透過された光ビーム(すな わち、光ビームの光ディスク 50からの反射光)を集光して、フォトディテクタ 17の受光 面上に照射する。  [0069] The condensing lens 16 condenses the light beam transmitted through the beam splitter 14 as it is (that is, the light beam reflected from the optical disk 50) and irradiates the light receiving surface of the photodetector 17 with the light beam. .
[0070] フォトディテクタ 17は、例えば、フォトダイオードにより構成され、集光レンズ 16から 照射される光ビームを受光して、受光した光ビームのパワーに応じた検出信号を、フ オトディテクタ用アンプ 21に出力する。  [0070] The photodetector 17 is configured by, for example, a photodiode, receives the light beam emitted from the condenser lens 16, and sends a detection signal corresponding to the power of the received light beam to the photodetector amplifier 21. Output.
[0071] フォトディテクタ用アンプ 21は、フォトディテクタ 17より出力される検出信号から、 RF 信号を生成し、該 RF信号を再生回路 22に出力する。  The photodetector amplifier 21 generates an RF signal from the detection signal output from the photodetector 17 and outputs the RF signal to the reproduction circuit 22.
[0072] 再生回路 22は、本発明における「再生手段」の一具体例を構成しており、フォトディ テクタ用アンプ 21から出力される RF信号に対して、復調処理ゃ復号処理や誤り訂正 処理やデコード処理等を施して、再生信号を生成する。再生回路 22は、生成した再 生信号を外部のディスプレイやスピーカ等に出力し、その結果、光ディスク 50に記録 されているデータ力 例えば映像コンテンツや音声コンテンツ或いはその他のコンテ ンッとして再生される。  [0072] The reproduction circuit 22 constitutes one specific example of the "reproduction means" in the present invention. The RF signal output from the photodetector amplifier 21 is demodulated, decoded, or error-corrected. Or a decoding process or the like to generate a reproduction signal. The reproduction circuit 22 outputs the generated reproduction signal to an external display, a speaker or the like, and as a result, it is reproduced as data power recorded on the optical disc 50, for example, video content, audio content, or other content.
[0073] CPU24は、情報記録再生装置 1の各構成要素とバスを介して接続され、各構成要 素に指示を行うことで、情報記録再生装置 1全体の制御を行う。通常、 CPU24が動 作するためのソフトウエア又はファームウエアは、情報記録再生装置 1内のメモリに格 納されている。  [0073] The CPU 24 is connected to each component of the information recording / reproducing apparatus 1 via a bus, and controls the entire information recording / reproducing apparatus 1 by giving an instruction to each component. Usually, software or firmware for the CPU 24 to operate is stored in a memory in the information recording / reproducing apparatus 1.
[0074] 記録回路 25は、本発明における「記録手段」の一具体例を構成しており、光デイス ク 50に記録するためのデータとして外部より入力される記録データに対して、誤り訂 正符号付加処理や変調処理や暗号化処理やエンコード処理等を施して、記録信号 を生成する。生成された記録信号は、レーザドライブ回路 26に出力される。 [0075] レーザドライブ回路 26は、 CPU24の制御を受けることによって本発明の「光強度 制御手段」の一具体例を構成しており、レーザダイオード 11の動作を制御するため の駆動信号をレーザダイオード 11に対して出力する。より具体的には、レーザドライ ブ回路 26は、光ディスク 50に対してデータを記録する際には、書き込み光として所 定のパワーで、或いは CPU24から出力されるパワーの値に応じたパワー(以下、「記 録パワー」という)で、且つ記録回路 25より出力される記録信号に応じた変調を施し ながら光ビームが照射されるような駆動信号を生成し、レーザダイオード 11に出力す る。或いは、レーザドライブ回路 26は、光ディスク 50に記録されたデータを再生する 際には、読み取り光として所定のパワーで、或いは CPU24から出力されるパワーの 値に応じたパワーで (以下、「再生パワー」 t 、う)光ビームが照射されるような駆動信 号を生成し、レーザダイオード 11に出力する。 The recording circuit 25 constitutes one specific example of “recording means” in the present invention, and corrects errors with respect to recording data input from the outside as data for recording on the optical disk 50. A recording signal is generated by performing code addition processing, modulation processing, encryption processing, encoding processing, and the like. The generated recording signal is output to the laser drive circuit 26. The laser drive circuit 26 constitutes a specific example of the “light intensity control means” of the present invention under the control of the CPU 24, and a drive signal for controlling the operation of the laser diode 11 is transmitted to the laser diode. Output to 11. More specifically, when recording data on the optical disc 50, the laser drive circuit 26 uses a predetermined power as a write light or a power (hereinafter referred to as a power value output from the CPU 24). And a recording signal that is irradiated with a light beam while being modulated in accordance with the recording signal output from the recording circuit 25, and outputs it to the laser diode 11. Alternatively, when reproducing the data recorded on the optical disc 50, the laser drive circuit 26 uses a predetermined power as reading light or a power corresponding to a power value output from the CPU 24 (hereinafter referred to as “reproduction power”). T)) Generate a drive signal that is irradiated with the light beam and output it to the laser diode 11.
[0076] フィルタ素子ドライブ回路 27は、 CPU24の制御を受けることによって本発明の「フィ ルタ制御手段」の一具体例を構成しており、フィルタ 13に入射する光ビームの透過 量の変更を制御可能に構成されている。  The filter element drive circuit 27 constitutes a specific example of the “filter control means” of the present invention under the control of the CPU 24, and controls the change in the transmission amount of the light beam incident on the filter 13. It is configured to be possible.
[0077] スピンドルモータ 28は、光ディスク 50を回転及び停止させるもので、光ディスク 50 へのアクセス時に動作する。より詳細には、スピンドルモータ 28は、図示しないサー ボユニット等によりスピンドルサーボを受けつつ所定速度で光ディスク 50を回転及び 停止させるように構成されて 、る。  The spindle motor 28 rotates and stops the optical disc 50, and operates when accessing the optical disc 50. More specifically, the spindle motor 28 is configured to rotate and stop the optical disc 50 at a predetermined speed while receiving spindle servo from a servo unit (not shown) or the like.
[0078] 以上のような構成を有する情報記録再生装置 1においては、レーザダイオード 11か ら照射される光ビームは、フィルタ 13に入射する。この際、レーザダイオード 11から 照射される光ビームはフィルタ 13により透過量が制御された後、ビームスプリッタ 14 において反射されて、対物レンズ 15に入射され、光ディスク 50上に集光される。この ようにして、光ディスク 50上に光ビームが集光されると、当該光ビームは、光ディスク 5 0において反射された後、再度、対物レンズ 15を介してビームスプリッタ 14に入射し 、ビームスプリッタ 14を透過する。その後、集光レンズ 16に入射し、集光レンズ 16〖こ よりフォトディテクタ 17上に集光される。この結果、フォトディテクタ 17から受光信号が フォトディテクタ用アンプ 21に出力され、且つフォトディテクタ用アンプ 21から RF信 号が再生回路 22に出力される。 [0079] また、フォトディテクタ 17から RF信号が出力されると、 CPU24は、光ディスク 50に 記録されているデータの再生時には、当該 RF信号に対応するデータを再生するよう に再生回路 22を制御し、再生回路 22は、当該データを外部に出力する。これに対し て、光ディスク 50に対するデータの記録時には、 CPU24は、例えば、光ディスク 50 上のアドレス取得や記録すべきデータに対応した駆動信号の出力タイミングをこの R F信号に基づ 、て決定する。 In the information recording / reproducing apparatus 1 having the above-described configuration, the light beam emitted from the laser diode 11 is incident on the filter 13. At this time, the light beam irradiated from the laser diode 11 is controlled by the filter 13 and then reflected by the beam splitter 14, enters the objective lens 15, and is condensed on the optical disk 50. When the light beam is collected on the optical disk 50 in this way, the light beam is reflected by the optical disk 50 and then enters the beam splitter 14 again through the objective lens 15, so that the beam splitter 14 Transparent. Thereafter, the light enters the condensing lens 16 and is condensed on the photodetector 17 by the condensing lens 16 mm. As a result, a light reception signal is output from the photodetector 17 to the photodetector amplifier 21, and an RF signal is output from the photodetector amplifier 21 to the reproduction circuit 22. [0079] When the RF signal is output from the photodetector 17, the CPU 24 controls the reproduction circuit 22 to reproduce the data corresponding to the RF signal when reproducing the data recorded on the optical disc 50, The reproduction circuit 22 outputs the data to the outside. On the other hand, when data is recorded on the optical disc 50, the CPU 24 determines the output timing of the drive signal corresponding to the address acquisition and data to be recorded on the optical disc 50 based on this RF signal, for example.
[0080] (1 - 2) フィルタの基本構成  [0080] (1-2) Basic filter configuration
続いて、図 2から図 4を参照して、フィルタ 13の具体的構成について説明を進める。 ここに、図 2は、フィルタ 13の第 1の具体例を概念的に示す断面図であり、図 3は、フ ィルタ 13の第 2の具体例を概念的に示す断面図であり、図 4は、フィルタ 13の第 3の 具体例を概念的に示す断面図である。  Next, a specific configuration of the filter 13 will be described with reference to FIGS. FIG. 2 is a sectional view conceptually showing a first specific example of the filter 13, and FIG. 3 is a sectional view conceptually showing a second specific example of the filter 13, and FIG. FIG. 5 is a sectional view conceptually showing a third specific example of the filter 13.
[0081] まず、本実施例にお!、てフィルタ 13は、例えば、 EC (Electrochromic)材料と呼ば れる材料を利用して構成することができる。この EC材料は、印加電圧により可逆的に 吸収波長が変化するエレクト口クロイズム現象を起こす材料であり、印加電圧により透 明な状態力 所定周波数の光線のみを吸光して各色を呈した状態に変化する特性 を有している。この EC材料としては、無機系、有機系の 2系統が存在し、無機系 EC 材料としては、例えば、電気吸光反応を利用した W03 (三酸ィ匕タングステン)、 MoO 3 (三酸化モリブデン)等の力ソード EC (還元により着色)や、プルシアンブルー (KxF eyFez(CN)6)、 Ni(OH) n等のァノーデイツク EC (酸ィ匕により着色)があり、有機 EC材 料としては、有機 EL (Electro Luminescent)材料として用いられる、ポリフエナザシリン 等の機能性高分子がある。  First, in the present embodiment, the filter 13 can be configured using a material called an EC (Electrochromic) material, for example. This EC material is a material that causes the electochromism phenomenon in which the absorption wavelength reversibly changes depending on the applied voltage. Transparent state force is absorbed by the applied voltage, and changes to a state in which each color is exhibited by absorbing only light of a predetermined frequency. It has the characteristics to There are two types of EC materials, inorganic and organic. Examples of inorganic EC materials include W03 (tungsten trioxide) and MoO 3 (molybdenum trioxide) using electroabsorption reaction. Power Sword EC (colored by reduction) and Prussian blue (KxFeyFez (CN) 6), Nianod EC (colored by acid) such as Ni (OH) n, and organic EL materials are organic EL There are functional polymers such as polyphenacillin that are used as (Electro Luminescent) materials.
[0082] 図 2に示すように、フィルタ 13の第 1の具体例(以下、「フィルタ 13a」という)は、例え ば Si02 (酸ィ匕珪素)のような透過性の高い基材により構成される基板 101を備える。 この基板 101上には透明電極 102が形成され、この透明電極 102上にゾル 'ゲル法 或いは引き上げ法、蒸着等の方法による製膜後、焼成を行うことにより EC層 103が 形成される。また、この EC層 103上には、更に透明電極 104が積層される。この結果 、透明電極 102と透明電極 104の間に EC層 103がサンドイッチされた状態にて形成 されることとなる。透明電極 102及び透明電飾 104は、夫々、フィルタ素子ドライブ回 路 27内に設けられている電源と接続されており、フィルタ素子ドライブ回路 27は、透 明電極 102と透明電極 104との間に所定の電圧を印加することにより、 EC層 103に おける吸光特性 (例えば、吸収波長)を可逆的に変更させることとなる。つまり、フィル タ 13aに入射する光ビームの透過量を可逆的に変更させることとなる。 [0082] As shown in Fig. 2, the first specific example of the filter 13 (hereinafter referred to as "filter 13a") is made of a highly permeable base material such as Si02 (acid-silicon). A substrate 101 is provided. A transparent electrode 102 is formed on the substrate 101, and an EC layer 103 is formed on the transparent electrode 102 by film formation by a sol-gel method, a pulling method, vapor deposition, or the like, followed by baking. A transparent electrode 104 is further laminated on the EC layer 103. As a result, the EC layer 103 is sandwiched between the transparent electrode 102 and the transparent electrode 104. The transparent electrode 102 and the transparent illumination 104 are respectively connected to the filter element drive circuit. The filter element drive circuit 27 is connected to a power source provided in the path 27, and the filter element drive circuit 27 applies a predetermined voltage between the transparent electrode 102 and the transparent electrode 104 to thereby absorb light in the EC layer 103. (For example, the absorption wavelength) is reversibly changed. That is, the transmission amount of the light beam incident on the filter 13a is reversibly changed.
[0083] なお、 EC材料における吸光度は、利用する材料によって異なるため、具体的にフィ ルタ 13aを設計するに際しては、レーザダイオード 11より照射される光ビームのパヮ 一を、当該フィルタ 13aを透過させることでどれだけ減少させるかに応じて、 EC層 10 3の厚さや、 EC層 103に用いられる EC材料や、 EC層 103に印加される電圧の大き さ等を決定することが好まし 、。  [0083] Since the absorbance in the EC material varies depending on the material to be used, when specifically designing the filter 13a, the filter 13a allows the light beam irradiated from the laser diode 11 to pass through the filter 13a. It is preferable to determine the thickness of the EC layer 103, the EC material used for the EC layer 103, the magnitude of the voltage applied to the EC layer 103, etc., depending on how much it is reduced.
[0084] 次に、有機 EC材料を用いた場合、図 3に示すように、フィルタ 13の第 2の具体例( 以下、「フィルタ 13b」という)は、 2枚の透明基板 111及び透明基板 114を間隙を持 つて張り合わせ、透明基板 111と透明基板 114との間に有機 EC材料カゝら構成される EC層 113を充填して構成される。透明基板 111と透明基板 114との夫々の対向面 上には、透明電極 112及び透明電極 115が形成されている。透明電極 112及び透 明電極 115の夫々は、フィルタ素子ドライブ回路 27内に設けられている電源と接続さ れており、フィルタ素子ドライブ回路 27は、透明電極 112と透明電極 115との間に所 定の電圧を印加することにより、 EC層 113における吸光特性を可逆的に変化させる こととなる。つまり、フィルタ 13bに入射する光ビームの透過量を可逆的に変更させる こととなる。  Next, when an organic EC material is used, as shown in FIG. 3, a second specific example of the filter 13 (hereinafter referred to as “filter 13b”) includes two transparent substrates 111 and 114. And an EC layer 113 composed of an organic EC material member is filled between the transparent substrate 111 and the transparent substrate 114. On the opposing surfaces of the transparent substrate 111 and the transparent substrate 114, a transparent electrode 112 and a transparent electrode 115 are formed. Each of the transparent electrode 112 and the transparent electrode 115 is connected to a power source provided in the filter element drive circuit 27, and the filter element drive circuit 27 is provided between the transparent electrode 112 and the transparent electrode 115. By applying a constant voltage, the light absorption characteristics in the EC layer 113 are reversibly changed. That is, the transmission amount of the light beam incident on the filter 13b is reversibly changed.
なお、この場合にお ヽても EC層 113の厚さや印加電圧値等を適宜設計する必要が あることは、上記無機 EC材料力も構成される EC層 103と同様である。  Even in this case, it is necessary to appropriately design the thickness, applied voltage value, and the like of the EC layer 113, as in the EC layer 103 in which the inorganic EC material force is also configured.
[0085] また、 EC材料を用いることに加えて又は代えて、コレスティック液晶等の液晶材料 を用いて、フィルタ 13を構成することもできる。コレスティック液晶は、印加される電圧 の大きさや温度に応じてその透過率を変更することができる。具体的には、図 4に示 すように、フィルタ 13の第 3の具体例(以下、「フィルタ 13c」という)は、 2枚の透明基 板 121及び透明基板 124を間隙を持って張り合わせ、透明基板 121と透明基板 124 との間に液晶材料カゝら構成される液晶層 123を充填して構成される。透明基板 121 と透明基板 124との夫々の対向面上には、透明電極 122及び透明電極 125が形成 されている。透明電極 122及び透明電極 125の夫々は、フィルタ素子ドライブ回路 2 7内に設けられている電源と接続されており、フィルタ素子ドライブ回路 27は、透明電 極 122と透明電極 125との間に所定の電圧を印加することにより、液晶層 123を構成 して 、る液晶材料中に含まれる液晶分子の配列特性を可逆的に変化させることとな る。つまり、フィルタ 13cに入射する光ビームの透過量を可逆的に変更させることとな る。なお、この場合においても液晶層 123の厚さや印加電圧値等を適宜設計する必 要があることは、上記無機 EC材料力も構成される EC層 103や有機 EC材料力も構成 される EC層 113と同様である。 [0085] In addition to or instead of using the EC material, the filter 13 can also be configured using a liquid crystal material such as a cholestic liquid crystal. The transmittance of the cholestic liquid crystal can be changed according to the applied voltage and temperature. Specifically, as shown in FIG. 4, in the third specific example of the filter 13 (hereinafter referred to as “filter 13c”), two transparent substrates 121 and 124 are bonded together with a gap between them. A liquid crystal layer 123 composed of a liquid crystal material is filled between the transparent substrate 121 and the transparent substrate 124. A transparent electrode 122 and a transparent electrode 125 are formed on the opposing surfaces of the transparent substrate 121 and the transparent substrate 124, respectively. Has been. Each of the transparent electrode 122 and the transparent electrode 125 is connected to a power source provided in the filter element drive circuit 27, and the filter element drive circuit 27 is provided between the transparent electrode 122 and the transparent electrode 125. By applying this voltage, the liquid crystal layer 123 is constituted, and the alignment characteristics of the liquid crystal molecules contained in the liquid crystal material are reversibly changed. That is, the transmission amount of the light beam incident on the filter 13c is reversibly changed. Even in this case, it is necessary to appropriately design the thickness, applied voltage value, etc. of the liquid crystal layer 123 because the EC layer 103 also includes the above-described inorganic EC material force and the EC layer 113 that also includes the organic EC material force. It is the same.
[0086] また、上述した無機 EC材料や有機 EC材料やこれスティック液晶等の液晶材料を 用いることに加えて又は代えて、フォトポリマーや、フォトリリフラクティブ液晶や、異性 化材料や、蛍光色素を用いて、上述したフィルタ 13を構成することもできる。  [0086] In addition to or instead of using the above-described inorganic EC material, organic EC material, and liquid crystal material such as stick liquid crystal, a photopolymer, a photorefractive liquid crystal, an isomerized material, or a fluorescent dye is used. Thus, the filter 13 described above can also be configured.
[0087] そして、上述したフィルタ 13は、透過量の変化をピコ秒のオーダーで或いはフェムト 秒のオーダーで行うことができる材料を用いることが好ましい。つまり、透過量が低い 状態から高!、状態への切り替え、或いは透過量が高!、状態から低!、状態への切り替 えを、ピコ秒のオーダーで或いはフェムト秒のオーダーで行うことができる材料を用い てフィルタ 13を構成することが好ましい。但し、透過量が低い状態から高い状態への 切り替え、或いは透過量が高い状態から低い状態への切り替えを、ナノ秒のオーダ 一で行うことができる材料を用いてフィルタ 13を構成してもよ 、。  [0087] The filter 13 described above is preferably made of a material that can change the amount of transmission in the order of picoseconds or in the order of femtoseconds. In other words, it is possible to switch from a low transmission level to a high !, state, or a high transmission level !, from a low state to a state, on the order of picoseconds or femtoseconds. It is preferable to configure the filter 13 using a material. However, the filter 13 may be configured using a material capable of switching from a low transmission amount to a high state or from a high transmission amount to a low state on the order of nanoseconds. ,.
[0088] (1 - 3) 情報記録再生装置の動作原理  [0088] (1-3) Operating Principle of Information Recording / Reproducing Device
続いて、図 5及び図 6を参照して、第 1実施例に係る情報記録再生装置の動作原理 について説明する。ここに、図 5は、記録信号 (記録データ)に応じた記録ストラテジ の波形、レーザダイオード 11から照射される光ビームの光強度、フィルタ 13の透過 量、及び光ディスク 50に照射される光ビームの光強度の夫々の、時間軸に沿った変 化の様子を概念的に示すグラフであり、図 6は、光ビームのオーバーシュート及びァ ンダーシュートを概念的に示す波形図である。  Next, with reference to FIG. 5 and FIG. 6, the operation principle of the information recording / reproducing apparatus in the first example will be explained. FIG. 5 shows the waveform of the recording strategy according to the recording signal (recording data), the light intensity of the light beam emitted from the laser diode 11, the transmission amount of the filter 13, and the light beam emitted to the optical disc 50. FIG. 6 is a graph conceptually showing how the light intensity changes along the time axis, and FIG. 6 is a waveform diagram conceptually showing the overshoot and undershoot of the light beam.
[0089] 以下の動作原理の説明においては、記録回路 25からレーザドライブ回路 26に出 力される記録信号によれば、図 5 (a)に示す波形で光強度が変化する光ビームを照 射することで、光ディスク 50にデータを記録することが要求されて 、るものと仮定して 説明を進める。言い換えれば、図 5 (a)に示す波形で変化する光強度での光ビーム の照射を実現可能な、図 5 (a)に示す波形と概ね同様の波形を有するストラテジパル スに応じて光ビームを照射することが必要とされているものと仮定して説明を進める。 [0089] In the following description of the operating principle, according to the recording signal output from the recording circuit 25 to the laser drive circuit 26, the light beam whose light intensity changes with the waveform shown in FIG. Assuming that data is required to be recorded on the optical disc 50 Proceed with the explanation. In other words, the light beam can be irradiated with a light intensity that changes with the waveform shown in Fig. 5 (a), and the light beam is applied according to a strategy pulse having a waveform substantially similar to the waveform shown in Fig. 5 (a). The explanation will be made assuming that it is necessary to irradiate.
[0090] この場合、レーザドライブ回路 26は、図 5 (b)に示す光強度で変化するような光ビー ムを照射するように、レーザダイオード 11を駆動する。より具体的には、レーザドライ ブ回路 26は、図 5 (a)に示す波形の立ち上がり及び立ち下がりのタイミングないしは 位相を概ね同一としつつも、図 5 (a)に示す厳密な方形波形状の波形よりも緩やかに 立ち上がり且つ緩やかに立ち下がるような態様で光ビームの光強度が変化するよう に、レーザダイオード 11を駆動する。より具体的には、レーザドライブ回路 26は、図 5 (b)に示す略正弦波形状の波形で光強度が変化するように、レーザダイオード 11を 駆動する。図 5 (a)に示す波形の振幅が相対的に大きい期間には、レーザドライブ回 路 26は、光ビームの光強度が相対的に大きくなるようにレーザダイオード 11を駆動 する。他方、図 5 (a)に示す波形の振幅が相対的に小さい期間には、レーザドライブ 回路 26は、光ビームの光強度が相対的に小さくなるようにレーザダイオード 11を駆 動する。 In this case, the laser drive circuit 26 drives the laser diode 11 so as to irradiate an optical beam that changes with the light intensity shown in FIG. 5 (b). More specifically, the laser drive circuit 26 has the exact square wave shape shown in FIG. 5 (a) while the timing or phase of the rise and fall of the waveform shown in FIG. The laser diode 11 is driven so that the light intensity of the light beam changes in such a manner that it rises more slowly than the waveform and falls more slowly. More specifically, the laser drive circuit 26 drives the laser diode 11 so that the light intensity changes in a substantially sinusoidal waveform shown in FIG. During a period in which the amplitude of the waveform shown in FIG. 5 (a) is relatively large, the laser drive circuit 26 drives the laser diode 11 so that the light intensity of the light beam becomes relatively large. On the other hand, during the period when the amplitude of the waveform shown in FIG. 5 (a) is relatively small, the laser drive circuit 26 drives the laser diode 11 so that the light intensity of the light beam becomes relatively small.
[0091] 図 5 (b)に示す光ビームの光強度の変化に対して、フィルタ制御回路 27は、図 5 (a )に示す波形と同一の或いは概ね同一の波形で透過量が変化するように、フィルタ 1 3に対して、例えば所定の電圧を印加する。より具体的には、フィルタ制御回路 27は 、フィルタ 13を透過した後の光ビームの光強度力 図 5 (a)に示す波形で変化するよ うに、フィルタ 13に対して印加する電圧を調整することで、フィルタ 13の透過量を制 御する。つまり、図 5 (a)に示す波形の振幅が相対的に大きい期間には、フィルタ素 子ドライブ回路 27は、フィルタ 13の透過量が相対的に大きくなるように所定の電圧を フィルタ 13に印加する。他方、図 5 (a)に示す波形の振幅が相対的に小さい期間に は、フィルタ素子ドライブ回路 27は、フィルタ 13の透過量が相対的に小さくなるように 所定の電圧をフィルタ 13に印加する。  [0091] In response to the change in the light intensity of the light beam shown in FIG. 5B, the filter control circuit 27 causes the transmission amount to change with the same or substantially the same waveform as that shown in FIG. 5A. For example, a predetermined voltage is applied to the filter 13. More specifically, the filter control circuit 27 adjusts the voltage applied to the filter 13 so as to change with the waveform shown in FIG. 5 (a). Thus, the transmission amount of the filter 13 is controlled. That is, during a period when the amplitude of the waveform shown in FIG. 5A is relatively large, the filter element drive circuit 27 applies a predetermined voltage to the filter 13 so that the transmission amount of the filter 13 is relatively large. To do. On the other hand, during a period in which the amplitude of the waveform shown in FIG. 5A is relatively small, the filter element drive circuit 27 applies a predetermined voltage to the filter 13 so that the transmission amount of the filter 13 is relatively small. .
[0092] その結果、図 5 (b)に示す波形で光強度が変化するようにレーザダイオード 11から 照射された光ビームは、図 5 (c)に示す波形で透過量が変化するフィルタ 13を透過 することによって、図 5 (d)に示す波形で光強度が変化しながら光ディスク 50に照射 される。 As a result, the light beam irradiated from the laser diode 11 so that the light intensity changes in the waveform shown in FIG. 5 (b) passes through the filter 13 whose transmission amount changes in the waveform shown in FIG. 5 (c). By transmitting the light, the optical intensity is changed with the waveform shown in FIG. Is done.
[0093] このように、第 1実施例によれば、レーザドライブ回路 26は、図 5 (a)に示す厳密な 方形波の形状で光強度を変化させるようにレーザダイオード 11を駆動する必要がな くなる。より具体的には、光強度が急激にないしは瞬間的に増力 tlし且つ光強度が急 激にないしは瞬間的に減少するような方形波の形状で光強度を変化させるようにレ 一ザダイオード 11を駆動する必要がない。その結果、相対的に緩やかに光強度が 増加し且つ相対的に緩やかに光強度が減少するような略正弦波の形状で光強度を 変化させるようにレーザダイオード 11を駆動すればよい。つまり、レーザドライブ回路 26は、パルス幅が相対的に短い(即ち、高速で且つ急激に ONZOFFする)方形波 の光ビームを照射するようにレーザダイオード 11を駆動する必要がなくなるため、レ 一ザダイオード 11を好適に駆動することができる。更に、レーザドライブ回路 26がレ 一ザダイオード 11を駆動することで発生する熱量を、相対的に減少させることができ る。  As described above, according to the first embodiment, the laser drive circuit 26 needs to drive the laser diode 11 so as to change the light intensity in the form of a strict square wave shown in FIG. 5 (a). It ’s gone. More specifically, the laser diode is changed so as to change the light intensity in the shape of a square wave in which the light intensity suddenly or instantaneously increases tl and the light intensity sharply or instantaneously decreases. There is no need to drive. As a result, the laser diode 11 may be driven so as to change the light intensity in a substantially sinusoidal shape in which the light intensity increases relatively slowly and the light intensity decreases relatively slowly. In other words, the laser drive circuit 26 does not need to drive the laser diode 11 so as to irradiate a square-wave light beam having a relatively short pulse width (that is, high-speed and suddenly ONZOFF). The diode 11 can be driven suitably. Furthermore, the amount of heat generated when the laser drive circuit 26 drives the laser diode 11 can be relatively reduced.
[0094] そして、厳密な方形波で光強度を変化させるようにレーザダイオード 11を駆動しな くとも、図 5 (c)に示す波形で透過量が変化するフィルタ 13を光ビームが透過すること で、厳密な方形波で光強度を変化させるようにレーザダイオード 11を駆動した場合と 同様の光ビームを、光ディスク 50に照射することができる。これにより、光ディスク 50 にデータを好適に記録することができる。  [0094] Even if the laser diode 11 is not driven so as to change the light intensity with a strict square wave, the light beam passes through the filter 13 whose transmission amount changes in the waveform shown in Fig. 5 (c). Thus, the optical disk 50 can be irradiated with the same light beam as when the laser diode 11 is driven so as to change the light intensity with a strict square wave. As a result, data can be suitably recorded on the optical disc 50.
[0095] カロえて、フィルタ 13を用いることにより、いわば光学的に光ビームの光強度を変化さ せることができるため、レーザドライブ回路 26により光ビームの光強度を変化させる場 合と比較して、光ビームの波形をより高精度に制御することができる。  [0095] By using the filter 13, it is possible to optically change the light intensity of the light beam, so compared with the case where the laser drive circuit 26 changes the light intensity of the light beam. The waveform of the light beam can be controlled with higher accuracy.
[0096] 更に、透過量が低 、状態から高!、状態への切り替え、或いは透過量が高!、状態か ら低 、状態への切り替えを、ピコ秒のオーダーで或!、はフェムト秒のオーダーで行う ことができるフィルタ 13を用いれば、将来の記録スピードの増加によっても、きわめて 短 、パルス幅を有する光ビームを、光ディスク 50に好適に照射することができる。  [0096] Furthermore, the transmission amount is low, the state is high !, the state is switched, or the transmission amount is high !, the state is low, the state is switched on the order of picoseconds or is femtoseconds. By using the filter 13 that can be ordered, the optical disk 50 can be suitably irradiated with a light beam having a pulse width that is extremely short even if the recording speed increases in the future.
[0097] エラー!ハイパーリンクの参照に誤りがあります。エラー!ハイパーリンクの参照に誤り があります。 更には、光学的に光ビームの光強度を変化させることができるため、図 6に示すような光ビームのオーバーシュートやアンダーシュートの発生をも抑制するこ とができる。このため、オーバーシュートないしはアンダーシュートを発生させる要因と なるレーザダイオード 11のパラメータのばらつきの許容範囲を相対的に拡大すること ができる。これにより、レーザダイオード 11の設計の幅 (例えば、材料の選択の幅等) を相対的に広げることができる。カロえて、光ディスク 50に照射される光ビームの波形と いう情報記録再生装置 1の特性の均一化を比較的容易に図ることができる。 [0097] Error! There is an error in the hyperlink reference. error! There is an error in the hyperlink reference. Furthermore, since the light intensity of the light beam can be optically changed, the occurrence of overshoot and undershoot of the light beam as shown in FIG. 6 can be suppressed. You can. For this reason, it is possible to relatively expand the permissible range of variations in the parameters of the laser diode 11 that cause overshoot or undershoot. This makes it possible to relatively widen the design width of the laser diode 11 (for example, the material selection width). In addition, the characteristics of the information recording / reproducing apparatus 1 such as the waveform of the light beam applied to the optical disc 50 can be made relatively easy.
[0098] これは特に、光ディスク 50に対するデータの記録スピードが増加する場合に、より 有効となる。つまり、光ディスク 50に対するデータの記録スピードが増加すれば、光ビ ームのパルス幅はどんどん短くなる力 光ビームの波形はフィルタ 13を用いて制御す ることができるため、レーザドライブ回路 26の負担はそれほど急激には増加しない。 従って、記録スピードの増加量によるパルス幅の減少量と比較して、レーザドライブ 回路 26の発熱量の増加量を抑制することができる。  This is more effective particularly when the data recording speed on the optical disc 50 is increased. In other words, if the recording speed of data on the optical disc 50 increases, the pulse width of the optical beam becomes shorter and shorter. The waveform of the optical beam can be controlled by using the filter 13, so that the burden of the laser drive circuit 26 is reduced. Does not increase so rapidly. Therefore, the amount of increase in the amount of heat generated by the laser drive circuit 26 can be suppressed as compared with the amount of decrease in the pulse width due to the increase in recording speed.
[0099] 尚、オーバーシュートやアンダーシュートが発生する場合には、ある一定パワー以 上で透過率が" 0"になる又はあるパワー以上でも透過率が" 0"になるフィルタを用い て、オーバーシュートやアンダーシュートを取り除くことが好ましい。このようなフィルタ として、光アンプや調光ガラス等を用いることができる。  [0099] When overshoot or undershoot occurs, a filter that has a transmittance of "0" above a certain power or a transmittance of "0" above a certain power is used. It is preferable to remove shoots and undershoots. As such a filter, an optical amplifier, a light control glass, or the like can be used.
[0100] 尚、上述の第 1実施例においては、レーザドライブ回路 26は、光強度が略正弦波 形状に変化する光ビームを照射するようにレーザダイオード 11を駆動しているが、均 一なな 、しは一定の光強度を有する光ビームを照射するようにレーザダイオード 11 を駆動しても、上述した各種利益を相応に享受することができる。言い換えれば、 DC レベルの光強度で光ビームを照射するようにレーザダイオード 11を駆動しても、上述 した各種利益を相応に享受することができる。  [0100] In the first embodiment described above, the laser drive circuit 26 drives the laser diode 11 so as to irradiate a light beam whose light intensity changes to a substantially sinusoidal shape. Even if the laser diode 11 is driven so as to irradiate a light beam having a constant light intensity, the above-mentioned various benefits can be enjoyed accordingly. In other words, even if the laser diode 11 is driven so as to irradiate the light beam with a DC level light intensity, the above-described various benefits can be enjoyed accordingly.
[0101] 尚、フィルタ 13を採用する場合、透過ないしは吸光される光ビームの他にフィルタ 1 3において反射される光ビームも発生し得る。この場合、光ビームの入射軸を法線と する角度にフィルタ 13を設置してしまうと、当該フィルタ 13上にて反射された光ビー ムが光軸上にて迷光する可能性がある。従って、フィルタ 13は、光ビームの入射軸に 対して所定の角度 Θをもって設置し、フィルタ 13において当該光軸上に反射光が発 生しな 、ようにすることが好まし!/、。  [0101] When the filter 13 is employed, a light beam reflected by the filter 13 can be generated in addition to the light beam transmitted or absorbed. In this case, if the filter 13 is installed at an angle with the incident axis of the light beam as a normal line, the light beam reflected on the filter 13 may stray on the optical axis. Therefore, it is preferable to install the filter 13 at a predetermined angle Θ with respect to the incident axis of the light beam so that no reflected light is generated on the optical axis in the filter 13! /.
[0102] 力!]えて、図 5 (b)に示す光ビームの光強度の変化における立ち上がり及び立ち下が りの位相(或いは、増減の傾向ないしは光ビームの ONZOFFのタイミング)と、図 5 ( c)に示すフィルタ 13の透過量の変化における立ち上がり及び立ち下がりの位相(或 いは、増減の傾向ないしはフィルタ 13の透過量変化における ONZOFFのタイミン グ)とを揃えるないしは一致させることが好ましい。この位相を揃えるないしは一致さ せる態様については、第 2実施例においてより詳細に説明する。 [0102] Power! The rise and fall of the change in the light intensity of the light beam shown in Fig. 5 (b) Phase (or increase / decrease tendency or ONZOFF timing of the light beam) and the rising and falling phases (or increase / decrease tendency or filter) of the change in the transmission amount of the filter 13 shown in FIG. It is preferable to align or match the ONZOFF timing of 13 transmission amount changes). A mode in which the phases are aligned or matched will be described in more detail in the second embodiment.
[0103] (2) 第 2実施例  [0103] (2) Second Example
続いて、図 7から図 9を参照して、第 2実施例に係る情報記録再生装置について説 明する。ここに、図 7は、第 2実施例に係る情報記録再生装置の基本構成を概念的に 示すブロック図であり、図 8は、フィルタ 13の透過量を変化させるタイミングをずらさな い場合の、レーザダイオード 11から照射される光ビームの光強度、フィルタ 13の透 過量、及び光ディスク 50に照射される光ビームの光強度の夫々の、時間軸に沿った 変化の様子を概念的に示すグラフであり、図 9は、フィルタ 13の透過量を変化させる タイミングをずらした場合の、レーザダイオード 11から照射される光ビームの光強度、 フィルタ 13の透過量、及び光ディスク 50に照射される光ビームの光強度の夫々の、 時間軸に沿った変化の様子を概念的に示すグラフである。  Subsequently, an information recording / reproducing apparatus according to the second embodiment will be described with reference to FIGS. FIG. 7 is a block diagram conceptually showing the basic structure of the information recording / reproducing apparatus in the second example. FIG. 8 is a diagram in the case where the timing for changing the transmission amount of the filter 13 is not shifted. A graph conceptually showing how the light intensity of the light beam emitted from the laser diode 11, the transmission amount of the filter 13, and the light intensity of the light beam emitted to the optical disc 50 change along the time axis. FIG. 9 shows the light intensity of the light beam irradiated from the laser diode 11, the transmission amount of the filter 13, and the light beam irradiated to the optical disc 50 when the timing of changing the transmission amount of the filter 13 is shifted. It is a graph which shows notionally how the light intensity changes along the time axis.
[0104] 尚、第 2実施例においては、第 1実施例と同様の構成については同一の参照符号 を付して、その詳細な説明につ 、ては省略する。  Note that in the second embodiment, the same components as those in the first embodiment are denoted by the same reference numerals, and detailed description thereof is omitted.
[0105] 図 7に示すように、第 2実施例に係る情報記録再生装置 2は、光ピックアップ 10aと、 フォトディテクタ(PD: Photo Detector)用アンプ 21と、再生回路 22と、 CPU24と、記 録回路 25と、レーザドライブ回路 26と、フィルタ素子ドライブ回路 27と、スピンドルモ ータ 28と、積分回路 31と、参照値格納回路 32と、コンパレータ 33と、位相補償サー ボ回路 34とを備える。  As shown in FIG. 7, the information recording / reproducing apparatus 2 according to the second embodiment includes an optical pickup 10a, a photo detector (PD) amplifier 21, a reproducing circuit 22, a CPU 24, and a recording device. A circuit 25, a laser drive circuit 26, a filter element drive circuit 27, a spindle motor 28, an integration circuit 31, a reference value storage circuit 32, a comparator 33, and a phase compensation servo circuit 34 are provided.
[0106] 第 2実施例に係る情報記録再生装置 2では、光ピックアップ 10aは、レーザダイォー ド 11と、フロントモニタ(FM : Front Monitor) 12と、フィルタ 13と、ビームスプリッタ 14 と、対物レンズ 15と、集光レンズ 16と、フォトディテクタ 17とを備えている。  In the information recording / reproducing apparatus 2 according to the second embodiment, the optical pickup 10a includes a laser diode 11, a front monitor (FM) 12, a filter 13, a beam splitter 14, and an objective lens 15. The condenser lens 16 and the photo detector 17 are provided.
[0107] フロントモニタ 12は、本発明の「モニタリング手段」の一具体例を構成しており、例え ば受光センサ等を備えており、レーザダイオード 11から照射される光ビームのパワー (即ち、光ビームの光強度値ないしはエネルギー量であって、受光センサ等における 受光量に応じた値)を測定可能に構成されている。測定されたパワーは、積分回路 3 1へ出力される。 The front monitor 12 constitutes a specific example of the “monitoring means” of the present invention. For example, the front monitor 12 includes a light receiving sensor and the like, and the power of the light beam emitted from the laser diode 11 (ie, light This is the light intensity value or energy amount of the beam. The value according to the amount of received light) can be measured. The measured power is output to the integrating circuit 31.
[0108] また、積分回路 31は、フロントモニタ 12において測定された光ビームのパワーを積 分可能に構成されている。積分回路 31において積分された光ビームのパワーは、光 ビームの光強度の DC成分を示しており、コンパレータ 33へ出力される。  Further, the integrating circuit 31 is configured to be able to integrate the power of the light beam measured by the front monitor 12. The power of the light beam integrated in the integration circuit 31 indicates a DC component of the light intensity of the light beam and is output to the comparator 33.
[0109] 参照値格納回路 32は、積分回路において積分される光ビームのパワーとの比較の 際に参照される参照値を、コンパレータ 33に出力可能に構成されている。参照値の 具体例としては、 "0"又は光ビームの光強度の最大値を示す" Vmax"が格納されて おり、これらの参照値をコンパレータ 33へ出力する。  [0109] The reference value storage circuit 32 is configured to be able to output to the comparator 33 a reference value that is referred to when compared with the power of the light beam integrated in the integrating circuit. As a specific example of the reference value, “0” or “Vmax” indicating the maximum value of the light intensity of the light beam is stored, and these reference values are output to the comparator 33.
[0110] コンパレータ 33は、積分回路 31から出力される光ビームのパワーの積分値と、参 照値格納回路 32から出力される参照値を比較し、該比較結果を位相補償サーボ回 路 34に出力する。  The comparator 33 compares the integrated value of the power of the light beam output from the integration circuit 31 with the reference value output from the reference value storage circuit 32, and the comparison result is input to the phase compensation servo circuit 34. Output.
[0111] より具体的には、時刻 tにおける光ビームの光強度の DC成分 (即ち、光ビームの光 強度の積分値)を V(t)とすると、 V (t+ A t) -V (t)が、参照値である" 0"又は" Vma X"と一致するか否かが比較される。そして、一致するか否かを示す比較結果が位相 補償サーボ回路 34へ出力される。この倍、参照値と光ビームの光強度の積分値も、 位相補償サーボ回路 34へ出力されるように構成してもよい。  [0111] More specifically, if the DC component of the light intensity of the light beam at time t (that is, the integrated value of the light intensity of the light beam) is V (t), then V (t + At +) -V (t ) Is compared with the reference value “0” or “Vma X”. Then, a comparison result indicating whether or not they match is output to the phase compensation servo circuit 34. This double, the integrated value of the reference value and the light intensity of the light beam may be configured to be output to the phase compensation servo circuit 34.
[0112] 位相補償サーボ回路 34は、コンパレータ 33における比較結果に基づいて、フィル タ 13の透過量を変化させるタイミング (ないしは、位相)を調整する。より具体的には、 V (t+ A t) -V (t)力 参照値である" 0"又は" Vmax"と一致していれば、フィルタ 13 の透過量を変化させるタイミングを変化させない。他方、 V(t+ A t) -V (t)が、参照 値である" 0"又は" Vmax"と一致していなければ、 V (t+ A t)— V(t)力 参照値で ある" 0"又は" Vmax"と一致するように、フィルタ 13の透過量を変化させるタイミング を変化させる。フィルタ 13の透過量を変化させるタイミングの変化は、 V (t+ A t) -V (t)力 参照値である" 0"又は" Vmax"とどれだけ誤差を有しているかに応じて行うこ とが好ましい。  The phase compensation servo circuit 34 adjusts the timing (or phase) for changing the transmission amount of the filter 13 based on the comparison result in the comparator 33. More specifically, if the V (t + A t) -V (t) force matches the reference value “0” or “Vmax”, the timing for changing the transmission amount of the filter 13 is not changed. On the other hand, if V (t + At) -V (t) does not match the reference value "0" or "Vmax", V (t + At) — V (t) force reference value " The timing for changing the transmission amount of the filter 13 is changed so as to coincide with “0” or “Vmax”. The change in the timing of changing the amount of transmission of the filter 13 depends on how much difference there is between the V (t + At) -V (t) force reference value "0" or "Vmax". And are preferred.
[0113] このように、第 2実施例に係る情報記録再生装置 2によれば、光ビームの光強度の 変化における立ち上がり及び立ち下がりの位相(或いは、増減の傾向ないしは光ビ ームの ONZOFFのタイミング)と、フィルタ 13の透過量の変化における立ち上がり 及び立ち下がりの位相(或いは、増減の傾向ないしはフィルタ 13の透過量変化にお ける ON/OFFのタイミング)とを撤えるな!/ヽしは一致させることができる。 As described above, according to the information recording / reproducing apparatus 2 in the second example, the rising and falling phases (or the tendency of increase / decrease or the optical beam in the change of the light intensity of the light beam). ONZOFF timing) and the rising and falling phases of the change in the transmission amount of the filter 13 (or the tendency of increase / decrease or the ON / OFF timing of the change in the transmission amount of the filter 13). ! / Thanks can be matched.
[0114] 仮に、第 2実施例の如くフィルタ 13の透過量を変化させるタイミングを変化させなけ れば、図 8 (a)に示すように、光ビームの光強度の変化における立ち上がり及び立ち 下がりの位相と、フィルタ 13の透過量の変化における立ち上がり及び立ち下がりの位 相とがずれてしまう場合が生じ得る。この場合、光ディスク 50に実際に照射される光 ビームの光強度は、図 8 (b)に示すように、方形波の一部が欠けた不適切な波形で 変化することになる。 [0114] If the timing for changing the transmission amount of the filter 13 is not changed as in the second embodiment, as shown in FIG. 8 (a), the rise and fall of the change in the light intensity of the light beam is suppressed. There may be a case where the phase and the rising and falling phases in the change in the transmission amount of the filter 13 are shifted. In this case, the light intensity of the light beam actually irradiated onto the optical disc 50 changes with an inappropriate waveform lacking a part of the square wave as shown in FIG. 8 (b).
[0115] しかるに、第 2実施例によれば、フィルタ 13の透過量を変化させるタイミングを変化 させることで、図 9 (a)に示すように、光ビームの光強度の変化における立ち上がり及 び立ち下がりの位相と、フィルタ 13の透過量の変化における立ち上がり及び立ち下 力 Sりの位相とを揃えるないしは一致させることができる。その結果、光ディスク 50に実 際に照射される光ビームの光強度は、図 9 (b)に示すように、適切な方形波形状で変 化する。これにより、第 2実施例に係る情報記録再生装置 2によれば、上述した各種 利益を享受することにカ卩えて、光ディスク 50へのデータの記録の信頼性を相対的に 高めることができる。  [0115] However, according to the second embodiment, by changing the timing of changing the transmission amount of the filter 13, as shown in Fig. 9 (a), the rise and rise in the change in the light intensity of the light beam. The falling phase and the phase of the rising and falling force S in the change in the transmission amount of the filter 13 can be aligned or matched. As a result, the light intensity of the light beam actually irradiated onto the optical disc 50 changes in an appropriate square wave shape as shown in FIG. 9 (b). As a result, according to the information recording / reproducing apparatus 2 in the second embodiment, the reliability of data recording on the optical disc 50 can be relatively improved in consideration of the above-described various benefits.
[0116] 更に、本実施例に力かる情報記録再生装置 2においては、 CPU24やレーザドライ ブ回路 26やフィルタ素子ドライブ回路 27や積分回路 31や参照値格納回路 32ゃコ ンパレータ 33や位相補償サーボ回路 34等を、光ピックアップ 10と別体の装置により 構成した例について説明した力 これらは光ピックアップ 10と一体的に構成するよう に、更にはレーザダイオード 11に含めるように構成しても良 、ことは言うまでもな 、。  [0116] Furthermore, in the information recording / reproducing apparatus 2 that is useful in this embodiment, the CPU 24, the laser drive circuit 26, the filter element drive circuit 27, the integration circuit 31, the reference value storage circuit 32, the comparator 33, and the phase compensation servo The force described in the example in which the circuit 34 and the like are configured by a device separate from the optical pickup 10 may be configured so as to be integrated with the optical pickup 10 and further included in the laser diode 11. Needless to say.
[0117] 上述の実施例では、情報記録媒体の一例として光ディスク 50及び情報記録装置 若しくは情報再生装置の一例として光ディスク 50に係るレコーダ若しくはプレーヤに ついて説明したが、本発明は、光ディスク及びそのレコーダ若しくはプレーヤに限ら れるものではなぐ他の高密度記録或いは高転送レート対応の各種情報記録媒体並 びにそのレコーダ若しくはプレーヤにも適用可能である。  In the above-described embodiment, the optical disc 50 and the recorder or player related to the optical disc 50 as an example of the information recording device or the information reproducing device have been described as an example of the information recording medium. The present invention is not limited to a player, and can be applied to other high-density recording or various information recording media compatible with a high transfer rate, as well as the recorder or player.
[0118] 本発明は、上述した実施例に限られるものではなぐ請求の範囲及び明細書全体 力 読み取れる発明の要旨或いは思想に反しない範囲で適宜変更可能であり、その ような変更を伴なう光ピックアップ装置、照射方法、情報記録装置及び情報再生装置 、並びにコンピュータプログラムもまた本発明の技術的範囲に含まれるものである。 産業上の利用可能性 [0118] The present invention is not limited to the embodiments described above, but the entire claims and specification. The optical pickup device, the irradiation method, the information recording device, the information reproducing device, and the computer program that can be changed as appropriate without departing from the gist or idea of the invention that can be read. It is included in the scope. Industrial applicability
本発明に係る光ピックアップ装置、照射方法、情報記録装置及び情報再生装置、 並びにコンピュータプログラムは、例えば光ディスク等の情報記録媒体に対するデー タの記録及び再生に用いる光ピックアップ装置に利用可能であり、該光ピックアップ 装置を備える情報記録装置及び情報再生装置に利用可能である。また、例えば民 生用或いは業務用の各種コンピュータ機器に搭載される又は各種コンピュータ機器 に接続可能な情報記録装置及び情報再生装置等にも利用可能である。  The optical pickup device, the irradiation method, the information recording device and the information reproducing device, and the computer program according to the present invention can be used for an optical pickup device used for recording and reproducing data on an information recording medium such as an optical disk. The present invention can be used for an information recording device and an information reproducing device including an optical pickup device. Further, the present invention can also be used for information recording devices and information reproducing devices that are mounted on or connectable to various computer devices for consumer use or business use.

Claims

請求の範囲 The scope of the claims
[1] 情報記録媒体の記録面に出射光を照射する光源と、  [1] a light source that emits emitted light onto a recording surface of an information recording medium;
前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御手段と、  Light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape;
前記出射光の光路上に配置され、入射される前記出射光の透過量を変更するフィ ノレタと、  A finer disposed on the optical path of the outgoing light and changing a transmission amount of the outgoing outgoing light;
前記出射光の透過量を変更するように前記フィルタを制御するフィルタ制御手段と を備えることを特徴とする光ピックアップ装置。  An optical pickup device comprising: filter control means for controlling the filter so as to change a transmission amount of the emitted light.
[2] 前記フィルタ制御手段は、前記情報記録媒体に記録されるデータに応じて前記フ ィルタの透過量を変更するように前記フィルタを制御することを特徴とする請求の範 囲第 1項に記載の光ピックアップ装置。  [2] The filter according to claim 1, wherein the filter control means controls the filter so as to change a transmission amount of the filter according to data recorded on the information recording medium. The optical pickup device described.
[3] 前記フィルタ制御手段は、前記情報記録媒体に記録されるデータに応じたストラテ ジパルスに応じて前記フィルタの透過量を変更するように前記フィルタを制御すること を特徴とする請求の範囲第 1項に記載の光ピックアップ装置。 [3] The filter control means controls the filter so as to change a transmission amount of the filter in accordance with a strategy pulse corresponding to data recorded in the information recording medium. The optical pickup device according to item 1.
[4] 前記ストラテジパルスは、所定の第 1振幅を有する第 1パルスと前記第 1振幅よりも 小さい第 2振幅を有する第 2パルスとを少なくとも含んでおり、 [4] The strategy pulse includes at least a first pulse having a predetermined first amplitude and a second pulse having a second amplitude smaller than the first amplitude,
前記フィルタ制御手段は、前記第 1パルスに応じた前記フィルタの透過量が、前記 第 2パルスに応じた前記フィルタの透過量よりも増加するように前記フィルタを制御す ることを特徴とする請求の範囲第 3項に記載の光ピックアップ装置。  The filter control means controls the filter so that a transmission amount of the filter according to the first pulse is larger than a transmission amount of the filter according to the second pulse. 4. An optical pickup device according to claim 3,
[5] 前記光強度制御手段は、前記情報記録媒体に記録されるデータに応じて前記出 射光の光強度を変化させるように前記光源を制御することを特徴とする請求の範囲 第 1項に記載の光ピックアップ装置。 5. The light intensity control means controls the light source so as to change the light intensity of the emitted light according to data recorded on the information recording medium. The optical pickup device described.
[6] 前記光強度制御手段は、前記情報記録媒体に記録されるデータに応じたストラテ ジパルスに応じて前記出射光の光強度を変化させるように前記光源を制御すること を特徴とする請求の範囲第 1項に記載の光ピックアップ装置。 6. The light intensity control means controls the light source so as to change the light intensity of the emitted light according to a strategy pulse corresponding to data recorded on the information recording medium. The optical pickup device according to item 1 of the range.
[7] 前記ストラテジパルスは、所定の第 1振幅を有する第 1パルスと前記第 1振幅よりも 小さい第 2振幅を有する第 2パルスとを少なくとも含んでおり、 [7] The strategy pulse includes at least a first pulse having a predetermined first amplitude and a second pulse having a second amplitude smaller than the first amplitude,
前記光強度制御手段は、前記第 1パルスに応じた前記出射光の光強度が、前記第 2パルスに応じた前記出射光の光強度よりも大きくなるように前記光源を制御すること を特徴とする請求の範囲第 6項に記載の光ピックアップ装置。 The light intensity control means is configured such that the light intensity of the emitted light according to the first pulse is the first pulse. 7. The optical pickup device according to claim 6, wherein the light source is controlled to be greater than the light intensity of the emitted light corresponding to two pulses.
[8] 前記出射光の光強度の増減における立ち上がり及び立ち下がりの夫々の位相と、 前記フィルタの透過量の変更における立ち上がり及び立ち下がりの夫々の位相とを 同期させる同期手段を更に備えることを特徴とする請求の範囲第 1項に記載の光ピッ クアップ装置。 [8] The apparatus further comprises synchronization means for synchronizing each phase of rising and falling when the light intensity of the emitted light is increased and decreased and each phase of rising and falling when the transmission amount of the filter is changed. The optical pick-up device according to claim 1.
[9] 前記フィルタを透過した前記出射光の光強度をモニタリングするモニタリング手段を 更に備え、  [9] It further comprises monitoring means for monitoring the light intensity of the emitted light that has passed through the filter,
前記同期手段は、モニタリングされた光強度の積分値と所定の基準値とを比較する ことで、前記位相を同期させることを特徴とする請求の範囲第 8項に記載の光ピックァ ップ装置。  9. The optical pick-up device according to claim 8, wherein the synchronization unit synchronizes the phase by comparing an integrated value of the monitored light intensity with a predetermined reference value.
[10] 時間 tにおける前記出射光の光強度の積分値を V (t)とすると、前記同期手段は、 V  [10] When the integrated value of the light intensity of the emitted light at time t is V (t), the synchronization means
(t+ A t)— V(t)が 0又は最大値をとるように前記位相を同期させることを特徴とする 請求の範囲第 9項に記載の光ピックアップ装置。  10. The optical pickup device according to claim 9, wherein the phases are synchronized so that (t + At) —V (t) takes 0 or a maximum value.
[11] 前記フィルタは、 [11] The filter is
印加される電圧の値により吸収波長が変化する吸光層と、  A light-absorbing layer whose absorption wavelength varies depending on the value of the applied voltage;
前記吸光層に対して前記電圧を印加する電極と  An electrode for applying the voltage to the light absorption layer;
を備えており、  With
前記フィルタ制御手段は、前記電極に対して印加する前記電圧の値を変更するこ とで、前記フィルタの透過量を変更するように前記フィルタを制御することを特徴とす る請求の範囲第 1項に記載の光ピックアップ装置。  The filter control means controls the filter so as to change a transmission amount of the filter by changing a value of the voltage applied to the electrode. The optical pickup device according to Item.
[12] 前記フィルタは、 [12] The filter is
印加される電圧の値により分子配列が変化する液晶素子を含む液晶層と、 前記液晶層に対して前記電圧を印加する電極と  A liquid crystal layer including a liquid crystal element whose molecular arrangement changes according to the value of the applied voltage; an electrode for applying the voltage to the liquid crystal layer;
を備えており、  With
前記フィルタ制御手段は、前記電極に対して印加する前記電圧の値を変更するこ とで、前記フィルタの透過量を変更するように前記フィルタを制御することを特徴とす る請求の範囲第 1項に記載の光ピックアップ装置。 The filter control means controls the filter so as to change a transmission amount of the filter by changing a value of the voltage applied to the electrode. The optical pickup device according to Item.
[13] 前記フィルタは、前記出射光の光路に対して予め定められた角度を持って配置さ れていることを特徴とする請求の範囲第 1項に記載の光ピックアップ装置。 13. The optical pickup device according to claim 1, wherein the filter is disposed with a predetermined angle with respect to the optical path of the emitted light.
[14] 情報記録媒体の記録面に出射光を照射する光源と、前記出射光の光路上に配置 され、入射される前記出射光の透過量を変更するフィルタとを備える光ピックアップ装 置における前記出射光の照射方法であって、 [14] The optical pickup apparatus comprising: a light source that emits outgoing light onto a recording surface of an information recording medium; and a filter that is disposed on an optical path of the outgoing light and that changes a transmission amount of the incident outgoing light. A method of irradiating emitted light,
前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御工程と、  A light intensity control step of controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape;
前記出射光の透過量を変更するように前記フィルタを制御するフィルタ制御工程と を備えることを特徴とする照射方法。  A filter control step of controlling the filter so as to change a transmission amount of the emitted light.
[15] 情報記録媒体の記録面に出射光を照射する光源と、 [15] a light source for irradiating the recording surface of the information recording medium with emitted light;
前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御手段と、  Light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape;
前記出射光の光路上に配置され、入射される前記出射光の透過量を変更するフィ ノレタと、  A finer disposed on the optical path of the outgoing light and changing a transmission amount of the outgoing outgoing light;
前記出射光の透過量を変更するように前記フィルタを制御するフィルタ制御手段と 前記情報記録媒体にデータを記録する記録手段と  Filter control means for controlling the filter so as to change the transmission amount of the emitted light; and recording means for recording data on the information recording medium;
を備えることを特徴とする情報記録装置。  An information recording apparatus comprising:
[16] 情報記録媒体の記録面に出射光を照射する光源と、 [16] a light source for irradiating the recording surface of the information recording medium with emitted light;
前記出射光の光強度を略正弦波形状に変化させるように前記光源を制御する光強 度制御手段と、  Light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sinusoidal shape;
前記出射光の光路上に配置され、入射される前記出射光の透過量を変更するフィ ノレタと、  A finer disposed on the optical path of the outgoing light and changing a transmission amount of the outgoing outgoing light;
前記出射光の透過量を変更するように前記フィルタを制御するフィルタ制御手段と 前記情報記録媒体に記録されたデータを再生する再生手段と  Filter control means for controlling the filter so as to change the transmission amount of the emitted light; and reproduction means for reproducing data recorded on the information recording medium;
を備えることを特徴とする情報再生装置。  An information reproducing apparatus comprising:
[17] 情報記録媒体の記録面に出射光を照射する光源と、前記出射光の光強度を略正 弦波形状に変化させるように前記光源を制御する光強度制御手段と、前記出射光の 光路上に配置され、入射される前記出射光の透過量を変更するフィルタと、前記出 射光の透過量を変更するように前記フィルタを制御するフィルタ制御手段と、前記情 報記録媒体にデータを記録する記録手段とを備える情報記録装置に備えられたコン ピュータを制御する記録制御用のコンピュータプログラムであって、該コンピュータを[17] A light source that irradiates the recording surface of the information recording medium with the emitted light, and the light intensity of the emitted light is substantially positive. Light intensity control means for controlling the light source so as to change it into a chord wave shape, a filter disposed on the optical path of the outgoing light and for changing the transmission amount of the incident outgoing light, and the transmission amount of the outgoing light A computer program for recording control for controlling a computer provided in an information recording apparatus comprising filter control means for controlling the filter so as to change data and recording means for recording data on the information recording medium. The computer
、前記光強度制御手段及び前記フィルタ制御手段の少なくとも一部として機能させる ことを特徴とするコンピュータプログラム。 A computer program that functions as at least part of the light intensity control means and the filter control means.
情報記録媒体の記録面に出射光を照射する光源と、前記出射光の光強度を略正 弦波形状に変化させるように前記光源を制御する光強度制御手段と、前記出射光の 光路上に配置され、入射される前記出射光の透過量を変更するフィルタと、前記出 射光の透過量を変更するように前記フィルタを制御するフィルタ制御手段と、前記情 報記録媒体に記録されたデータを再生する再生手段とを備える情報再生装置に備 えられたコンピュータを制御する再生制御用のコンピュータプログラムであって、該コ ンピュータを、前記光強度制御手段及び前記フィルタ制御手段の少なくとも一部とし て機能させることを特徴とするコンピュータプログラム。  A light source for irradiating the recording surface of the information recording medium with the emitted light, a light intensity control means for controlling the light source so as to change the light intensity of the emitted light into a substantially sine wave shape, and an optical path of the emitted light A filter that is arranged and changes the transmission amount of the emitted light that is incident, filter control means that controls the filter so as to change the transmission amount of the emitted light, and data recorded on the information recording medium. A computer program for reproduction control for controlling a computer provided in an information reproduction apparatus comprising reproduction means for reproducing, wherein the computer is used as at least part of the light intensity control means and the filter control means. A computer program characterized by functioning.
PCT/JP2006/321718 2005-10-31 2006-10-31 Optical pickup device, irradiating method, information recording device and information reproducing device, and computer program WO2007052639A1 (en)

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Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS647327A (en) * 1987-03-25 1989-01-11 Casio Computer Co Ltd Method and apparatus for optical information recording
JPH0817065A (en) * 1994-06-30 1996-01-19 Sony Corp Optical pickup device
JP2002260272A (en) * 2001-02-28 2002-09-13 Sony Corp Optical head, recording/reproducing device, and variable optical coupling element
JP2004220744A (en) * 2003-01-17 2004-08-05 Sony Corp Optical head and optical recording medium driving device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS647327A (en) * 1987-03-25 1989-01-11 Casio Computer Co Ltd Method and apparatus for optical information recording
JPH0817065A (en) * 1994-06-30 1996-01-19 Sony Corp Optical pickup device
JP2002260272A (en) * 2001-02-28 2002-09-13 Sony Corp Optical head, recording/reproducing device, and variable optical coupling element
JP2004220744A (en) * 2003-01-17 2004-08-05 Sony Corp Optical head and optical recording medium driving device

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