JP5072567B2 - Optical pickup device - Google Patents

Description

  The present invention relates to an optical pickup apparatus that performs an operation of reading a signal recorded on an optical disc and an operation of recording a signal on an optical disc.

  2. Description of the Related Art Optical disc apparatuses that can perform signal reading operations and signal recording operations by irradiating a signal recording layer of an optical disc with laser light emitted from an optical pickup device have become widespread.

  As an optical disk apparatus, an apparatus using an optical disk called CD or DVD has been widely used, but recently, an optical disk with improved recording density, that is, a Blu-ray standard or an HD DVD (High Density Digital Versatile Disk) standard. Those using optical discs have been developed.

  As a laser beam for performing an operation of reading a signal recorded on a CD standard optical disk, an infrared light having a wavelength of 780 nm is used, and a laser beam for performing an operation of reading a signal recorded on a DVD standard optical disk. In this case, red light having a wavelength of 650 nm is used.

  The protective layer provided on the upper surface of the signal recording layer in the CD standard optical disc has a thickness of 1.2 mm, and an aperture of an objective lens used for reading a signal from the signal recording layer. The number is defined as 0.45. Also, the thickness of the protective layer provided on the upper surface of the signal recording layer in the DVD standard optical disc is 0.6 mm, and the numerical aperture of the objective lens used for reading signals from the signal recording layer Is defined as 0.6.

  As a laser beam for performing an operation of reading a signal recorded on an optical disc of the Blu-ray standard or the HD DVD standard with respect to the optical disc of the CD standard and the DVD standard, a laser beam having a short wavelength, for example, a wavelength of 405 nm Blue-violet light is used.

  The thickness of the protective layer provided on the upper surface of the signal recording layer in the HD DVD standard optical disc is 0.6 mm, and the numerical aperture of the objective lens used for reading signals from the signal recording layer Is defined as 0.65.

As described above, optical discs with different standards have different wavelengths of laser light for reading signals. Therefore, laser diodes that emit laser beams of different wavelengths are used to read signals from all optical discs. It is configured as follows. (See Patent Document 1)
Further, in order to perform the reading operation of the signals recorded on all the optical discs, the position of the recording layer of the signal is different, so it is necessary to switch the numerical aperture corresponding to each optical disc. Optical pickup devices that can be used have been developed. (See Patent Document 2)
JP 2004-295983 A JP 2006-172605 A

  When reading signals recorded on optical discs of different standards, laser diodes that emit laser light of a wavelength corresponding to each optical disc and means for setting the numerical aperture of the objective lens in correspondence with each optical disc In addition to the necessity, it is necessary to provide an optical component for each optical disk, so that there is a problem that not only the configuration is complicated, but also the manufacturing cost is expensive.

  The present invention is intended to provide an optical pickup device that can solve such a problem.

The present invention includes a laser diode that emits laser light of a first wavelength, an objective lens that focuses the laser light emitted from the laser diode onto a signal recording layer provided on an optical disc, and the laser diode and objective lens. Spherical aberration correction means provided in the optical path between the first optical disk and the second optical disk having different standards in the same optical system by performing spherical aberration correction operation by the spherical aberration correction means. A photodetector for performing a reading operation of a recorded signal and irradiating a return light which is a laser beam of a first wavelength reflected from a signal recording layer of each optical disc of the first optical disc and the second optical disc; a push-pull signal for each optical disc performs the tracking control operation obtained from the photodetector, defined in the second optical disk The depth d of the groove formed in the signal recording layer with respect to the wavelength of the laser light to be generated is d = λ / 4n (where λ is the wavelength of the laser light defined on the second optical disc, and n is the wavelength of the second optical disc) The second optical disk having the optical disk of a type set so as to have a relationship of the refractive index of the protective layer covering the signal recording layer is read using a laser beam having a wavelength defined for the first optical disk. , for the second optical disc is characterized in that to obtain a push-pull signal at a defined wavelength and the wavelength determined in the first optical disk different laser beam.

The present invention also performs Thus spherical aberration correction operation to the position adjustment operation of the collimating lens, to adjust the focusing position of the objective lens, suitable for signal reading operation to the signal recording layer provided on the optical disc This is characterized in that a spot is generated.

  The optical pickup device of the present invention is not only capable of reading signals recorded on a plurality of optical discs having different standards with laser light emitted from one laser diode, but also with the same optical Since the system is used to read signals from all the optical discs, the configuration is simplified and it can be manufactured at low cost.

In particular , the optical pickup device of the present invention includes a photodetector that is irradiated with return light that is laser light having a first wavelength reflected from the signal recording layer of each optical disc of the first optical disc and the second optical disc. A push-pull signal for the optical disk is obtained from the photodetector and the tracking control operation is performed. For the second optical disk, the push-pull signal is obtained with a laser beam having a wavelength different from the specified wavelength. Therefore, the groove depth d in the standard of the second optical disk is a value of λ / 4n (where λ is the wavelength of the laser beam specified for use in reading the signal of the second optical disk, and n is the protection of the second optical disk) Even in the case of an optical disc corresponding to the refractive index of the layer, a push-pull signal can be obtained from the photodetector and each optical data of the first optical disc and the second optical disc can be obtained. Line to give a tracking control operation by the push-pull signal to the disk, the circuit is usable optical pitch of the circuit configuration to perform simple tracking control operation
Ru can provide up equipment.

  1 and 2 are schematic views showing an embodiment of the optical pickup device of the present invention, FIG. 3 is a block circuit diagram for generating a tracking error signal, and FIG. 4 is a block circuit diagram for generating a focus error signal and a reproduction signal. is there.

  In this embodiment, a case will be described in which an HD DVD standard optical disk is used as the first optical disk, a DVD standard optical disk is used as the second optical disk, and a CD standard optical disk is used as the third optical disk.

  In FIG. 1, reference numeral 1 denotes a laser diode that emits a laser beam having a wavelength suitable for reading operation of a signal recorded on the first optical disc, for example, 405 nm of blue-violet light, and 2 denotes a laser emitted from the laser diode 1. A diffraction grating on which light is incident, a diffraction grating part 2a that separates laser light into 0th-order light, + 1st-order light, and -1st-order light, and an incident laser light that is converted into linearly polarized light in the S direction. It comprises a two-wave plate 2b.

  Reference numeral 3 denotes a polarization beam splitter on which the laser light transmitted through the diffraction grating 2 is incident, and a control film 3a for reflecting the S-polarized laser light and transmitting the laser light polarized in the P direction is provided. . Reference numeral 4 denotes a monitor photodetector provided at a position to which the laser beam transmitted through the control film 3a of the polarization beam splitter 3 in the laser beam emitted from the laser diode 1 is irradiated. Is used to control the output of the laser light emitted from the laser diode 1.

  A quarter wave plate 5 is provided at a position where the laser beam reflected by the control film 3a of the polarization beam splitter 3 is incident. The incident laser beam is changed from linearly polarized light to circularly polarized light. It has the function of converting. Reference numeral 6 denotes a collimating lens to which the laser light transmitted through the quarter-wave plate 5 is incident. The collimating lens 6 emits the incident laser light as parallel light or divergent light, and the collimating lens driving coil 7 performs the optical axis direction. That is, it is configured to be displaced in the directions of arrows A and B. The collimating lens 6 is displaced in the optical axis direction to correct spherical aberration due to the protective layer of the optical disc D and to adjust the condensing position of the laser beam by the objective lens described later.

  When the optical disc D is the first optical disc and the second optical disc, the signal recording layers L1 and L2 of each optical disc are at positions indicated by solid lines, and when the optical disc D is the third optical disc, the signal recording layer L3 is at positions indicated by broken lines. So that it is standardized.

  Reference numeral 8 denotes a reflection mirror that receives the laser light converted into parallel light by the collimator lens 6 and reflects the laser light, and is reflected from the signal recording layers L1, L2, and L3 of the optical disc D as described later. The return light is incident and the return light is reflected in the direction of the polarization beam splitter 3.

  Reference numeral 9 denotes an objective lens that receives the laser beam reflected by the reflection mirror 8 and condenses the laser beam on the signal recording layers L1, L2, and L3 of the optical disc D, and has a numerical aperture of the first optical disc. The standard is set to 0.65.

Reference numeral 10 denotes a sensor lens to which the return light transmitted through the control film 3a provided in the polarizing beam splitter 3 is incident. Cylindrical surfaces, flat surfaces, concave curved surfaces, or convex curved surfaces are formed on the incident surface side and the output surface side. Has been. The sensor lens 10 is configured to generate a focus error signal used for the focus control operation by generating astigmatism in the return light. Reference numeral 11 denotes a photodetector provided at a position where the return light that has passed through the sensor lens 10 is collected and irradiated, and is constituted by a quadrant sensor or the like in which photodiodes are arranged as will be described later. Yes.

  A focusing coil 12 performs a focusing operation of laser light by displacing the objective lens 9 in a direction perpendicular to the signal surface of the optical disc D, and a tracking coil 13 displaces the objective lens 9 in the radial direction of the optical disc D. It is.

  Reference numeral 14 denotes a light detection signal generation circuit for generating a tracking error signal, a focus error signal, and a reproduction signal read from the optical disk D based on the signal obtained from the light detector 11, and a specific example thereof is shown in FIGS. The description will be given with reference.

  First, a tracking error signal generation circuit that generates a tracking error signal will be described with reference to FIG. As shown in FIG. 3, the light receiving unit incorporated in the photodetector 11 has a four-divided sensor unit 11a irradiated with the main beam M and two-divided sensor units 11b and 11c irradiated with the sub beams S1 and S2, respectively. Is provided. The quadrant sensor unit 11a is composed of sensors A, B, C, and D as shown, and the bipartite sensor units 11b and 11c are composed of sensors E and F and sensors G and H, respectively. ing.

  In such a configuration, if the spot position of the laser beam deviates in the radial direction of the optical disc D with respect to the signal tracks provided on the signal recording layers L1, L2, and L3 of the optical disc D, that is, if tracking is deviated, 4 The position of the main beam M and the positions of the sub beams S1 and S2 generated on the split sensor unit 11a and the split sensor units 11b and 11c move in the direction of the arrow C or D, and as a result, the amount of light received by each sensor. Will change.

  The circuit diagram shown in FIG. 3 is for performing a tracking control operation called a differential push-pull method. In the figure, reference numeral 15 denotes a first adder for adding signals obtained from sensors A and D constituting the four-divided sensor unit 11a irradiated with the main beam M, and reference numeral 16 denotes a sensor B which is also irradiated with the main beam M. A second adder that adds signals obtained from C, a first subtractor 17 that subtracts an output signal of the second adder 16 from an output signal of the first adder 15, and a sub beam S1 that is irradiated 2 A second subtractor 19 subtracts the signal obtained from the sensor F from the signal obtained from the sensor E constituting the divided sensor unit 11b, and 19 is a signal obtained from the sensor G irradiated with the sub beam S2 constituting the two-divided sensor unit 11c. It is the 3rd subtracter which subtracts the signal obtained from the sensor H from.

  Reference numeral 20 denotes a third adder for adding the output signal of the second subtractor 18 and the output signal of the third subtracter 19, and 21 denotes the output signal of the third adder 20 by K times (K is the main beam M). An amplification circuit 22 for subtracting the output signal of the amplification circuit 21 from the output signal of the first subtractor 17. The output signal is output to the output terminal 23 as a tracking error signal.

  When the signals obtained from the sensors A, B, C, D, E, F, G, and H are A, B, C, D, E, F, G, and H, and the tracking error signal is TE, the tracking error is obtained. The signal TE is calculated from TE = (A + D) − (B + C) −K {(E−F) + (G−H)}. The tracking error signal TE is obtained from the circuit shown in FIG. I can do it. Such a tracking control operation by the differential push-pull method is generally known, and the details thereof are omitted.

  As described above, the tracking error signal TE generation circuit incorporated in the photodetection signal generation circuit 14 is configured. Next, the generation operation of the focus error signal FE and the reproduction signal RF will be described with reference to FIG. explain.

  First, the generation operation of the focus error signal FE will be described. The generation operation of the focus error signal FE using the astigmatism method is such that the shape of the main beam M generated and irradiated on the four-divided sensor unit 11a when the focus shift occurs in the focusing operation by the objective lens 9 is well known. The change to an elliptical shape is used.

  In FIG. 4, reference numeral 24 denotes a fourth adder that adds signals obtained from the sensors A and C constituting the four-divided sensor unit 11 a irradiated with the main beam M, and reference numeral 25 denotes a sensor B that is also irradiated with the main beam M. A fifth adder for adding the signal obtained from D, and 26 is a fifth subtracter for subtracting the output signal of the fifth adder 25 from the output signal of the fourth adder 24. The output signal is a focus error signal. It is output to the output terminal 27 as FE. In this way, the focus error signal FE by the astigmatism method is generated, but such an operation is generally known, and details thereof will be omitted.

  As described above, the generation operation of the focus error signal FE is performed, but the generation operation of the reproduction signal is performed as follows. That is, in FIG. 4, 28 is a sixth adder for adding the output signal of the fourth adder 24 and the output signal of the fifth adder 25, and the output signal is output to the output terminal 29 as the reproduction signal RF. Is done. That is, the reproduction signal of the signal recorded on the optical disc D is obtained by adding the signals obtained from all the sensors A, B, C, and D constituting the quadrant sensor unit 11a irradiated with the main beam M. Will be.

  The photodetection signal generation circuit 14 shown in FIG. 1 is configured by the circuits shown in FIGS. 3 and 4 as described above, and the tracking error signal TE, the focus error signal FE, and the reproduction generated from each circuit. A signal RF is output from each output terminal 23, 27 and 29.

  A pickup control circuit 30 controls the operation of the optical pickup device based on a signal output from the light detection signal generation circuit 14 and a signal output from a control circuit (not shown) incorporated in the optical disc apparatus. Reference numeral 31 denotes a tracking coil drive circuit to which a tracking control signal output from the pickup control circuit 30 is applied, and is configured to supply a drive signal corresponding to the tracking error signal TE to the tracking coil 13. . As a result of supplying such a drive signal to the tracking coil 13, the objective lens 9 is displaced in the radial direction of the optical disk D. Such a displacement direction is performed in a direction to decrease the value of the tracking error signal TE described above. become. As a result of such an operation, an operation of causing the laser spot generated by the focusing operation of the objective lens 9 to follow the signal tracks provided on the signal recording layers L1, L2, and L3 of the optical disc D, that is, a tracking control operation is performed. Can be done.

  Reference numeral 32 denotes a focusing coil driving circuit to which a focus control signal output from the pickup control circuit 30 is applied, and is configured to supply a driving signal corresponding to the above-described focus error signal FE to the focusing coil 12. . As a result of supplying such a drive signal to the focusing coil 12, the objective lens 9 is displaced in a direction perpendicular to the signal surface of the optical disc D. Such a displacement direction reduces the value of the focus error signal FE described above. Will be done in the direction. As a result of such an operation, an operation for generating a laser spot generated by the focusing operation of the objective lens 9 on the signal recording layers L1, L2, and L3 of the optical disc D, that is, a focus control operation can be performed.

Reference numeral 33 denotes a collimating lens driving circuit to which a collimating lens position control signal output from the pickup control circuit 30 is applied. The driving signal is supplied to the collimating lens driving coil 7, and the collimating lens 6 is moved in the direction of the optical axis. It is configured to be displaced in the A and B directions.

  In this way, the collimating lens 6 is displaced in the directions of the arrows A and B. Such a displacement operation is performed corresponding to the optical disc D to be used, that is, the first optical disc, the second optical disc, and the third optical disc. The position of the collimating lens 6 whose displacement is controlled by such an operation is set so that the spherical aberration is corrected in each optical disk used, that is, the position where the spherical aberration is minimized.

  As described above, the spherical aberration correction operation is performed by adjusting the position of the collimating lens 6. However, since the signal recording layer L3 of the third optical disk is farthest from the objective lens 9, the third optical disk is used. Is configured such that the light emitted from the collimating lens 6 becomes divergent light. That is, the collimator lens 6 is configured to be diverged so that the condensing position of the objective lens 9 is adjusted to be the position of the signal recording layer L3 by using divergent light.

  As described above, the embodiment shown in FIG. 1 is configured. Next, the operation of the optical pickup apparatus configured as described above will be described. When a reproduction operation of a signal recorded on the optical disk D is performed, a driving current is supplied to the laser diode 1 and a laser beam having a wavelength of 405 nm is emitted from the laser diode 1. Laser light emitted from the laser diode 1 is incident on the diffraction grating 2 and is separated into 0th-order light, + 1st-order light, and −1st-order light by the diffraction grating portion 2 a constituting the diffraction grating 2, and 1 / It is converted into linearly polarized light in the S direction by the two-wavelength plate 2b. The laser beam that has passed through the diffraction grating 2 is incident on the polarization beam splitter 3, reflected by the control film 3 a provided on the polarization beam splitter 3, and partially transmitted through the laser beam. The detector 4 is irradiated.

  The laser light reflected by the control film 3 a enters the collimating lens 6 through the quarter-wave plate 5 and is converted into parallel light by the action of the collimating lens 6. The laser light converted into parallel light by the collimating lens 6 is reflected by the reflecting mirror 8 and then enters the objective lens 9. The laser light incident on the objective lens 9 is irradiated as a spot on the signal recording layers L1, L2, and L3 of the optical disc D by the focusing operation of the objective lens 9. In this way, the laser light emitted from the laser diode 1 is irradiated as desired spots on the signal recording layers L1, L2, and L3 of the optical disc D. In this case, the numerical aperture of the objective lens 9 is 0.65. It is set to be.

  Further, when the above-described focusing operation of the laser beam by the objective lens 9 is performed, spherical aberration occurs due to the difference in the thickness of the protective layer between the signal recording layers L1, L2, and L3 and the signal incident surface of the optical disc D. However, since the collimating lens 6 is displaced to the position where the spherical aberration of each optical disk D is minimized, the influence of the spherical aberration can be eliminated. When the third optical disk is used, the collimating lens 6 performs a spherical aberration correction operation and a converging position adjustment operation to generate a laser spot suitable for the signal reading operation on the signal recording layer L3. Is called.

The operation of irradiating the signal recording layers L1, L2, and L3 provided on the optical disc D with laser light is performed by the above-described operation. When such an irradiation operation is performed, the signal recording layers L1, L2, and L3 The reflected return light is incident on the objective lens 9 from the optical disc D side. The return light incident on the objective lens 9 is incident on the polarization beam splitter 3 through the reflecting mirror 8, the collimating lens 6 and the quarter wavelength plate 5. Since the return light incident on the polarizing beam splitter 3 is converted into linearly polarized light in the P direction, it passes through the control film 3 a provided on the polarizing beam splitter 3.

  The return light of the laser light that has passed through the control film 3 a is incident on the sensor lens 10, and astigmatism is generated by the action of the sensor lens 10. The return light in which astigmatism is generated by the sensor lens 10 is irradiated to a sensor unit such as a four-divided sensor provided in the photodetector 11 by the condensing operation of the sensor lens 10. As described above, as a result of the return light being applied to the photodetector 11 in this way, the change in the spot shape applied to the sensor unit incorporated in the photodetector 11 is utilized as described above. 14, the tracking error signal TE, the focus error signal FE, and the reproduction signal RF are generated.

  When the light detection signal generation circuit 14 generates the tracking error signal TE, the focus error signal FE, and the reproduction signal RF, the pickup control operation is performed by the pickup control circuit 30 to which such signals are input. That is, since the control operation of the drive signal to the tracking coil 13 accompanying the supply operation of the tracking control signal from the pickup control circuit 30 to the tracking drive circuit 31 is performed, the tracking control operation in the optical pickup device is performed.

  Further, since the control operation of the drive signal to the focusing coil 13 accompanying the operation of supplying the focusing control signal from the pickup control circuit 30 to the focusing coil drive circuit 32 is performed, the focus control operation in the optical pickup device is performed. Then, the reproduction signal RF read from the optical disc D is supplied to a decoding circuit incorporated in the optical disc apparatus, and the signal is demodulated.

  As described above, the tracking control operation and the focus control operation in the optical pickup device are performed, and the signal recorded on the optical disc D is read. 4 is irradiated with a part of the laser beam, the drive current value supplied to the laser diode 1 can be controlled using the monitor signal obtained from the monitor photodetector 4.

  Since the output of the laser beam can be controlled by controlling the value of the drive current supplied to the laser diode 1, not only the operation of reading the signal recorded on the optical disc D but also the case where the signal is recorded on the optical disc D It is also possible to adjust the laser output required for the laser.

  As described above, the operation of the embodiment shown in FIG. 1 is performed. Next, another embodiment shown in FIG. 2 will be described. In FIG. 2, the same components as those in the embodiment shown in FIG.

  In FIG. 2, reference numeral 34 denotes a liquid crystal control optical element using liquid crystal as spherical aberration correction means, and an electrode pattern for correcting spherical aberration generated from each optical disk D is formed as is well known. A liquid crystal drive control circuit 35 controls the operation of the liquid crystal control optical element 34 based on a control signal supplied from the optical pickup control circuit 30, and is suitable for correcting the spherical aberration of each optical disk D used. It is configured to control so as to obtain a pattern shape.

  Further, as described above, the liquid crystal control optical element 34 is configured to correct the spherical aberration. However, when the third optical disk is used, the condensing position of the objective lens 9 is moved backward to make the signal recording layer L3. A laser spot suitable for a signal reading operation is generated on the top.

  In the optical pickup device shown in FIG. 2, the same control operation as that of the embodiment shown in FIG. 1 is performed. However, the spherical aberration correction operation is replaced by the liquid crystal control optical element instead of the collimating lens 6 moving operation. This is different from the point performed at 34.

  As described above, the operation of the embodiment shown in FIGS. 1 and 2 is performed. Next, the tracking control operation by the differential push-pull method described in this embodiment will be described.

  Such tracking control operation is performed using the signal obtained from the quadrant sensor unit 11a as described above, that is, (A + D)-(B + C). Such a signal is generated in the land formed in the signal recording layer. And the difference in the height of the groove.

  That is, the phase difference of the return light obtained from the difference in height between the land and the groove is φ, the wavelength of the laser light is λ, the refractive index of the protective layer covering the signal recording layers L1, L2, and L3 of the optical disc D is n, When the depth of the groove is d, the phase difference φ is expressed as φ = 2π / λ × 2nd. As is apparent from such an equation, when d = λ / 4n, the phase difference φ is π, so that the push-pull signal becomes 0 and the tracking error signal cannot be generated.

  Therefore, in the standard of the optical disk, in consideration of the wavelength, refractive index, etc. of the laser beam used, d which is the depth of the groove is set to have a relationship of d = λ / 5n.

  In the embodiment of the present invention, the wavelength of the laser beam is set to 405 nm, and the numerical aperture of the objective lens is set to 0.65. Under such conditions, in the HD DVD standard as the first optical disk, the groove depth d is , D = λ / 5n. Therefore, when the first optical disk is used, a tracking error signal for performing the tracking control operation by the differential push-pull can be generated, so that the tracking control operation by the differential push-pull method can be performed without any trouble. I can do it.

  Under such conditions, the groove depth d in the standard of the DVD disc as the second optical disc is d = λ / 3n in the case of DVD-R / RW, and the tracking control operation by the differential push-pull is performed. A tracking error signal can be generated. The value of d corresponds to a value of λ / 5n in the case of 660 nm which is the wavelength of the laser beam set corresponding to the DVD-R / RW standard optical disc.

  In the case of a DVD-ROM in a DVD standard optical disk, d = λ / 2.4n, and a tracking error signal for performing a tracking control operation by differential push-pull can be generated. The value of d corresponds to a value of λ / 4n in the case of 660 nm which is the wavelength of the laser beam set corresponding to the DVD-ROM standard optical disc. The depth d of the groove of the DVD-ROM cannot be obtained when a laser beam of 660 nm is used, because d is λ / 4n. Therefore, since the conventional optical pickup device cannot perform the tracking control operation by the differential push-pull method, it is configured to perform the tracking control operation using a special control method such as a phase difference method. It was.

Therefore, when reading signals recorded on DVD-R / RW discs and DVD-ROM discs using laser light having a wavelength of 660 nm, in addition to the tracking control circuit based on the push-pull method, the phase difference Since it is necessary to incorporate a tracking control circuit according to the law, there is a problem that not only the configuration becomes complicated but also the cost becomes high. In the present invention, since laser light having a wavelength of 405 nm is used, the push-pull method can be adopted as a tracking control method for all optical discs of the DVD standard, and the circuit configuration and the like can be simplified.

  Further, in the case of an optical disc called CD-ROM / R / RW in the CD standard which is the third optical disc, d = λ / 2.6n, and a tracking error signal for performing tracking control operation by differential push-pull is obtained. Can be generated. The value of d corresponds to a value of λ / 5n in the case of 780 nm which is the wavelength of the laser beam set in correspondence with the optical disc of the CD-ROM / R / RW standard.

  As described above, according to the present invention, the tracking control operation for the second optical disk and the third optical disk can be performed with a laser beam having a wavelength corresponding to the standard of the first optical disk, that is, the shortest wavelength of 405 nm. The reading operation of signals recorded on optical disks of different standards can be performed by the same optical system.

  As described above, when reading the signals recorded on the optical disc D of three different standards, the laser beam having the shortest wavelength is used and the objective lens 9 having the largest numerical aperture is used. Therefore, although the condensing position of the objective lens 9 is set to be the position of the signal recording layers L1 and L2 of the first optical disc and the second optical disc, in the present invention, the position adjustment of the collimating lens 6 or the liquid crystal control is performed. Since the focusing position of the objective lens 9 is retracted by the adjustment operation by the element 34, the focusing position can be matched with the signal recording layer L3 of the third optical disc.

  Further, the spot diameter of the laser beam generated on the signal recording layer L3 by the focusing operation by the objective lens 9 becomes small. By setting the range of the intensity distribution of the laser beam used as the spot wide, the spot diameter can be reduced. The signal can be enlarged, and the signal recorded on the third optical disk can be read without any trouble.

  In this embodiment, the collimating lens 6 is displaced in the optical axis direction by a driving signal supplied from the collimating lens driving circuit 33 to the collimating lens driving coil 7. This is performed using a signal obtained from the signal generation circuit 14. For example, the collimating lens driving coil 7 is driven so that the intensity of the return light reflected from the signal recording layers L1, L2, and L3 of the optical disc D, the magnitudes of the tracking error signal TE, and the focus error signal FE become desired values. A signal is supplied and the position of the collimating lens 6 is adjusted by displacement.

  When the liquid crystal control optical element 34 is used as the spherical aberration correction means, the intensity of the return light reflected from the signal recording layers L1, L2, and L3 of the optical disc D, the magnitude of the tracking error signal TE, and the focus error signal FE are large. By adjusting the drive control signal supplied from the liquid crystal drive control circuit 35 to the liquid crystal control optical element 34 so that the desired value becomes a desired value, the reading operation suitable for each optical disk is set. I can do it.

  In the present embodiment, the reading operation of signals recorded on three types of optical discs having different standards for the first optical disc, the second optical disc, and the third optical disc is performed in the same optical system. It is also possible to perform an operation of reading signals recorded on two different types of optical disks.

  In the present invention, the collimating lens and the liquid crystal control optical element are used as means for correcting the spherical aberration. However, various spherical aberration correcting elements can of course be used.

It is the schematic which shows one Example of the optical pick-up apparatus of this invention. It is the schematic which shows one Example of the optical pick-up apparatus of this invention. It is a block circuit diagram which generates a tracking error signal. FIG. 4 is a block circuit diagram for generating a focus error signal and a reproduction signal.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Laser diode 2 Diffraction grating 3 Polarizing beam splitter 6 Collimating lens 7 Collimating lens drive coil 9 Objective lens 10 Sensor lens 11 Photo detector 12 Focusing coil 13 Tracking coil 14 Photo detection signal generation circuit 30 Pickup control circuit 31 Tracking coil drive circuit 32 Focusing coil drive circuit 33 Collimate lens drive circuit 34 Liquid crystal control optical element 35 Liquid crystal drive control circuit D Optical disc

Claims (2)

A first optical disc defined to perform a signal reading operation with a laser beam of a first wavelength and a signal reading operation with a laser beam of a second wavelength that is longer than the first wavelength are specified. And an optical pickup device for reading a signal from the second optical disc, the laser diode emitting a laser beam of the first wavelength, and the laser beam emitted from the laser diode on a signal recording layer provided on the optical disc. The objective lens for condensing, and spherical aberration correction means provided in the optical path between the laser diode and the objective lens, and by performing spherical aberration correction operation by the spherical aberration correction means, the same optical system The signal recorded on the first optical disc and the second optical disc is read, and the first optical disc and the second optical disc are read. A photo-detector that is irradiated with return light, which is laser light of the first wavelength reflected from the signal recording layer of each optical disc of the disc, is provided, and a push-pull signal for each optical disc is obtained from the photo-detector and tracking control operation And the depth d of the groove formed in the signal recording layer with respect to the wavelength of the laser beam defined on the second optical disc is d = λ / 4n (where λ is the laser beam defined on the second optical disc) And n is the refractive index of the protective layer that covers the signal recording layer of the second optical disk). performs signal reading operation using a push-pull signal by a laser beam having a wavelength for the second optical disc as defined in the first optical disk is different from the defined wavelength The optical pickup apparatus is characterized in that to obtain the. A collimating lens is used as the spherical aberration correcting means, the spherical aberration is corrected by displacing the collimating lens in the optical axis direction, and the focusing of the objective lens is performed by displacing the collimating lens in the optical axis direction. The optical pickup device according to claim 1, wherein the position is adjusted.

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