JP5188461B2 - Optical pickup, optical information recording apparatus, and optical information reproducing apparatus - Google Patents

Description

  The present invention relates to an optical pickup and an optical information recording / reproducing apparatus equipped with the optical pickup.

  For example, Japanese Patent Application Laid-Open No. 7-272303 is a background art related to this technique. This publication describes, as a problem, “to provide an optical disc apparatus, an optical pickup, and an optical pickup assembling method capable of reducing the overall shape with a simple configuration and simplifying assembling work as necessary”. As a solving means, there is a description that "the output signals between the light receiving surfaces E, G, F, and H are added in advance and then amplified and output before the amplifier circuits 15E and 15H".

JP 7-272303 A

  In recent years, as a means for realizing an increase in the recording capacity of an optical disk, a technique relating to an optical information recording medium (hereinafter referred to as an optical disk for the sake of simplicity) having a multi-layered recording layer has been developed.

  In addition, there is so-called tracking control for stably and highly accurately condensing a laser beam on a predetermined recording track provided on a recording layer of an optical disc. As a general tracking control signal detection method, there is a differential push-pull method (hereinafter, this method is referred to as a DPP method).

  An object of the present invention is to provide an optical pickup and an optical information recording / reproducing apparatus that are stable and highly accurate even for a recording medium having multiple recording layers.

  The above object can be achieved by the configurations described in the claims.

  According to the present invention, it is possible to provide a stable and highly accurate optical pickup and optical information recording / reproducing apparatus.

The schematic plan view which shows the photodetector which is the principal part of a 1st Example. FIG. 2 is a schematic front view showing a conventional optical system configuration of an optical pickup according to the present invention. The schematic plan view which shows the prior art example of a photodetector. 1 is a schematic sectional view of a multilayered optical disc. FIG. 3 is a schematic cross-sectional view showing an optical path of a light beam incident on a multilayered optical disc. The schematic plan view which shows the photodetector which is the principal part of a 2nd Example. The schematic front view which shows the shape of the diffraction grating used by the 3rd Example. The schematic plan view which shows the state of the sub-light-beam spot which injects into a photodetector in a 3rd Example. FIG. 5 is a schematic diagram of an optical information recording / reproducing apparatus equipped with optical pickups according to first to third embodiments. The schematic plan view which shows the photodetector which is the principal part of a 4th Example. The schematic plan view which shows the photodetector which is the principal part of a 5th Example.

  Examples will be described below.

  The DPP method will be briefly described.

  FIG. 2 is a schematic diagram of a main optical system of an optical pickup using tracking control signal detection means based on the DPP method.

  Two laser beams emitted from the semiconductor laser 1 are used to generate a main light beam 50 (0th-order light) for actually reproducing or recording an information signal by a light beam splitting element such as a diffraction grating 2 and a tracking control signal. Are divided into sub-beams 51 and 52 (± first-order diffracted light). Each of these light fluxes is independently condensed on a predetermined recording layer in the optical disc 10 by the objective lens 5 through the half mirror 3 and the collimating lens 4. At this time, the condensing spot (not shown) of the main light beam 50 and the condensing spots (not shown) of the sub-light beams 51 and 52 are arranged such that the irradiation position interval in the radial direction of the optical disc 10 is the recording track interval of the optical disc 10. Irradiation is performed so as to match approximately half of the distance. Then, the reflected light beam from the optical disk 10 at each of these condensed spots passes through the objective lens 5, the collimating lens 4, and the half mirror 3 again, and then enters the photodetector 8 through the detection lens 7.

  The objective lens 5 is provided with an actuator 6 for driving the objective lens 5 in a predetermined direction, and tracking control is performed by feeding back a tracking control signal described later to the actuator 6 to control the position of the objective lens. Executed.

  By the way, for example, as shown in FIG. 3, the photodetector 8 is a light receiving region 80 on which the converging spot 60 made of the optical disk reflected light of the main light beam 50 enters and light made of the optical disk reflected light of the sub-light beams 51 and 52. Light receiving areas 81 and 82 on which the spots 61 and 62 are incident are arranged in parallel in the vertical direction of the figure. Of these, the light receiving area 80 for the main light beam 50 is constituted by a light receiving surface divided into four by a cross-shaped dividing line, for example, as shown in the figure, while the light receiving areas 81 and 82 for the sub light flux are divided lines. Each of the light receiving surfaces 83 and 84 is divided into two in the vertical direction in the figure. Then, a current corresponding to the incident light intensity is generated from each of the divided light receiving surfaces, and each current-voltage conversion is performed independently by the current-voltage conversion amplifiers 201 to 208, and then subtracted by the subtractors 210 and 211. A signal obtained by adding a push-pull signal of the main light beam 50 (hereinafter referred to as a main PP signal for simplicity) and a push-pull signal of the sub-light beams 51 and 52 (hereinafter referred to as sub PP signal for simplicity). Is output).

  The main PP signal and the sub PP signal output at this time are output with their signal phases shifted from each other by 180 degrees because the respective focused spots on the optical disc 10 are arranged as described above. For this reason, both PP signals are amplified by the amplifiers 212 and 213 with appropriate amplification factors K1 and K2, respectively, and then subtracted by the subtractor 214, so that unnecessary DC components included in both the main PP signal and the sub PP signal are obtained. In other words, a good tracking control signal from which disturbance components having the same phase are removed is output.

  As described above, the DPP method can remove a tracking control signal offset caused by tracking displacement of an objective lens, for example, with a simple optical system configuration, and can stably detect a high-quality tracking control signal. It is widely used as an effective tracking control signal detection means. Hereinafter, an arithmetic circuit including subtractors 210 and 211, amplifiers 212 and 213, and subtracter 214 configured to detect a tracking control signal as described above is referred to as tracking control signal detection circuit 500.

  Note that the position control of the objective lens 5 in the optical pickup is not limited to the tracking control described above, and naturally, position control along the optical axis direction, so-called focus control, is simultaneously performed. As a detection method of the focus control signal used for the focus control, for example, an astigmatism method is generally used, and, for example, in the photodetector 8 shown in FIG. These signals can be generated from signals detected on the respective light receiving surfaces through a predetermined arithmetic circuit.

  As described above, the DPP method is a widely used method.

  However, when such a tracking control signal detection means based on the DPP method is used for an optical pickup or an optical information recording / reproducing apparatus for reproducing or recording an optical disk having a multi-layered recording layer, the following new problems arise.

  That is, each light beam is applied to a recording layer that is actually a signal recording or reproducing target (hereinafter, this recording layer is referred to as a target layer for the sake of simplicity) among the recording layers in the multilayered optical disc. When condensed, a part of the amount of light does not reflect this target layer, but is reflected by the recording layer other than the target layer and becomes an unnecessary light beam that does not contribute to actual signal detection, and is almost the same as the original signal light beam. There arises a problem that the light follows the same optical path and enters each light receiving surface in the photodetector. The unwanted light flux incident on the light receiving surface interferes with the original signal light flux on the light receiving surface, and unnecessary disturbance components leak into the signal output from each light receiving surface as a result of the light quantity imbalance due to the interference fringes. It will end up.

  This phenomenon will be specifically described by taking as an example an optical disc 10 having two recording layers (layer spacing δ) 100 and 101 as shown in FIG.

  For example, FIG. 5 schematically shows a state in which a main light beam 50 and sub-light beams 51 and 52 (not shown) are condensed from the lower side of the drawing onto the optical disk 10 having the same two recording layers 100 and 101 as FIG. It is the figure shown in.

  First, FIG. 5A shows a case where each light beam is condensed on the recording layer 100 on the near side (the lower side in the figure), that is, a case where the recording layer 100 is a target layer. In such a case, a part of the light amount of the light spot condensed on the recording layer 100 is transmitted through the recording layer 100 and reflected by the recording layer 101 on the back side (upper side in the figure) to be an unnecessary light beam 53. Become.

  5B shows the case where each light beam is condensed on the recording layer 101 on the back side (upper side in the figure), that is, the recording layer 101 is the target layer, contrary to the case of FIG. It shows a case. In such a case, the light beam once passes through the recording layer 100 on the near side (the lower side of the figure) and then is condensed on the recording layer 101. At this time, a part of the light quantity reflects the recording layer 100 and is unnecessary. A light beam 54 is obtained.

  Such unnecessary light fluxes 53 and 54 follow the optical path almost the same as the original signal light flux and reach the photodetector, but at this time, they are irradiated with a large spread on each light receiving surface in the photodetector. Then, a part of the light overlaps with an original signal light beam irradiated on each light receiving region, thereby causing interference. As a result, bright and dark interference fringes are generated in each light receiving region, and unnecessary disturbance components leak into signals detected from the respective light receiving surfaces due to local light quantity imbalance caused by the interference fringes.

  In particular, the sub PP signal used for tracking control signal detection by the DPP method generally has a signal intensity smaller than that of the main PP signal. Therefore, the light amount imbalance due to the interference between the unnecessary light beam and the signal light beam is not generated. This greatly affects and a relatively large disturbance component leaks from the actual signal amplitude. As a result, large waveform distortion and fluctuation occur in the tracking control signal detected by the DPP method, and the signal quality is deteriorated.

  The inventor examined the degree of influence of the interference between the unnecessary light flux and the signal light flux on the sub PP signal. Of the light quantity imbalance in each light receiving area caused by the interference, the light receiving area for detecting the sub PP signal is used. It has been found that the light quantity imbalance generated on and near the dividing lines (83 and 84 in FIG. 3) provided in (light receiving areas 81 and 82 in FIG. 3) has the most adverse effect on the quality of the sub PP signal. did.

  On the other hand, the main PP signal and the sub PP signal itself are generated mainly by the change in the amount of light at the periphery of each spot of the light spots (ie, 60 to 62 in FIG. 3) focused on each light receiving area. It is also known that the higher the information signal recording density is, the higher the tendency is as the recording track interval is narrower.

  Based on the above situation, an optical pickup using a tracking control signal detection means based on the DPP method and having a function of recording an information signal on an optical disc having two or more recording layers or reproducing the recorded information signal And in an optical information reproducing apparatus equipped with the same, the quality deterioration of the tracking control signal caused by the interference between the unnecessary light beam generated from the recording layer other than the target layer and the original signal light beam on each light receiving area of the photodetector. An object of the present invention is to provide an optical pickup that can be satisfactorily improved and can detect a stable and highly accurate tracking control signal, and an optical information reproducing apparatus equipped with the optical pickup.

  FIG. 1 is a diagram showing a configuration of a photodetector which is a main part of the first embodiment. In FIG. 1, the same components as those of the photodetector already described with reference to FIG.

  The optical system configuration of the optical pickup in this embodiment may be the same as that of the optical pickup shown in FIG. A difference from FIG. 2 is a light receiving surface pattern in the photodetector 8. As is clear from the comparison of the light receiving surface pattern of the photodetector 8 of this embodiment shown in FIG. 1 and the light receiving surface pattern of the photodetector 8 shown in FIG. The width W on the short side is set to a predetermined dimension as will be described later on the center parting line (corresponding to parting lines 83 and 84 in the conventional example of FIG. 3) of the light receiving regions 81 and 82 into which 61 and 62 respectively enter. A set shading zone or dead zone 73 and 74 is provided. Of these, the light shielding band can be realized by depositing a light-impermeable medium such as aluminum on the light receiving surface so that the light beam does not directly enter the light receiving surface covered with the light shielding band. Thus, the present embodiment can be easily applied to an optical pick that is not compatible with the present embodiment. In addition, the dead zone can be realized by, for example, deleting the light receiving surface of the corresponding part so that a signal current corresponding to the light beam is not generated even if the light beam is actually incident on the part.

  The light-shielding band is not limited to a medium whose transmittance is almost zero with respect to light in the entire wavelength band such as aluminum as described above. For example, it transmits only light in a specific wavelength band. A medium having wavelength selectivity such that the rate is substantially zero may be used as the light shielding band.

  Thereby, an optical pickup corresponding to the present embodiment can be generated at low cost. By providing such a light-shielding zone or dead zone on the light-receiving areas 81 and 82 for the sub-beams, the unwanted light flux generated from the recording layer other than the reproduction or recording target layer and the recording / reproduction target layer in the multi-layer disc as described above. Even if interference with the original signal light beam obtained occurs, it is possible to effectively reduce the disturbance component that leaks into the sub PP signal.

  On the other hand, since the sub PP signal itself is generated mainly by the change in the amount of light at the periphery of each light spot condensed in each light receiving region as described above, there is almost no influence by the light shielding zone or the dead zone. Therefore, as a result, even in an optical disc having a multi-layered recording layer, a tracking control signal based on the DPP method can be detected with high accuracy and stability.

  The width W on the short side of the light-shielding zone or dead zone is about 20% to the diameter of the condensing spots 61 and 62 of the sub-beams incident on the light-receiving regions 81 and 82 as a result of the inventors' investigation. It has been found that setting within the range of 40% is most effective in terms of the disturbance component. More specifically, in a normal optical pickup, the diameter of the condensing spots 61 and 62 of the sub-beams incident on the light receiving regions 81 and 82 is most commonly designed to be about 100 μm. The width W on the short side of the light shielding zone or dead zone is preferably set within a range of about 20 μm to 40 μm.

  Next, a second embodiment will be described with reference to FIG.

  FIG. 6 shows the main part of the second embodiment. Also in this figure, the same components as those shown in FIGS. 1 and 3 are denoted by the same reference numerals.

  In this embodiment, instead of providing a light shielding zone or a dead zone as in the first embodiment shown in FIG. 1, newly above and below the original dividing lines 83 and 84 provided in the sub-beam light receiving areas 81 and 82 are newly provided. 83, 84 are provided with dividing lines 85, 86, 87, and 88, and each of these three dividing lines provides light receiving area 81 on four light receiving surfaces 81a to 81d and light receiving area 82 on 82a to 82d. Each is divided into four light receiving surfaces. At this time, the interval between the dividing lines 85 and 86 and the interval W between the dividing lines 87 and 88 are approximately the same as the width W on the short side of the light shielding zone or dead zone in the first embodiment shown in FIG. ing. Among the light receiving surfaces divided into four in this way, for example, a signal output from the light receiving surface 81a via the current-voltage conversion amplifier 201 and the signal line 301, and a light receiving surface 81d from the signal line 301 via the current-voltage conversion amplifier 202. When a sub PP signal is generated from the output signal, this signal becomes exactly the same signal as the sub PP signal obtained from the photodetector of the first embodiment shown in FIG. In exactly the same manner, the sub PP generated from the signal output from the signal line 305 via the current-voltage conversion amplifier 207 from the light receiving surface 82a and the signal output from the signal line 308 via the current-voltage conversion amplifier 208 from the light receiving surface 82d. The signal is also exactly the same as the sub PP signal obtained from the photodetector of the first embodiment. On the other hand, the signal detected from the light receiving surface 81a or the light receiving surface 82a via the current-voltage conversion amplifier 201 or 207 and the signal detected from the light receiving surface 81b or the light receiving surface 82b via the current-voltage conversion amplifier 209 or 211 are added. A signal output from the signal line 302 or 306 after addition processing at 215 or 217, a signal detected from the light receiving surface 81d or the light receiving surface 82d via the current-voltage conversion amplifier 202 or 208, and a current from the light receiving surface 81c or the light receiving surface 82c. When the signal detected via the voltage conversion amplifier 210 or 212 is added by the adder 216 or 218 and the sub PP signal is generated from the signal output from the signal line 303 or 307, this signal is converted into the conventional signal shown in FIG. Is exactly the same as the sub PP signal obtained from the photo detector It becomes No.. Therefore, in this embodiment, the signal line for generating the sub PP signal is selectively switched as described above by using the changeover switches 401 and 402, so that the photodetector of the present invention and the conventional light can be obtained with one photodetector. Both functions of the detector can be combined. Therefore, the versatility of the optical pickup can be improved by properly using the above functions depending on the type of optical disk, for example, a multilayered disk or a conventional single-layer recording disk.

  Next, a third embodiment will be described with reference to FIGS. In the present embodiment, the optical system configuration of the optical pickup and the configuration of the photodetector 8 may be the same as those shown in FIGS. 2 and 3, respectively. Instead, the diffraction grating 2 used as a light beam splitting element has a different structure from the conventional grating. FIG. 7 is a schematic plan view showing the structure of the diffraction grating 2 used in this embodiment. In this embodiment, the diffraction grating 2 is placed in a direction substantially perpendicular to the grating groove direction (that is, the direction corresponding to the disk radial direction on the diffraction grating 2) (that is, the direction corresponding to the tangential direction of the disk on the diffraction grating 2). It is divided into three regions 21, 22, and 23 by two extending dividing lines. Of these, the lattice regions are engraved in the two regions 21 and 23 that sandwich the central region 22. In 22, the lattice is a transparent flat plate.

  When the light beam emitted from the laser light source enters the diffraction grating 2 having such a structure, only the light beam portion passing through the central region 22 is not diffracted, and only the central light beam is diffracted and separated from the main light beam. The light flux is in a state of being removed in a substantially band shape. For this reason, the condensing spot of the sub-light beam finally incident on the light receiving areas 81 and 82 in the photodetector 8 through the optical disk should also be incident on the dividing lines 83 and 84 and in the vicinity thereof, as shown in FIG. The light flux part of the light beam passes through in a band shape, and becomes a condensing spot divided into two like 61a and 61b and 62a and 62b, and is incident on each light receiving surface.

  For this reason, even if the light receiving region of the photodetector 8 has a configuration in which no light shielding zone or dead zone is provided, the same effect as that of the first embodiment shown in FIG. 1 can be obtained.

  In general, the structure of the diffraction grating as shown in FIG. 7 as in this embodiment is more cost-effective than providing a light-shielding zone or dead zone in a precise and expensive component such as a photodetector. There is an advantage that it is advantageous in terms of workability.

  For the width W ′ of the central region 22 of the three-part grid shown in FIG. 7, the interval W between the focused spots 61a and 61b or 62a and 62b on the light receiving regions 81 and 82 of the photodetector 8 is It is desirable to design so as to be equivalent to W of the shading zone or the dead zone in the embodiment of FIG.

  Next, a fourth embodiment of the present invention will be described with reference to FIG. In this embodiment, as in the first embodiment of the present invention shown in FIG. 1, predetermined light-shielding bands or dead bands 73 and 74 are provided on the center parting lines of the sub-beam light receiving areas 81 and 82. Further, by providing each light receiving region 81, 82 with a dividing line that is substantially perpendicular to the central part dividing line, each light receiving region is divided into four as with the main light receiving region 80. The purpose of dividing the sub-beam light-receiving areas 81 and 82 in addition to the main light-beam light-receiving area 80 in this way is to use the astigmatism method in the sub-beam light-receiving areas 81 and 82 as well as the main light-beam light-receiving area 80. This is for detecting the focus control signal. In order to detect the focus control signal by the astigmatism method from each of the main light beam receiving area 80 and the sub light beam light receiving areas 81 and 82, as shown in FIG. Although an arithmetic circuit comprising adders 228 to 235 and subtracters 236 and 237 provided in FIG. 1 is used, the detection of the focus error signal by the astigmatism method is already a well-known technique, and thus further detailed description is omitted. To do. In addition to the adder and subtractor described above, the focus control signal detection circuit 501 includes an amplifier 238 for amplifying the focus control signal detected in the sub-beam light receiving areas 81 and 82 at a predetermined amplification factor K3 and the amplified signal. An adder 239 for adding the sub-beam focus control signal and the main beam focus control signal detected in the main light-receiving area 80 is disposed. A method of adding a signal obtained by adding the focus control signal of the main light beam and the focus control signal of the sub light beam to a new focus control signal is called a differential astigmatism method (DAD method), and astigmatism. This method is an effective method for detecting a good focus control signal by removing a disturbance component leaking into the focus control signal by this method. However, since this method itself is a known technique, detailed description thereof is omitted. In the focus control signal detection circuit 501, either a signal obtained by adding the focus control signal of the main light beam and the focus control signal of the sub light beam as described above or a focus control signal generated only from the main light beam as in the conventional case. A change-over switch 403 is provided for switching and outputting, and it is possible to selectively switch which focus control signal is output according to the type of the optical disk to be reproduced or recorded. In this embodiment, in addition to the focus control signal detection circuit 501 described above, a tracking control signal detection circuit 500 similar to that in the embodiments of FIGS. 1 and 6 is also provided. Details of this tracking control signal detection circuit are provided. Has already been described with reference to FIGS. 1, 3, 6, etc., and detailed description thereof will be omitted here.

  Next, a fifth embodiment of the present invention will be described with reference to FIG. In this embodiment, the light receiving surface configuration is almost the same as that of the second embodiment of the present invention shown in FIG. 6, but the dividing lines 83, 85, 86 of the light receiving areas 81 and 82 for the sub-beams are further provided. , 84, 87, and 88, the light receiving areas are divided into eight areas in total by providing substantially perpendicular dividing lines. As in the second embodiment of the present invention shown in FIG. 6, the tracking control signal detection circuit 500 detects the tracking control signal, and in the same way as in the fourth embodiment of the present invention shown in FIG. The focus control signal can be detected by the control signal 501. The detailed contents of each of the tracking control signal detection method and the focus control signal detection method are the same as those already described in the other embodiments, so that detailed description is omitted here, but the configuration as in this embodiment is used. As a result, either the focus control signal or the tracking control signal can be selectively switched between the signal based on the light receiving surface configuration of the present invention or the signal based on the conventional light receiving surface configuration.

  By the way, the optical pickup using the present invention is not limited to the optical system configuration or the light receiving surface configuration described in the above embodiments, and a DPP method or a detection method equivalent to the DPP method is used as a tracking control signal detection method. Any optical system configuration or light receiving surface configuration can be used as long as the optical pickup is employed or an optical information reproducing apparatus equipped with the optical pickup.

  FIG. 9 is a schematic diagram of an optical information recording / reproducing apparatus equipped with the optical pickups according to the first to fourth embodiments. 900 is an optical disk, 910 is a laser lighting circuit, 920 is an optical pickup, 930 is a spindle motor, 940 is a spindle motor drive circuit, 950 is an access control circuit, 960 is an actuator drive circuit, 970 is a servo signal generation circuit, and 980 is an information signal A reproduction circuit, 990 is an information signal recording circuit, and 9000 is a control circuit. The control circuit 9000, the servo signal generation circuit 970, and the actuator drive circuit 960 control the actuator according to the output from the optical pick pickup 920. By using the output from the optical pickup in this embodiment for actuator control, stable and highly accurate information recording and information reproduction can be performed.

  By using each of the above-mentioned means, an unnecessary light beam generated from a recording layer other than the target layer to be reproduced or recorded when an information signal is reproduced or recorded on the recording layer from an optical disc having a multilayered recording layer It is possible to satisfactorily improve the deterioration of the quality of the tracking control signal caused by the interference with the original signal beam and to detect a stable and highly accurate tracking control signal.

DESCRIPTION OF SYMBOLS 1 ... Semiconductor laser light source, 2 ... Diffraction grating, 5 ... Objective lens, 8 ... Optical detector, 10 ... Optical disk, 50 ... Main light beam, 51, 52 ... Sublight beam, 73, 74 ... Shading zone or dead zone, 80, 81 , 82: Light receiving area, 100, 101 ... Recording layer, 900 ... Optical disc, 910 ... Laser lighting circuit, 920 ... Optical pickup, 930 ... Spindle motor, 940 ... Spindle motor drive circuit, 950 ... Access control circuit, 960 ... Actuator drive Circuit, 970 ... Servo signal generation circuit, 980 ... Information signal reproduction circuit, 990 ... Information signal recording circuit, 9000 ... Control circuit

Claims (2)

A semiconductor laser light source;
A beam splitter having a function of splitting a laser beam emitted from the semiconductor laser light source into a main beam and a sub beam;
An objective lens for condensing each of the main light beam and the sub light beam on a predetermined recording layer provided in an optical information recording medium;
A light detector that independently receives the main light beam and the sub light beam reflected from the recording layer and detects a predetermined signal; and
The photodetector includes a light receiving surface for main light flux that is divided into four by two split lines substantially perpendicular to each other on which the main light flux is incident, and three light beams that are incident on the sub-light flux and are substantially parallel to each other. A dividing line,
Has a secondary light beam-receiving surface which is divided into eight by the one dividing line which is substantially orthogonal to the three division lines, the shut-off means for cutting off a predetermined output from said photodetector,
When the optical information recording medium has a plurality of layers, the blocking means blocks the output from the four light receiving areas located substantially in the center of the light receiving surface for the sub-beam by the blocking means, and An optical pickup characterized in that when the information recording medium has only a single layer, it is not blocked by the blocking means . A semiconductor laser light source;
A beam splitter having a function of splitting a laser beam emitted from the semiconductor laser light source into a main beam and a sub beam;
An objective lens for condensing each of the main light beam and the sub light beam on a predetermined recording layer provided in an optical information recording medium, and the main light beam and the sub light beam reflected by the recording layer are independently received and predetermined light is received. A photodetector for detecting the signal,
The photodetector includes a light receiving surface for main light flux that is divided into four by two split lines that are substantially perpendicular to each other where the main light flux is incident, and is divided into two by at least one split line that is incident on the sub light flux. a secondary light beam-receiving surface that is, has a blocking means for chromatic said line dividing and a predetermined width in the vicinity provided in sub beam light receiving plane,
When the optical information recording medium has a plurality of layers , the blocking means blocks an output from a light receiving area located substantially at the center of the light receiving surface for the sub-beam, and the optical information recording medium is a single optical information recording medium. In the case of having only this layer, the output from the light receiving region located substantially in the center of the light receiving surface for the sub-beam is not cut off .

Images