JPH05242519A - Optical head device - Google Patents

Abstract

PURPOSE:To provide an optical head device capable of easily adjusting the position of the photodetector by arranging an optical divider having plural areas for respectively leading reflected light from an information recording face to different photodetectors. CONSTITUTION:A light beam from a laser light source 31 is made incident upon the optical divider 41 constituted by forming a diffraction grating 44 between bases 42, 43 through a collimeter lens 32. The incident light beam is directly transmitted through the divider 41, made incident upon a lambda/4 plate 34 and converted into a circularly polarized light and then the polarized light is converged upon an information recording face 37 by an objective lens 35 through a disk base 36. A light beam reflected on the recording face 37 is transmitted again through the lambda/4 plate 34 and converted into polarized light having a polarizing face rectangular to an incident face and the polarized light is made incident upon the divider 41. Reflected light from the divider 41 is diffracted or reflected by the grating 44, led through the base 43 while repeating full reflection and then made incident upon photodetectors 39, 40. Thus, a compact and light-weight device capable of easily adjusting the position of its photodetector can be provided.

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical head device for irradiating an information recording surface of an information carrier with light to detect or record information, and more particularly to an optical head device which is small and lightweight and suitable for mass production. is there.

[0002]

2. Description of the Related Art Conventionally, an optical head device has been constructed, for example, as shown in FIG. Here, the divergent light flux emitted from the laser light source 1 enters the collimator lens 2, becomes a parallel light flux, and enters the polarization beam splitter 3. Here, the polarization beam splitter 3 has a characteristic of transmitting almost 100% of linearly polarized light having an oscillating surface in a specific direction and reflecting almost 100% of linearly polarized light having an oscillating surface in a direction orthogonal thereto. The linearly polarized light transmitted through the polarization beam splitter 3 passes through the λ / 4 plate 4 to become circularly polarized light, which is condensed by the objective lens 5 on the information recording surface 7 provided on the substrate 6 of the information carrier, and the spot diameter is 1 μm. Form the front and back spots. Further, the light beam reflected by the information recording surface 7 passes through the objective lens 5 to become a parallel light beam and has a wavelength of λ / 4.
After passing through the plate 4, it becomes linearly polarized light whose vibrating surface is orthogonal to that at the time of incidence, and then enters the polarization beam splitter 3 again.
Here, the polarization beam splitter 3 functions as a light splitter due to the above-mentioned characteristics, reflects the reflected light from the information recording surface 7 and separates it from the incident light, and the light detector 9 as a converged light flux through the sensor lens 8. Lead to.

When information is recorded using such an optical head device, the laser light source 1 is driven in accordance with the information signal to modulate the light incident on the information recording surface 7. When detecting information, unmodulated light is applied to the information recording surface 7 on which information is recorded due to uneven pits or changes in reflectance, and the reflected light modulated by the recorded information is detected by a photodetector. 10. Detect and reproduce information. At this time, on the information recording surface 7, a track composed of a recording signal train or a guide track previously provided on the substrate 6 or the like extends in a direction perpendicular to the paper surface in FIG.
Densely formed. Therefore, in order to record or detect information correctly, it is necessary to perform control so that the spot always traces the above-mentioned track, that is, so-called auto-tracking.

[0004]

Conventionally, as an auto-tracking method, an element having a plurality of light-receiving surfaces divided in a direction corresponding to the width direction of a track is used as a photodetector 9 and obtained from each light-receiving surface. A method of obtaining a tracking error signal by subtracting the obtained signals is known. According to this tracking error signal, the spot is correctly guided on the track by a method such as moving the objective lens 5 perpendicularly to the optical axis by a mechanism (not shown). However, in such a conventional method, the information recording surface 7
Since the photodetector 9 was provided in the vicinity of the image forming position of
The mounting error of the photodetector has a great influence on the accuracy of the tracking error signal, and there is a drawback that a highly accurate position adjustment between the components is required at the time of assembling the device. Further, in order to increase the tolerance of the assembling accuracy, a method of detecting a tracking error signal in a parallel light flux of reflected light from the information recording surface using a large photodetector has been performed.
However, this method also has drawbacks such that the size of the photodetector becomes large and the response of the photodetector to a high frequency band is lowered, or the photodetector itself becomes expensive.

On the other hand, in the optical head device, in addition to the above-mentioned auto-tracking, information is recorded at high density on the information recording surface, and in order to detect the recorded information at high density, the light from the light source is always recorded as information. Autofocusing is performed to focus on the recording surface. Conventionally, various methods such as a so-called astigmatism method, a critical angle method, a Foucault method, a knife edge method, a beam lateral displacement method, etc. are known for this autofocusing, and one example thereof will be described with reference to FIG. An apparatus whose schematic configuration is shown in FIG. 13 is proposed in Japanese Patent Laid-Open No. 57-64335. Here, the semiconductor laser 11
The light emitted from is collimated by the collimator lens 12 and is condensed by the objective lens 15 on the information recording surface 17 on the substrate 16. The signal read on the information recording surface 17 is reflected by the information recording surface 17, and the monitor sensor 25 detects a change in the output of the semiconductor laser 11 due to a change in the amount of return light returning to the semiconductor laser 11 through the same optical path as when the light was incident. A so-called scoop (SCOOP) method is used. Further, the sensor lens 21 having the focal length f occupies a part of the pupil plane of the objective lens 15, and a part 26 of the light reflected by the information recording surface becomes a focused light beam 27 by the sensor lens 21 and is divided into two. It is incident on the photodetector 22.
When the information recording surface 17 becomes far from or near the focal position of the objective lens 15, the focused light flux 27 moves left and right on the photodetector 22. Therefore, a focus error signal is obtained by subtracting the respective outputs of the divided light receiving surfaces by the subtractor 23. The focusing actuator 24 is driven by this focus error signal, and an overfocus is performed so that the incident light is always focused on the information recording surface 17.

In the apparatus shown in FIG. 13, since the off-axis light beam of the objective lens is taken out, the detected light beam has a large effect on defocus, and highly sensitive focus error detection can be performed. However, on the other hand, the semiconductor laser 11
The light flux incident on the objective lens 15 from the light source is deflected by the sensor lens 21 and deformed. As a result, the information recording surface 17
It had a drawback that the upper spot became large.

[0007]

SUMMARY OF THE INVENTION An object of the present invention is to provide an optical head device in which the position of a photodetector can be easily adjusted.

Another object of the present invention is to provide an optical head device capable of partially extracting reflected light from the information recording surface by a photodetector without affecting the incident light on the information recording surface. There is a thing.

The above object of the present invention is achieved by providing an optical splitter having a plurality of regions for guiding the reflected light from the information recording surface to different photodetectors in the optical path from the light source to the information recording surface. To be done.

[0010]

Embodiments of the present invention will be described below with reference to the drawings.

FIG. 1 is a schematic sectional view showing the structure of a first embodiment of an optical head device according to the present invention. Laser light source 31
Is converted into a parallel light beam by the collimator lens 32, and the diffraction grating 4 is formed in the substrates 42 and 43 made of parallel flat plates.
4 is incident on the formed optical splitter 41. Since this light splitter 41 does not act on the incident light flux, the light flux is transmitted as it is, is incident on the λ / 4 plate 34 and becomes circularly polarized light, and is then transmitted through the substrate 36 by the objective lens 35. It is focused on the information recording surface 37. The light flux reflected by the information recording surface 37 passes through the objective lens 35 to become a parallel light flux, and again becomes λ
The polarized light is transmitted through the / 4 plate 34 and oscillates in a direction orthogonal to the time of incidence to enter the light splitter 41. This reflected light is diffracted or reflected by the diffraction grating 44 in the light splitter 41 and guided in the substrate 43 while repeating total reflection,
The light enters the photodetectors 39 and 40. Here, the information is recorded by driving the laser light source 31 in accordance with the information signal and modulating the incident light on the information recording surface 37. When detecting information, unmodulated light is applied to the information recording surface 37, and the reflected light modulated according to the information recorded therein is detected by the photodetectors 39 and 40 to reproduce the information.

FIG. 2 is a view of the light splitter 41 shown in FIG. 1 as seen from the direction of the light source 31. The diffraction grating 44 constituting the dividing surface of the optical splitter 41 is divided into two regions with the line segment AA 'as a boundary, and the two frame gratings 44a and 44b each having a different grating pattern are information recording surfaces. The reflected light from 37 is diffracted in different directions and guided to different photodetectors 40 and 39, respectively. By appropriately processing the output signals of the photodetectors 39 and 40, a focus error signal, a tracking error signal and an information reproduction signal necessary for the optical head device can be obtained.

First, the principle of detecting the focus error signal will be described. In the photodetector 39 described above, the light receiving surface is divided into three as shown in FIG. Information recording surface 37
It is assumed that the photodetectors are arranged so that when the minimum light spot is generated above (that is, in focus), the light amount distribution is as shown by the shaded portion in FIG. 3B. At this time, if the distance between the information recording surface 37 and the objective lens 35 is too large (that is, the object is out of focus), the spread of the light flux in the light receiving surface array direction decreases as shown in FIG. When the recording surface 37 and the objective lens 35 are too close to each other to be out of focus, the light amount distribution widens as shown in FIG.
Therefore, the light receiving surfaces 39A, 39B, 39C of the photodetector 39
The respective focus outputs I _A , I _B , and I _C of the focus error signal I are processed by the calculator 45 as follows.
You get _F.

I _F = (I _A + I _B ) −I _C

Next, the detection of the tracking error signal will be described. The split surface of the light splitter is the line segment A as described above.
It is divided into two areas by A '.
The direction of A'is arranged so as to coincide with the extending direction of the track formed of the signal train recorded on the information recording surface 37 or the guide track previously provided on the substrate 36 or the like. Therefore, the light received by the photodetectors 39 and 40 contains information from the right side and the left side of the track, respectively, and by calculating the difference between the outputs of these photodetectors 39 and 40 by the calculator 46, the so-called The push-pull tracking error signal I _T can be detected. Here, when the output of the photodetector 40 is represented by I _{D by} an arithmetic expression, I _T = (I _A + I _B + I _C ) −I _D.

In addition, the photodetector 3 is operated by the calculator 47.
The sum of the signal output of 9,40, calculating the _{I RF = (I A + I} B + I C) + I D, which is the information reproduction signal I _RF. The photodetector 40 used here may be an element of the same type as the photodetector 39, or may be one whose light-receiving surface is not divided.
When the photodetector 40 uses an element whose light-receiving surface is divided into three, the outputs from the respective light-receiving surfaces are I _D1 , I _D2 ,
If I _D3 , it is also possible to obtain the tracking error signal I ′ _T by the heterodyne method by performing the operation of I ′ _T = (I _D1 + I _C ) − (I _D3 + I _A ).

In this embodiment, since the optical splitter is formed in a parallel plate type, the optical head device as a whole can be made thin. Further, this optical splitter itself can be easily manufactured by collectively processing a plurality of substrates on a large-sized substrate and cutting them out, which is excellent in mass productivity. Further, in the present embodiment, the reflected light from the information recording surface is divided by the division surface of the optical divider, and each is detected by different photodetectors, so the mounting accuracy of the photodetector for detecting the tracking error signal is Is eased and assembly and adjustment is easy. Further, when the photodetector is integrally formed on the end face of the substrate of the light splitter, such assembling adjustment is unnecessary. Further, it is well known that it is generally desirable to detect the intensity distribution on the pupil plane of the objective lens in order to obtain a good tracking error signal, but in the present embodiment, it was placed near the objective lens. Since the intensity distribution on the split surface of the light splitter is detected, it means that the detection is effectively performed by splitting the pupil plane.
This enables highly reliable tracking control.

FIG. 4 schematically shows the structure of the diffraction grating used in the embodiment shown in FIG. Figure 4
(A) is a partial cross-sectional view of an optical splitter 41 using a volume type diffraction grating. The diffraction grating 44 is a substrate 4 made of a parallel plate.
It is sandwiched between 2 and 43 and is composed of a layer 50 having a low refractive index and a layer 51 having a high refractive index. Incident light 52 from the information recording surface is diffracted by this diffraction grating 44 to become diffracted light 53. When the diffraction grating 44 substantially satisfies the black condition for the incident light 52, most energy of the diffracted light 53 is concentrated in a specific diffraction direction. Further, when the angle formed by the incident light 52 and the diffracted light 53 is close to a right angle, the diffraction efficiency is greatly affected by the polarization state of the light beam, and the P-polarized light has a transmittance of 100% and the S-polarized light has a transmittance of 100%. It has a close diffraction efficiency. Therefore, by making the light traveling from the laser light source 31 toward the information recording surface 37 into the linearly polarized light of P polarization in the configuration as shown in FIG. 1, this light is transmitted with almost no influence by the light splitter 41 and has a wavelength of λ / 4. Due to the function of the plate 34, the reflected light from the information recording surface 37 becomes S-polarized light, is efficiently diffracted, and is guided to the photodetectors 39 and 40.

The diffraction grating 44 as shown in FIG. 4A is manufactured by using a volume hologram sensitizer such as dichromated gelatin. For example, the above-mentioned sensitive material is formed on the substrate to have a uniform thickness, and the light flux from the same laser is split on this, and then the interference fringes generated by overlapping at a predetermined angle are exposed,
Further development processing forms a diffraction grating. To manufacture a diffraction grating that diffracts a light beam in different directions as in the present invention, first, in the first step, a part of the photosensitive material is covered with a mask, and one interference fringe is exposed. Next, in a second step, this exposed portion is masked, and the interference fringes of different patterns are exposed by the light incident on the portion covered by the mask from an angle different from that in the first step. Finally, the mask is removed, and the interference fringes exposed in the first and second steps are processed by development. Further, even if the two sets of light fluxes are simultaneously irradiated to different portions of the photosensitive material without performing the baking twice as described above, the interference fringes of different patterns are exposed to a desired area by using an optical system at a time. It can also be baked.

FIG. 4B is a partial cross-sectional view showing another example of the structure of the optical splitter 41 used in the present invention. The diffraction grating 44 has a shape in which a reflection film 60 having an appropriate reflection characteristic, for example, a polarization beam splitter characteristic is sandwiched by layers 54 and 55 having unevenness and having substantially the same refractive index. Therefore, for the linearly polarized light 56 that is incident as P-polarized light, the diffraction grating 44 behaves as a simple parallel plate without any action, and for the linearly polarized light 57 that is incident as S-polarized light, it acts as a reflecting mirror. Diffracted light 58 is produced.

The diffraction grating 44 as shown in FIG. 4B can be produced by exposing a relief type photosensitive material such as a photoresist to a grating pattern through an appropriate optical system and developing it. In addition, it can also be produced by a method of mechanically processing a die and transferring it to a layer to be a substrate by a method such as injection, compression, thin layer copy, or a method of directly cutting the substrate.

In the embodiment shown in FIG. 2, the diffracted light from the diffraction grating 44 is converged and diffracted, and the diffraction grating which produces a lens action in this way is, for example, as shown in FIG. This can be realized by making the lattice into a conical shape in the structure as in b). When an optical means is used for producing the diffraction grating 44, a focusing action can be provided by an optical system as shown in FIG. In FIG. 5, parallel light beams 61 and 62 emitted from the same laser light source and divided by an optical system (not shown) are incident on conical mirrors 63 and 64 sharing a rotation axis 65 in parallel with the rotation axis 65. The two light beams reflected by the respective conical mirrors become a conical wavefront having a focal line on the rotation axis 65 and enter the hologram photosensitive material 67 on the substrate 66. At this time, the interference fringes generated in the area 68 on the photosensitive material surface are three-dimensionally conical with the rotation axis 65 as the center of rotation. Therefore, by developing the interference fringes thus exposed, a diffraction grating having a focusing action as shown in FIG. 2 is formed.

Although the first embodiment has been described above, the present invention is not limited to this, and various modifications can be made depending on the configuration of the split surface of the optical splitter. An example is shown below. All of the following embodiments will be described with reference to a view of the light splitter from the light source side, and optical elements other than the light splitter are not shown, but they are configured similarly to the embodiment shown in FIG.

FIG. 6 is a diagram showing an optical splitter used in the second embodiment of the present invention. In the present embodiment, two diffracted lights guided to different end faces of the light splitter in the first embodiment are detected by the end faces on the same side, and the same members as those in FIG. Reference numerals are given and detailed description is omitted. Here, the diffraction grating 74 forming the dividing surface of the optical splitter 71 is divided into two areas having different grating patterns with a line segment AA ′ corresponding to the track extending direction of the information recording surface as a boundary. Each of the frame gratings 74a and 74b focuses the reflected light from the information recording surface and diffracts it to different positions on one end surface of the light splitter 71, and guides it to the photodetectors 40 and 39, respectively. By processing the output signal of this photodetector in exactly the same manner as described in FIGS. 2 and 3, the focus error signal I _F , the tracking error signal I _T , and the information reproduction signal I _RF can be obtained. In this embodiment, since the photodetectors can be concentrated on one side of the light splitter, there is an advantage that the optical head device can be further downsized as compared with the first embodiment.

FIG. 7 is a diagram showing an optical splitter used in the third embodiment of the present invention. The diffraction grating formed on the light splitter 81 is manufactured by the same method as that of the above-described embodiment and divided into the piece gratings 82 and 83. Each piece lattice 82, 83
Is formed with a lens action so that the diffracted light forms a focal line in a predetermined direction, and guides each diffracted light to the 4-division photodetector 80 formed on one end face of the light splitter. Here, the direction of the focal line of the frame grating 82 coincides with the direction AA 'of the track image on the information recording surface. The outputs I _A , I _B , I _C , and I _D from the respective light-receiving surfaces of the four-division photodetector 80 are appropriately processed by a calculator (not shown) to generate various signals necessary for the optical head device. You can get it. For example, the information reproduction signal I _RF is the sum of the output obtained from the _{I RF = I A + I B} + I C + I D. Further, the focus error signal I _F is obtained by detecting the shake and spread in the plane of the paper of FIG. 7 of the light beam split by the frame grating 83 substantially at the pupil plane position of the objective lens. The position of the frame grating 83 and the diffraction direction of the light diffracted by this can be arbitrarily prepared as described above, and the photodetector 80 may be arranged anywhere, but as shown in FIG. The focusing error signal I _F can be detected with high sensitivity by arranging so that the change of the diffracted light is large in the division direction of the surface. Output I _A of the light receiving surface in particular, by taking the difference between I _B, obtained as I _F = I _A -I _B. Since the tracking error signal I _T is obtained from the light amount distribution in the reflected light beam from the information recording surface, it is obtained from the light amount difference of the light beams divided by the focal line of the frame grating 82 which coincides with the direction AA ′ of the track image. Actually 4
By calculating the output from the light receiving surface of each of the photodetector 80 is determined as _{I T = I A + I B} + I C -I D.

With the light flux control signals (focus error signal, tracking error signal) obtained as described above, the optical head device is controlled so that a desired light flux is incident on the information recording surface to detect or record information. It can be done reliably. Incidentally, in the embodiment shown in FIG.
Although the structure of the diffraction grating can be arbitrarily set as described above, it is not particularly shown, but a 4-division photodetector is a combination of 2-division photodetectors or a 2-division photodetector and a light receiving surface whose light is not divided. It is also possible to replace the combination with a detector or the like. Further, it goes without saying that the position of the piece lattice 83 can be set to any position within the lattice plane.

FIG. 8 shows an optical splitter used in the fourth embodiment of the present invention. In this embodiment, the optical splitter 91 is provided with a frame grating 93 for detecting a focus error signal as in the case of the third embodiment, and the other portion is a dividing line whose direction coincides with the track image direction AA '. Is further divided to form piece lattices 92a and 92b, respectively. The light diffracted or reflected by the frame grating 93 is guided to the two-split photodetector 95. Further, the two light beams diffracted or reflected by the frame gratings 92a and 92b are guided in the focal line direction by the respective gratings in the light splitter, and are guided to the corresponding photodetectors 97 and 96, respectively. The output of each light receiving surface of the two-division photodetector 95 is I
_A, I _B, the output of the photodetector 96 I _C, when the output of the photodetector 97 and I _D, by these not shown calculator,
The focus error signal, the tracking error signal, and the information reproduction signal can be obtained by performing the same processing as in the third embodiment. In the present embodiment, the light from the information recording surface is divided by the frame gratings 92a and 92b along the dividing line that coincides with the direction of the track image, and is guided to different photodetectors. It is possible to detect the tracking error signal more reliably by dividing and detecting the light amount distribution of the above at about the pupil plane position of the objective lens.

FIG. 9 is a diagram showing an optical splitter used in the fifth embodiment of the present invention. In this embodiment, the optical splitter 101
The upper diffraction grating is divided into piece gratings 102, 103 and 104, and has a shape just like that in which the piece grating 104 is added to the configuration of the third embodiment. The light beams diffracted or reflected by the frame gratings 102 and 103 are detected by the four-division photodetector 100, and the light beams diffracted or reflected by the frame grating 104 are detected by the photodetector 105. In this embodiment, as described above, by compensating for the symmetry with the direction AA ′ of the track image of the light flux in the frame grating 82 as the axis of symmetry, it is possible to simplify the arithmetic processing of the signals after the photodetector. .. Specifically, if the outputs from the divided light receiving surfaces of the four-division photodetector 100 are I _A , I _B , I _C , and I _{D, respectively,} and the output of the photodetector 105 is I _E , the information reproduction signal I _RF is obtained as _{I RF = I a + I B} + I C + I D + I E. Further, the focus error signal I _F is obtained as the difference between I _A and I _B such that I _F = I _A −I _B. The tracking error signal I _T is simply obtained as the difference between the output signals I _C and I _D of the photodetector 100 by adding the frame grating 104.

I _T = I _C -I _D

Further, in the embodiment, the photodetector 105
It is also possible to eliminate the above and obtain the information reproduction signal I _RF as I _RF = I _A + I _B + I _C + I _D. In this case, the light beam diffracted or reflected by the frame grating 104 may be reflected and scattered at the end surface of the light splitter 101 to generate stray light.
A light absorber may be installed at a position where the photodetector 105 is removed. In this embodiment as well, modifications such as replacement of the photodetector as described in the third embodiment are possible.

FIG. 10 is a diagram showing an optical splitter used in the sixth embodiment of the present invention. In this embodiment, the optical splitter 11
The diffraction grating on 1 is divided into piece gratings 112a, 112b, 113, and each piece grating diffracts or reflects a light beam while converging a light beam so as to form a focal line in a different direction. Piece lattice 1
The light flux from 13 is guided in the light splitter and detected by the two-split photodetector 114. The dividing line between the frame gratings 112a and 112b coincides with the track image direction AA ', and the respective diffracted lights are detected by the photodetectors 115 and 116. Assuming that the outputs of the respective light receiving surfaces of the two-division photodetector 114 are I _A and I _B , the output of the photodetector 115 is I _C , and the output of the photodetector 116 is I _D , the information reproduction signal I _RF is these outputs. , I _RF = I _A + I _B + I _C + I _D Further, the focus error signal I _F is obtained by detecting the shake and spread on the light receiving surface of the photodetector 114 of the light beam divided by the frame grating 113 substantially at the pupil plane position of the objective lens. The position and the diffraction direction of the frame grating can be arbitrarily produced as described in the third embodiment, and the optimum design capable of highly sensitive detection is made. Specifically 2
By taking the difference between the two output signals of the split photodetector, I _F = I _A −I _B is obtained. The tracking error signal I _T is divided by the frame grating 112 divided by the direction AA ′ of the track image.
a, 112b corresponding to the amount of light from the photodetectors 116, 1
It is obtained by detecting at 15 and taking the difference between the output signals.

I _T = I _C -I _D

In this embodiment, the photo detectors 115 and 116 are used.
Can be replaced with a single 2-split photodetector,
Further, the photodetectors 114, 115 and 116 may be combined into a four-division photodetector.

FIG. 11 is a diagram showing an optical splitter used in the seventh embodiment of the present invention. In this embodiment, the case where the direction AA ′ of the track image makes an arbitrary angle θ with the light splitter 121 is shown. Here, the diffraction grating of the light splitter 121 is
It is divided into frame gratings 122a, 112b, 123, 124, and diffracts or reflects the light flux while converging the light flux so as to form focal lines in different directions. Piece grid 122a, 122
The line dividing b coincides with the direction AA 'of the track image,
The piece lattices 123, 124 are manufactured at positions symmetrical with respect to the dividing line as the axis of symmetry. Piece grids 122a and 122
The light beam diffracted or reflected by b is guided to each light receiving surface of the two-divided photodetector 126. The luminous flux from the piece lattice 123 is 2
It is detected by the split photodetector 125. Also, the piece lattice 124
The light flux from is absorbed by the light absorber 127. The outputs of the respective light receiving surfaces of the two-division photodetector 125 are I _A , I _B , and 2
When the outputs of the light receiving surfaces of the divided photodetector 126 are I _C and I _D , the information reproduction signal I _RF , the focus error signal I _F , and the tracking error signal I _T are output by the calculator (not shown). It can be obtained by the same arithmetic processing as in the sixth embodiment.

In this embodiment, the piece gratings 124a and 122a are used for detecting the tracking error signal.
It is provided in order to compensate for the symmetry of the two light beams divided by b, and plays the same role as the frame grating 104 in FIG. Therefore, replacing the light absorber 127 with a photodetector,
In the same process as the fifth embodiment shown in FIG. 9, an information reproduction signal,
The light flux control signal may be obtained. Further, a configuration in which the frame grating 124 is removed in the present embodiment and the above-mentioned compensation is performed by the arithmetic processing after the photodetector as in the fourth embodiment shown in FIG. 8 can be considered.

Although various examples of the configuration of the optical splitter have been shown above, the present invention can be modified such that another optical splitter is used or the configuration other than the optical splitter is different. .. For example, when reading a magneto-optical recording, the λ / 4 plate 34 is removed in the configuration shown in FIG.
Detection can be performed by placing a polarizing plate immediately before 9, 40 or replacing the λ / 4 plate 34 with a Faraday element. In the embodiment, the light beam from the light splitter is directly guided to the photodetector, but the light beam is sent to the photodetector through an appropriate optical system by processing a cylindrical lens on the end face of the light splitter. You may guide me.

[0037]

As described above, according to the present invention, in the conventional optical head device, the plurality of regions for guiding the reflected light to the different light receiving surfaces are provided on the dividing surface of the optical splitter for dividing the reflected light from the information recording surface. By providing it, the position of the photodetector can be easily adjusted, and the light incident on the information recording surface is not affected,
It is expensive because the reflected light can be partially extracted to the photodetector.

[Brief description of drawings]

FIG. 1 is a schematic configuration diagram showing an embodiment of an optical head device according to the present invention.

FIG. 2 is a view of the light splitter of the apparatus shown in FIG. 1 viewed from the light source side.

FIG. 3 is a diagram illustrating a principle of detecting a focus error signal in the device shown in FIG.

FIG. 4 is a schematic cross-sectional view showing a configuration example of a diffraction grating used in the present invention.

FIG. 5 is a diagram illustrating an example of a method of forming a diffraction grating.

FIG. 6 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 7 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 8 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 9 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 10 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 11 is a diagram showing a configuration of an optical splitter used in another embodiment of the present invention.

FIG. 12 is a schematic diagram showing a configuration of a conventional optical head device.

FIG. 13 is a schematic diagram showing a configuration of a conventional optical head device.

[Explanation of symbols]

 31 laser light source 32 collimator lens 34 λ / 4 plate 35 objective lens 36 substrate 37 information recording surface 39 photodetector 40 photodetector 41 light splitter 42 substrate made of parallel flat plate 43 substrate made of parallel flat plate 44 diffraction grating

 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Kiyonobu Endo 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Tetsuro Kuwayama 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Incorporated (72) Inventor Osawa Dai 3-30-2 Shimomaruko, Ota-ku, Tokyo Canon Inc. (72) Inventor Yasuo Nakamura 1248 Shimokagemori, Chichibu-shi, Saitama Canon Electronics Inc.

Claims (2)

[Claims] 1. A light detector which irradiates the information recording surface with light emitted from a light source, and uses a light splitter arranged in an optical path from the light source to the information recording surface to detect reflected light from the information recording surface. In the optical head device for guiding to the light receiving surface and detecting or recording information, the split surface of the light splitter has a plurality of regions for respectively guiding the reflected light to different light receiving surfaces. .. 2. The optical head device according to claim 1, wherein the division surface of the optical divider is a diffraction grating having a plurality of frame gratings in which mutually different grating patterns are formed.