Optical head

Abstract: An optical head in which reflected laser light is split into two optical paths by a polarized light beam splitter (23) while astigmatisms are produced in the laser light by at least one astigmatism generating element (22), and the two split beams are led so as to be incident upon two quadrant photodetectors, respectively. A focus error signal is obtained as an electrical signal by subtracting the sum of the quantities of light received by one of the diagonal pairs of regions among the quadrant regions of the two photodetectors (24, 25) from the sum of the quantities of light received by the other diagonal pair. This arrangement enables cancelling of influence of double refraction in a magneto-optic disk or the like, thereby making the optical head free of the problem of such influence.

Description: BACKGROUND OF THE INVENTION FIELD OF THE INVENTION This invention relates to an optical head for recording, reproducing or erasing information by means of a laser beam and, more particularly, to a focusing servo device for controlling a spot of a laser beam by adjusting a position of an objective lens by means of the reflected laser beam. RELATED ART As optical recording mediums, a laser vision disk (LVD), a digital audio disk (DAD), a compact disk read only memory (CD-ROM) and a photo-magnetic disk memory are conventionally known. An optical head is used for reading information from these disks and writing information onto these disks. The optical head emits a laser beam to read information recorded on a disk and write information onto the disk. The laser beam must be emitted accurately onto the information recording surface of the disk. To this end, the optical head is usually controlled by a focusing servo device and a tracking servo device. A conventional focusing servo device converts a beam reflected by the information recording surface of the disk into electric signals and controls an actuator for focusing operation so that focus error signals among the electric signals become naught. As a method of the focusing servo operation, a method utilizing astigmatism is known. In EP-A-0,218,250, a focusing servo device is disclosed which adopts this method and comprises a cylindrical lens for generating astigmatism and a quadrant type photodetector. The cylindrical lens generates two elliptic light spots on an optical path. The quadrant photodetector is disposed in such a manner that its light receiving surface divided into four regions or sections is located at a predetermined position where a truly circular light spot of the laser beam is reflected on the light receiving surface when the laser beam is focused correctly on the disk. If the quadrant photodetector is disposed at a position deviated forward or backward from the predetermined position, an elliptic light spot is formed. In case that the focal point of a laser beam is deviated from a pit of the disk along its optical axis, an elliptic light spot is formed in the direction of a diagonal line passing through the first and third regions or the second and fourth regions. The photodetector provides an electric output corresponding to a difference in quantity of received light between two regions forming one diagonal pair and two regions forming the other diagonal pair. In this case, if the difference in quantity of received light is not zero, the focal point does not coincide with the reflecting surface of a pit of the disk. A focusing servo operation is performed so that the difference in quantity of received light becomes naught. The accuracy of the focusing servo operation has a connection with the optical property of material of a substrate with which the recording surface of the disk is covered. As a material of a disk substrate, glass or polymethyl methacrylate resin (PMMA) is often used in view of its optical property such as transparency. However, in view of cost and mass-production, it is considered that polycarbonate resin is used. Polycarbonate resin has a high double refractive index as an optical property. If the material of a disk substrate has a high double refractive index, the material has the following bad effect upon the focusing servo operation. That is, a laser beam is converged in the shape of a cone while passing through the substrate of the disk. At this time, rays near its optical axis enter perpendicularly the recording surface of the disk, and, however, rays at an outer periphery of bundle of rays center there with a large incident angle. In this case, if polycarbonate resin having a high double refractive index is used for a substrate with which the recording surface of the disk is covered, the rays at outer periphery are refracted double at an incident point and a reflecting point. This double refraction causes a phenomenon that the phase of the rays at the periphery of the bundle of rays is delayed in comparison with rays near the center portion of its optical axis. This phenomenon is called "Retardation". As a result, rays at a periphery of bundle of rays are elliptically polarized. There appear some uneven parts each having a high intensity of light at a periphery of a light spot formed on the light receiving surface of the photodetector due to the elliptic polarization of light. If there appear a few of high intensity parts at two divided regions (e.g. two cells of the first and third quadrants), this causes a state wherein there is a difference in quantity of received light between two diagonal pairs of regions of the photodetector irrespective of a good focusing. With this state, the focal point of an objective lens is moved needlessly, and focusing servo does not operate in case of need. SUMMARY OF THE INVENTION It is an object of the present invention to provide an optical head with a focus control which can be effected without influence by double refraction as a result of the substrate material of a disk. To achieve this object, the present invention provides an optical head for effecting recording/reproduction of information by irradiating a recording medium with laser light, comprising the features set out in claim 1. The optical head of the present invention is characterised in that the polarization axis of the linearly polarized light and the incident surface of the polarized light beam splitter are disposed at an angle of 45° relative to each other. Further, the operation means obtains for each quadrant photodetector and with respect to one astigmatism a differential output between a sum output from one pair of light receiving regions where an intensity of received light is increased brought about when retardation of the light rays at the periphery of the bundle of rays entering the surface of the recording medium occurs due to double refraction of the surface material, and a sum output from the other pair of light receiving regions where an intensity of received light is not changed when the rays of light at a centre portion of said bundle enter perpendicular to the surface. The differential output obtained is processed to obtain the focusing error signal. The nature, utility, and further features of this invention will be made more apparent from the following detailed description with respect to preferred embodiments of the invention when read in conjuction with the accompanying drawings briefly described below. BRIEF DESCRIPTION OF THE DRAWINGS In the accompanying drawings: FIG. 1 is a view showing an embodiment of an optical head according to this invention; FIG. 2 is a schematic view showing a positional relationship between some elements of an optical system in an embodiment of an optical head according to this invention; FIG. 3 is a view showing a state of light spots formed on the light receiving surface of a first quadrant photodetector; FIG. 4 is a view showing a construction of an optical head of another embodiment according to this invention; FIG. 5 is a schematic view showing an elliptic polarization at a periphery of bundle of rays; FIG. 6 is a view showing an uneveness of distribution of intensity of light on the light receiving surface of the quadrant photodetector; FIG. 7 is a view showing an embodiment of operation system of an optical head according to this invention; and FIG. 8 and 9 are two views of circuits showing an operation system of an optical head according to this invention, respectively. DESCRIPTION OF THE PREFERRED EMBODIMENT FIG. 1 is a schematic view showing an embodiment of a focusing servo device F according to this invention. The focusing servo device F comprises a light irradiation system 1 for irradiating the recording surface D b of a disk D with a laser beam so as to form a spot (referred to as an information reading light spot hereunder) on the recording surface D b , a detection system 2 for converting reflected light from the disk D into electric signals, an operation system 3 for picking up a focus error signal for a focusing servo operation and tracking error signal for tracking servo operation from electric signals transmitted from the detection system 2, a driving system 4 for adjusting a position and an inclination of an objective lens in response to a focus error signal and a tracking error signal. Light Irradiation System First, the construction of the light irradiation system 1 will now be explained. The light irradiation system 1 has a semiconductor laser 11 as a laser light source. A collimator lens 12 is provided in the optical path of laser light emitted from the semiconductor laser. The collimator lens 12 converts diffused light into a bundle of parallel rays. An objective lens 15 is provided opposite to the disk D. The objective lens 15 converges the bundle of parallel rays to focus it on the recording surface Db of the disk D. A first polarizing beam splitter 13 (referred to as a PBS hereunder) is disposed in the optical path between the collimator lens 12 and the objective lens 15. The PBS has a function to separate rays having a specific plane of polarization from the bundle of rays at a certain separation rate. In the optical path between the first PBS 13 and the objective lens 15 is provided a quarter-wave plate for shifting the phase of the laser beam by a quarter-wave length. The light irradiation system 1 will now be explained. The semiconductor laser 11 emits laser light linearly polarized. The emitted laser light is diffused light which is converted by the collimator lens 12 into a bundle of parallel rays. The bundle of parallel rays passes through the first PBS 13. After this, the quater-wave plate 14 generates a difference of optical path of a quater-wave length between two linearly polarized lights whose planes of polarization are disposed perpendicular to each other. The objective lens 15 converges the laser beam of bundle of parallel rays to form a light spot for reading information from the disk D on the recording surface D b of the disk D. The information reading spot light is reflected by the recording surface of the disk D. The objective lens 15 converts the laser light having been reflected and returned therefrom into a bundle of parallel rays which then passes through the quarter-wave plate 14 again. Therefore, at this time, there is a difference of optical path, corresponding to a half-wave length between two linearly polarized lights of the reflected laser light, whose planes of polarization are disposed perpendicular to each other. That is, at this time, the plane of polarization of the reflected laser light is rotated by 90 degrees from the plane of polarization at the incident time. The reflected light enters the first PBS 13 again and is directed toward other optical path to lead it to the detection system 2 by the first PBS 13 because of its different plane of polarization. Detection System The detection system 2 has a detecting lens 21 for converging the reflected laser light. In the optical path between the detecting lens 21 and its focal point is provided an astigmatism generating means 22 for obtaining two elliptic light spots in its light path from the reflected light which has passed through the astigmatism generating means 22 such as a cylindrical lens, a slanted plane-parallel plate or a deformed prism. In the optical path between the detecting lens 21 and two elliptic light spots is provided a second PBS 23 which is disposed obliquely at an angle of 45 degrees with respect to the linearly polarized light of the reflected light to divide equally bundle of rays of the reflected light into a first detecting light path and a second detecting bundle. Instead of this, the whole detecting system 2 may be slanted at an angle of 45 degrees with respect to the linearly polarized light of the reflected light. Further, the optical axis of a half-wave plate may be disposed obliquely at an angle of 22.5 degrees with respect to the incident surface of the first PBS 13 between the detecting system 2 and the first PBS 13. A first quadrant photodetector 24 is disposed in a predetermined position where a cross section of bundle of rays forms an exact circle on its light receiving surface when the laser beam is focused correctly. A second quadrant photodetector 25 is disposed in a mirror image position, in the second detecting light path, where the reflected light by the second PBS 23 forms a mirror image. Next, the operation of the detection system 2 will now be explained. The bundle of parallel rays reflected by the disk D is converged by the detecting lens 21 and passes through the astigmatism generating means 22. The second PBS 23 permits a half part of the reflected light having been converged to pass through itself to provide a first detecting optical path because of difference of planes of polarization of the reflected light while the remaining half part thereof is reflected by the PBS 23 to provide a second detecting optical path. If the distance between the objective lens 15 and the recording surface of the disk D is not changed, that is, the laser beam is focused exactly on the recording surface D b , the reflected light forms two truly circular light spots on the light receiving surfaces of the first and second optical detectors, respectively. However, if the distance therebetween is changed by some reason to cause the focal point of the laser light to be deviated from the recording surface Db of the disk D, two elliptic light spots are respectively formed on the light receiving surfaces of the first and second quadrant photodetectors 24, 25 under the influence of the astigmatism. FIG. 2 is a view showing a positional relationship between the light receiving surfaces of the first and second PBSs 13, 23 and the first and second quadrant photodetectors 24, 25. As shown in FIG. 2, a dividing line ℓd₁ of the light receiving surface of the quadrant photodetector 24 and a dividing line ℓd₂ of the light receiving surface of the quadrant photodetector 25 coincide optically with the track extending direction of the disk D. When the focal point of the laser light is deviated from the recording surface D b of the disk D, a light spot having a deformed elliptic shape whose apse line coincides with a diagonal line passing through two regions or quadrants disposed diagonally on the light receiving surface of each of quadrant photodetectors 24, 25. That is, a light spot whose apse line extends diagonally in the second and fourth quadrants 24a, 24c is formed on the light receiving surface of the first quadrant photodetector 24 while a light spot whose apse line extends diagonally in the first and third quadrants 25a, 25c. Therefore, the apse line of the first quadrant photodetector 24 is located symmetrically with that of the second quadrant photodetector 25 with respect to a dividing line of a light receiving surface. That is, the apse line of the deformed ellipse formed on the first photodetector 24 is perpendicular to the apse line of the deformed ellipse formed on the second photodetector 25. FIG. 3 shows states of light spots formed on the light receiving surfaces of the first and second quadrant photodetectors 24, 25, respectively. FIG. 3a shows a state wherein the objective lens 15 is located too close to the disk D. FIG. 3b shows a state wherein the focal point of the laser light coincides with the recording surface D b of the disk D. FIG. 3c shows a state wherein the objective lens 15 is located too far from the recording surface D b of the disk D. As shown in FIG. 3b, if the focal point is on the recording surface D b of the disk D, a light spot S o is formed on the light receiving surface of each of two photodetectors 24, 25. If the focal point is deviated from the recording surface of the disk D, for example, the objective lens 15 is located too close to the disk D, an elliptic light spot S₁ is formed on the light receiving surface of each of quadrant light detectors 24, 25. If the objective lens 15 is located too far from the disk D, an elliptic light spot S₂ whose apse line is perpendicular to that of the elliptic light spot S1 is formed on the light receiving surface of each of quadrant light detectors 24, 25. If the astigmatism generating means 22 is disposed so as to change its angle with respect to the optical axis, the disposition of the light spots S₁, S₂ can be reversed to the state shown in FIG. 3. That is, in this case, if the objective lens 15 is located too close to the disk D, an elliptic light spot is formed in the same manner as that of the light spot S₂ on the light receiving surface of each of detectors 24, 25. However, if the objective lens 15 is located too far from the disk D, it is possible that an elliptic light spot such as the elliptic light spot S₁ is formed thereon. Instead of the astigmatism generating means 22, two astigmatism generating means 26, 27 may be, as shown in FIG. 4, disposed symmetrically with respect to the PBS 23 midway of the first and second detection optical paths, respectively. If a material having a large double refraction such as polycarbonate resin is used for the substrate of the disk D, two uneven portions N, N result, each having a higher intensity of light in comparison with the other remaining regions of the photodetector, as can be seen from Figs. 3(a)-3(c). The reason for this phenomenon will be explained. Laser light is converged to the surface of the disk D in the shape of a cone. Therefore, the rays enters perpendicular to the substrate at a center portion of the bundle of rays while the rays enters the substrate at a periphery of the bundle of rays with a relatively large incident angle. Accordingly, the rays at the periphery of the bundle of rays are influenced by retardation (delay of phase) to cause the rays at the periphery of the bundle of rays to be elliptically polarized as shown in FIG. 5. In FIG. 5, the direction of linear polarization which is not rotated by magnetization on the recording surface at the time of recording information is indicated by an arrow, and two intensities of p-polarized light and s-polarized light correspond to two components in the directions of a line P and a line S in elliptic polarization and linear polarization, respectively. Accordingly, distribution of intensity on the light receiving surface of each of two photodetectors 24, 25 becomes uneven due to the component of the elliptic polarization thereby to generate two hatched portions in a pair of quadrants 24b, 24d disposed in one diagonal direction. Each of the two hatched portions has a larger amount of received light. Therefore, each of the pairs of quadrants 24b, 24d, 25a, 25c in the light receiving surfaces has a larger amount of light than that of each of the other pairs of quadrants 24a, 24c 25b, 25d as shown in FIG. 6. For this reason, even if the focal point of the objective lens 15 is located just on the recording surface D b of the disk D, the amount of the received light of the regions 24b, 24d, 25a, 25c is larger than that of the regions 24a, 24c, 25b, 25d. Therefore, the focusing servo operation is unnecessary performed. In contrast, even if the amount of received light of the diagonal regions 24a, 24c, 25b, 25d is larger than that of the other diagonal regions 24b, 24d, 25a, 25c, that is, even if the focusing servo operation is necessary, the focusing servo operation is not carried out. Operation System FIG. 7 shows a circuit of an operation system 3. The operation system 3 is electrically connected to the first and second quadrant photodetectors 24, 25. The operation system 3 comprises an addition circuit 301A as a first operation means, an addition circuit 302A as a second operation means, a subtraction circuit 303S as a third operation means, an addition circuit 304A as a fourth operation means, an addition circuit 305A as a fifth operation means, a substraction circuit 306S as a sixth operation means and an addition circuit 307A as a seventh operation means. The input terminals of the addition circuit 301A are connected to the two light receiving surfaces 24b, 24d of the first quadrant photodetector 24, disposed in one diagonal direction, respectively. The terminals of the addition circuit 302A are connected to the two light receiving circuit 24a, 24c of the first photodetector 24, in the other diagonal direction. The plus input terminal of the subtraction circuit 303S is connected to the output terminal of the addition circuit 301A while the minus input terminal of the substraction circuit 303S is connected to the output terminal of the addition circuit 302A. The input terminals of the addition circuit 304A are connected to the two light receiving surfaces 25b, 25d of the second quadrant light detector 25, disposed in one diagonal direction, respectively. The input terminals of the addition circuit 305A are connected to the two light receiving surfaces 25a, 25c of the second light detector 25, disposed in the other diagonal direction, respectively. The plus input terminal of the subtraction circuit 306S is connected to the output terminal of the addition circuit 304A while the minus input terminal of the subtraction circuit 306S is connected to the output terminal of the addition circuit 305A. Further, the input terminals of the addition circuit 307A are connected to the output terminal of the subtraction circuit 303S and the output terminal of the subtraction circuit 306S, respectively. The operation of this circuit system will now be explained. The addition circuit 301A calculates the total amount of light received by the light receiving surfaces 24b, 24d disposed in one diagonal direction to output a first signal. The addition circuit 302A calculates the total amount of light received by the light receiving surfaces 24a, 24c in the other diagonal direction to output a second signal. The subtraction circuit 303S as the third operation means subtracts the second signal from the first signal to output a third signal. The addition circuit 304A as the fourth operation means calculates the total amount of light received by the light receiving surfaces 25b, 25d of the second photodetector 25, disposed in one diagonal direction to output a fourth signal while the addition circuit 305A as the fifth operation means calculates the total amount of light received by the light receiving surfaces 25a, 25c thereof disposed in the other diagonal direction to output a fifth signal. The subtraction circuit 306S subtracts the fifth signal from the fourth signal to output a sixth signal. Thereafter, the addition circuit 307A as the seventh operation means adds together the third and sixth signals to output a focus error signal FE. If the focal point is on the recording surface D b , a truly circular light spot is formed on each light receiving surface and an amount of light received by each of four divided light receiving regions 24a, 24b,...24d is equal to each other. The second photodetector 25 has the state as that of the first photodetector 24. Therefore, at this time, the focus error signal becomes zero, that is, the focus error signal is not outputted. In case that the objective lens 15 is too close to the disk D, the focus error signal becomes a minus value. In case that the objective lens 15 is too far from the disk D, the focus error signal becomes a plus value. In this case, a pair of portions each having an uneven distribution of intensity of light, of the first photodetector 24 and a pair of portions each having an uneven distribution of intensity of light, of the second photodetector 25 are cancelled each other thereby to eliminate the influence by double refraction of the substrate of the disk. The characteristic feature of this invention resides in that the two quadrant type photodetectors are disposed so as to form mirror images with respect to the PBS 23 and the influence of double refraction is cancelled by an operation process. In the embodiment as shown in FIG. 7, two quadrant photodetectors are exclusively used as photodetectors for the focusing servo operation. However, in order to increase efficiency of the above systems, one of quadrant photodetectors may be utilized for picking up a tracking error signal TE and a magneto-optic reproduction signal RF as shown in FIG. 8. That is, an addition circuit 308A calculates a total amount of light received by the two adjacent light receiving regions 25b, 25c of the second photodetector 25. An addition circuit 309A calculates a total amount of light received by the other two light receiving regions 25a, 25d of the second light detector 25. A subtraction circuit 310S subtracts the output of the addition circuit 309A from the output of the addition circuit 308A to output a tracking error signal TE. In this case, the track of the disk D extends along the dividing line ℓd2 for dividing the light receiving surface of the second photodetector 25 into a pair of the light receiving regions 25b, 25c and a pair of the light receiving regions 25a, 25d. Therefore, when an incident beam is just on a recording track of the disk D, a light spot on the light receiving surface of the second photodetector 25 is divided into two equal semicircles by the dividing line ℓd2. When the incident beam is deviated from the track, the light spot is deviated from the dividing line ℓd2 in either side. When the focal point of the incident beam is just on the disk D and the light spot is just on the track, the tracking error signal becomes zero. When the light spot is deviated from the track, the tracking error signal becomes a plus or a minus value. In this case, since non-uniformity of the distribution of intensity of light on each light receiving surface is cancelled each other, the tracking error signal TE is not influenced by the double refraction of the substrate. An addition circuit 311A adds together the outputs of the addition circuits 301A, 302A. An addition circuit 312A adds together the outputs of the addition circuits 304A, 305A. Further, a subtraction circuit 313S subtracts the output of addition circuit 312A from the output of addition circuit 311A to output a magneto-optic reproduction signal RF. The operation system 3 may be assembled as shown in FIG.9. That is, when a focus error signal is calculated, an addition circuit 316A as an eighth operation means adds together the first signal as the output of the addition circuit 301A of the first operation means and the fourth signal as the output of the addition circuit 304A of the fourth operation means to output an eighth signal. In addition, an addition circuit 317A as a ninth operation means adds together the second signal as the output of the addition circuit 302A of the second operation means and the fifth signal as the output of the addition circuit 305A of the fifth operation means to output a ninth signal. Further, a subtraction circuit 318S subtracts the ninth signal from the eighth signal to output a focus error signal FE. In a case where the detection system 2 is shifted from the position at 45° to linearly polarized light, or in a case where there is certain non-uniformity of polarization film (substrate) characteristics or unevenness of the distribution of the sensitivity of each light receiving element, the outputs from the respective light receiving regions may be unbalanced, resulting in occurrence of an offset component in a focus error. For this reason, at least one of variable resistor means 314R. 315R. 319R, 320R as shown in FIGS. 7 to 9 may be provided to remove such an offset component at the time of calculation of the outputs from the respective light receiving regions. Driving System The driving system 4 has a driving means such as an actuator provided with a coil for changing the position, direction and angle of the objective lens and is electrically connected to the operation system 3. The focus error signal FE and the tracking error signal TE are transmitted to the driving system 4. The driving system 4 receives the focus error signal FE and the tracking error signal TE, and if each signal is not zero, the actuator is controlled so that each signal becomes zero by moving the position and angle of the objective lens 14 in order to adjust the distance between the objective lens 15 and the disk D and the position of the light spot for reading information with respect to the track of the disk D.

Claims: An optical head for effecting recording/reproduction of information by irradiating the surface of a recording medium with laser light, said optical heat comprising: a light irradiation means (1) having a light source (11) for irradiating the recording medium with laser light which is linearly polarized, and means for outputting light reflected by the recording medium; a converging means (21) for converging laser light output from said light irradiation means (1); a polarized light beam splitter (23) for splitting laser light reflected by the recording medium and leaving said converging means (21) into different optical paths according to the planes of polarization; first and second quadrant photodetectors (24,25) with four light receiving regions respectively disposed in the optical paths split by said polarized light beam splitter (23); an astigmatism generating means (22,26,27) for generating astigmatisms in the light led to said first and second quadrant photodetectors (24,25); and an operation means (3) for processing the outputs from the light receiving regions (24ad,25a-d) of said first and second photodetectors (24,25) to deliver a focusing error signal, characterised in that the polarization axis of the linearly polarized light and the incident surface of said polarized light beam splitter (23) are disposed at an angle of 45° relative to each other; and in that said operation means (3) obtains for each quadrant photodetector (24,25) and with respect to one astigmatism, a differential output between a sum output from one pair of said regions (24b,24d,25a,25c) where an intensity of received light is increased brought about when retardation of the light rays at the periphery of the bundle of rays entering the surface of the recording medium occurs due to double refraction of the surface material and a sum output from the other pair of said regions (24a,24c,25b,25d) where an intensity of received light is not changed when the rays of light at a centre portion of said bundle enter perpendicular to said surface, said differential output being processed to obtain said focusing error signal. An optical head according to claim 1, wherein said operation means includes: a first addition means (301A,305A) for obtaining, for each of said first and second quadrant photodetectors (24,25), a sum output from one pair of said regions (24b,24d,25a,25c) where an intensity of received light is increased brought about when said retardation occurs; a second addition means (302A,304A) for obtaining a sum output from the other pair of said regions (24b,24d,25a,25c) where an intensity of received light is not changed when said rays of light enter perpendicular to the surface; respective substraction means (303S,306S) for obtaining a difference between the outputs from said first and second addition means (301A,302A;304A,305A); and a third addition means (307A) for obtaining a sum of the outputs from said respective subtraction means (303S,306S) corresponding to said first and second photodetectors (24,25). An optical head according to claim 1, wherein said operation means includes: a first addition means (301A,304A) for obtaining for each of said first and second quadrant photodetectors (24,25) a sum output from one pair of said regions (24b,24d;25b,25d) where an intensity of received light is increased brought about when said retardation occurs; a second addition means (302A,305A) for obtaining for each of said first and second quadrant detectors (24,25) a sum output from the other pair of said regions (24a,24c;25a,25c) where an intensity of received light is not changed when said rays of light enter the surface perpendicularly; and a subtraction means (318S) for obtaining a differential output between sum outputs from each of said first (301A,304A) and second (302A,305A) additions means. An optical head according to claims 2 or 3, wherein said operation means includes at least one offset adjusting means in the form of a variable resistor means (314R,315R,319R,320R) at the input to said third addition means (307A) or at the input to said subtration means (318S). An optical head according to claim 1, wherein said astigmatism generating means (22) is disposed in an optical path of the laser light at a position before said polarized light beam splitter (23). An optical head according to claim 1, wherein said astigmatism generating means has a pair of elements (26,27) which are disposed in two optical paths split by said polarized light beam splitter (23). An optical head according to claim 1, wherein said astigmatism generating means comprises a cylindrical lens, a slanted plane-parallel plate or a shaped prism. An optical head according to claim 2, wherein said first addition means (301A,305A) adds together respective outputs from one pair of regions (24b,24d,25a,25c) arranged in one diagonal direction, of said first (24) or second quadrant photodetector (25) and said second addition means (302A,304A) adds together respective outputs from the other pair of regions (24a,24c;25b,25d), arranged in the direction perpendicular to said one diagonal direction, of said first (24) or second quadrant photodetector (25). An optical head according to claim 3, wherein said first addition means (301A,304A) adds together outputs from one pair of regions (24b,24d), arranged in one diagonal direction, of said first quadrant photodetector (24) and outputs from one pair of regions (25b,25d), arranged in the same direction as said one diagonal direction, of said second quadrant photodetector (25) and said second addition means (302A,305A) adds together outputs from the other pair of regions (24a,24c), arranged in the direction perpendicular to said one diagonal direction, of said first quadrant photodetector (24) and outputs from the other pair of regions (25a,25c), arranged in the direction perpendicular to said one diagonal direction, of said second quadrant photodetector (25). An optical head according to claim 1, wherein said operation means has a function to calculate a differential output between a sum output from two adjacent regions (25a,25d) on one side of a dividing line (ℓd₂) for dividing light receiving surface of one of photodetectors and a sum output from two adjacent regions (25b,25c) on the other side of the dividing line (ℓd₂) thereby to obtain a tracking error signal, said dividing line (ℓd₂) coinciding with a track extending direction of the disk.

Inventors: SATOH KATSUHARU PIONEER ELECTR, YANAGAWA NAOHARU PIONEER ELECT, SATOH, KATSUHARU, PIONEER ELECTRONIC CORP., YANAGAWA, NAOHARU, PIONEER ELECTRONIC CORP.
Applicants: PIONEER ELECTRONIC CORP, PIONEER ELECTRONIC CORPORATION
Application year: 1990
Main classification: G11B7
IPC codes: G11B7, G11B11