Optical Pickup Device Using Hologram Pattern and Hologram Pattern Generating Method

专利摘要:
In an optical pickup apparatus of a type in which light from a single true laser light source 11 is diffracted and separated into a plurality of light spots focused on a plurality of tracks of an optical disc for simultaneous reading of data on a track by the hologram module 13. Astigmatism and coma aberration are suppressed in. The non-diffractive hologram pattern 14 and the diffractive hologram patterns 15a, 15b, and 15c of the hologram module 13 allow the light diffracted by the hologram module to be transmitted to the optical element in the optical path from the laser light source 11 to the optical disk. It is determined to give inverse aberration as caused by The other hologram pattern 14 provides a light spot of uniform intensity formed by the laser by the optical element.
公开号:KR20010086251A
申请号:KR1020007008939
申请日:1999-02-12
公开日:2001-09-10
发明作者:타카요시 히라가；히로시 미야자와；토루 신조우
申请人:오카 마코토；가부시키가이샤 캔우드；
IPC主号:

专利说明:

Optical pickup device using hologram pattern and hologram pattern generating method
[3] 2. Related Technical Description
[4] In one of the methods of simultaneously reading data recorded on a plurality of tracks of a recording medium such as an optical disc, the light is emitted from the optical pickup apparatus and focused on each track of the recording medium and reflected from the tracks. Is detected with each photodetector. Methods for forming a plurality of light spots as shown in FIGS. 7 and 8 are known. The basis of these methods will be described in detail with reference to Figs. 7 and 8 and like elements in the following embodiments will be represented using the same reference numerals. In the method shown in Fig. 7, a semiconductor laser array 60 having the same number of semiconductor lasers as the required number of light spots is used to emit light from the light sources 61a, 61b, 61c, 61d of the semiconductor laser. In the method shown in FIG. 8, a single semiconductor laser 10 is used. The light emitted from the true laser light source 11 of the semiconductor laser 10 (the term " calm " was used to distinguish it from the " virtual " laser light sources 21a, 12b and 12c which will be described later) is shown in FIG. It is separated into a plurality of light beams by a diffraction grating 64 which acts to radiate from the light sources 61a, 61b, 61c, 61d of the semiconductor array 60 shown.
[5] However, the method shown in FIG. 7 using the semiconductor array 60 has the following related problems: (a) Since a plurality of semiconductor lasers are assembled into one package or chip, it is possible to reduce the dimensions of the semiconductor laser array. There is a limit; (b) the number of connecting terminals is increased; (c) it is difficult to make the array compact because the surface area of the array needs to be large to allow heat dissipation; (d) Since a plurality of semiconductor lasers with uniform performance are required, manufacturing yield and cost are not good.
[6] Although only a single semiconductor laser can reduce the unit cost using the diffraction grating 64, it is necessary to mount the diffraction grating 64 as close to the semiconductor laser as possible in order to make the optical pickup device compact. In this case, the diffraction grating is mounted very close to the semiconductor laser, and between the light beam incident from the true laser light source 11 into the diffraction grating 64 and the diffracted light beam emitted from the diffraction grating 64 (θ1> θ2). The angle θ of is closer. Therefore, the astigmatism and coma aberration of the light spot become large, which increases the diameter of the light spots 25a, 25b, and 25c and increases jitter in the reproduced signal.
[1] 1. Field of Invention
[2] BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical pickup apparatus for recording and reading out a recording medium such as an optical disc or an optical card, and more particularly, to a multi-beam optical pickup apparatus capable of simultaneously forming optical spots on a plurality of tracks of the recording medium. .
[23] 1 is a diagram showing the configuration of an optical pickup apparatus.
[24] FIG. 2 is an enlarged view of a portion of the optical pickup device shown in FIG. 1 from the semiconductor laser to the hologram module.
[25] 3 is a schematic diagram illustrating a diffraction hologram pattern.
[26] 4 is a diagram illustrating a method of determining each diffractive hologram pattern using optical elements.
[27] FIG. 5 is a diagram illustrating a method of forming a plurality of light sources having characteristics consistent with a true light source using the pinhole member in the half mirror position shown in FIG. 4.
[28] 6A-6C are graphs and diagrams illustrating a method of improving tracking servo light spots.
[29] 7 is a diagram showing the configuration of a conventional optical pickup apparatus for forming a plurality of light spots using a semiconductor laser array.
[30] 8 is a diagram showing the configuration of a conventional optical pickup apparatus for forming a plurality of light spots using a semiconductor laser array.
[31] FIG. 9 shows the angle θ between the light beam incident from the true light source into the diffraction grating and the diffracted light beam emitted from the diffraction grating arranged at some distance from the semiconductor laser of the optical pickup device shown in FIG. 8. One diagram.
[7] Summary of the Invention
[8] It is an object of the present invention to solve the above problems associated with a conventional optical pickup apparatus of the type in which a plurality of light spots are formed using diffraction of light emitted from a single true light source.
[9] An optical pickup apparatus of the present invention comprises: (a) a single true light source; (b) a hologram member for diffracted light emitted from the true laser light source to form at least one virtual laser light source; (c) a light spot forming optical element for receiving light from the hologram member and forming a plurality of light spots on the tracks of the recording medium. In the optical pickup apparatus, the hologram pattern of the hologram member is determined so that the diffracted light causes aberration and reverse aberration in the optical path from the true laser light source to the recording medium by the optical element.
[10] The light spot forming the optical element includes optical elements such as plate-shaped Fresnel bodies with uniform thickness as well as optical elements such as lenses having different thicknesses in the central and peripheral regions. The recording medium also includes an optical disc and a card capable of recording and reading data. Aberrations include astigmatism and coma.
[11] The tracks of the recording medium on which the plurality of light spots are formed are discontinuous tracks or continuous tracks. That is, the track of the recording medium may be a plurality of concentric tracks or one spiral track.
[12] The aberration caused by the optical element in the optical path from the true laser light source to the recording medium may be aberration caused by all optical elements or some optical elements. The hologram pattern of the hologram member is determined so that the diffracted light causes an aberration and reverse aberration in the optical path from the true laser light source to the recording medium by the optical element.
[13] The hologram pattern does not always need to completely eliminate the aberration caused by the optical element, but an optical spot in which data reading is appropriate sometimes has some aberration. In this case, the hologram pattern is designed such that the amount of the predetermined intrinsic aberration remains reliably without being completely eliminated, or the amount of the predetermined inherent aberration with the negative sign of the intrinsic aberration is intentionally formed. Obviously, the effect of reducing the aberration of the light spot on the recording medium is more aberration caused by all the optical elements in the optical path from the true laser light source to the recording medium than the hologram pattern giving the aberration caused by some optical elements. It is large for the hologram pattern of the hologram, which is a diffracted light that gives.
[14] The hologram pattern is an amplitude hologram pattern with contrast disturbing fringes or a phase hologram pattern with binary (stepped cross section) or saw blade (saw blade cross section) grooves. The hologram member generates at least one virtual laser light source. All of the plurality of virtual light sources may be generated on one or both sides of the true laser light source. In general, although a light spot formed on a track of a recording medium is used to detect reflected light and read data on the track, it may be used to record data.
[15] The aberration caused by the optical element from the true laser light source to the recording medium in the optical path is partially or completely eliminated by the hologram pattern of the hologram member (partial removal is practically applicable even though complete removal is preferred). Therefore, it is possible to form a light spot on the track on the recording medium, and the light source has no slight aberration or aberration.
[16] The column direction of the hologram pattern of the hologram member of the optical pickup device of the present invention is completely aligned with the long axis direction of the bright field pattern of the true laser light source. The field field pattern is elliptical and exhibits a strong cross section of the luminous flux at a position about 10 to 20 cm away from the semiconductor laser radiation point. The light distribution angle is larger in the long axis direction than in the short axis direction so that light output with more uniform intensity is obtained in the long axis direction than in the short axis. In the column direction of the hologram pattern aligned in the long axis direction of the flower field pattern, light can be applied with similar intensity to the hologram pattern and other hologram patterns at the spaced end of the hologram member. It is therefore possible to form a virtual laser light source with an intensity similar to that of a true laser light source and to reduce the difference in the intensities of the light to be applied to the hologram pattern. Since a plurality of optical spots having a small intensity difference can be applied to the optical disk, it is possible to suppress the change of the data signal read from the optical disk and to be changed photoelectrically. Therefore, deterioration of the quality of the data signal is prevented. Since the hologram member is exposed, in a state where light of uniform intensity can be received, and at a relatively spaced position from the true laser light source, the angle θ described with reference to FIG. 9 is astigmatism and coma aberration of the light spot. It can be made small so that is reduced.
[17] The hologram member of the optical pickup device of the present invention may be a phase hologram member. The hologram pattern for the diffracted light corresponding to each virtual laser light source is determined so that the amount of diffracted light that does not form a light spot is reduced and the reduced amount of light is used as a light spot that forms diffracted light.
[18] The amount of diffracted light that does not form a light spot has a cue opposite to the light spot that forms the diffracted light of the diffracted light. The light traveling toward the light spot for forming the optical element becomes the light spot for forming the diffraction light, while the light traveling toward the outside of the light spot for forming the optical element becomes the diffraction light that does not form the light spot. The phase hologram member can reduce the amount of light traveling in a particular direction and direct the reduced amount of light in the other direction. Therefore, the light spot with high light intensity can be formed by reducing the amount of diffracted light that does not form the light spot, and the reduced light amount is used as the light spot for forming the diffracted light.
[19] In the optical pickup apparatus of the present invention, the light spot on the recording medium formed by the non-diffracted light from the true laser light source is used for the servo operation. The hologram member has a hologram pattern that provides uniform light intensity of the servo light spot within the entire light spot area.
[20] Servo tasks include other tasks such as typical tracking servos and focus servos. The light spot on the recording medium formed by the non-diffracted light from the true laser light source is used not only solely for the servo operation but also for combining operations such as data reading, and the latter is generally used.
[21] The servo light spot is required to have a small light intensity change even when there is a tracking shift or the like. However, light spots on the recording medium generally have high light intensity in the center spot area and low light intensity in the peripheral spot area. Such light spots are not effective for servo light spots. Light from the true laser light source corresponding to the servo light source passes through the hologram member without diffraction. Such light passes through a hologram pattern that reduces light intensity in the center spot area and provides uniform light intensity of the light spot on the recording medium in the whole spot area, and an appropriate light spot can be formed for servo operation.
[22] An optical pickup apparatus of the present invention comprises: (a) a single calm laser light source; (b) an optical spot for receiving the light from the true laser light source via the hologram member and an optical spot for forming a servo light spot on the recording medium. The hologram member has a hologram pattern that provides uniform servo light in the entire servo light spot area.
[32] Embodiments of the present invention will be described in detail with reference to the accompanying drawings.
[33] FIG. 1 is a diagram showing the configuration of an optical pickup device 20, and FIG. 2 is an enlarged view of a portion of the optical pickup device 20 shown in FIG. 1 from the semiconductor laser 10 to the hologram module 13. FIG. to be. The optical pickup device 20 has an optical path from the semiconductor laser 10 to the objective lens 19. The semiconductor laser 10 has a single laser chip. Light from the single calm laser light source 11 ("calm" was used to distinguish it from the "virtual" laser light sources 12a, 12b, 12c) of the semiconductor laser 10 is emitted toward the hologram module 13 do. The hologram module 13 has one non-diffraction hologram pattern 14 and three diffractive hologram patterns 15a, 15b and 15c. The light from the true laser light source 11 is not diffracted but transmitted through the non-diffraction hologram pattern 14 and the light from the true laser light source 11 is diffracted by the diffraction hologram patterns 15a, 15b, 15c and the eyepiece Proceed toward 18. The diffraction light flux from each diffraction hologram pattern 15a, 15b, 15c coincides with the beam speed emitted from the one corresponding to one virtual laser light source 12a, 12b, 12c. The column direction of the true and virtual laser light source 11 is parallel to the column direction of the non-diffraction and diffraction hologram patterns 14, 15a, 15b, 15c. The true and virtual laser light sources 11, 12a, 12b are arranged at equal intervals. In FIG. 1, although the non-diffraction and diffraction hologram patterns 14, 15a, 15b, 15c are arranged on the hologram module 13 on the side of the semiconductor laser 10, they are the corresponding side of the semiconductor laser 10. It may be arranged on the hologram module 13 on the image. Also in FIG. 1, although the non-diffraction and diffraction hologram patterns 14, 15a, 15b, and 15c are arranged separately in the column direction, they may be arranged to partially overlap in the column direction. Light emitted from the hologram module 13 passes through the eyepiece 18 to be transmitted into the parallel beam of light traveling towards the objective lens 19. The light emitted from the objective lens 19 forms light spots 24, 25a, 25b, 25c on each track of the optical disc 23 as images of the true and virtual laser light sources 11, 12a, 12b, 12c. . The tracks formed by the light spots 24, 25a, 25b, 25c are located continuously in the radial direction of the optical disc 23. The light spots of each of the reflected light spots 24, 25a, 25b, 25c travel through the objective lens 19 and the eyepiece 18 in a direction opposite to incident light and through a beam splitter (not shown). (Not shown) is reached, thereby reading data on each track.
[34] The true laser light source 11 is arranged such that the long axis direction of the flower field pattern coincides with the column direction of the non-diffraction and diffraction hologram patterns 14, 15a, 15b, 15c of the hologram module 13. The true field pattern of the true laser light source 11 is elliptical. The intensity of the light field pattern maintains a predetermined value or a large value in a wide range along the long axis of the ellipse. Therefore, the light intensity of the virtual laser light sources 12a, 12b, 13c in the long axis direction set as described above can be made uniform along the long axis direction. The non-diffraction and diffractive hologram patterns 14, 15a, 15b, 15c can modulate the hologram pattern with a black and white obstructed fringe or phase hologram pattern with binary or saw blade grooves formed in glass or the like.
[35] The light from the true laser light source 11 is reflected by the eyepiece 18 and the objective lens 19 and diffracted by the hologram module 13 so that the quality of the light spots 25a, 25b, 25c on the optical disc 23 is lowered. Because it accommodates astigmatism and coma aberration. In order to avoid this, the diffraction hologram patterns 15a, 15b, and 15c have the light beams emitted from these patterns. It is designed to give the reverse diffraction of the whole astigmatism and coma aberration in the optical path. This inverse diffraction overlaps with the inherent astigmatism and coma aberration to reduce or eliminate the light spots 25a, 25b, 25c (the reduction may be practically applicable even if the diffraction is zero, although it is most desirable). . The reverse diffraction may be astigmatism and coma aberration caused only by diffraction, which may be diffraction of total astigmatism and coma aberration within the optical path from the true laser light source 11 to the light spots 25a, 25b, 25c. have. In this case, the astigmatism and coma aberration of the light spots 25a, 25b, 25c are partially eliminated with respect to the aberration caused by diffraction only.
[36] 3 is a schematic diagram of each diffractive hologram pattern 15a, 15b, 15c. The diffraction grating pattern 65 of the diffraction grating 64 of the conventional optical pickup apparatus shown in Fig. 8 is a pattern composed of a plurality of parallel straight lines, and therefore it is considered that only diffraction can eliminate the entire aberration. In contrast, each of the diffractive hologram patterns 15a, 15b, and 15c, which provides the diffraction function and the aberration elimination function, is a pattern composed of curves instead of parallel straight lines.
[37] A method of determining the hologram pattern is described, which gives diffracted light coming from the respective diffractive hologram patterns 15a, 15b, and 15c, and shows the astigmatism and coma aberration of each light spot 25a, 25b, or 25c. In order to eliminate, aberrations of the whole aberration are given in the optical path from the true laser light source 11 to the respective light spots 25a, 25b, and 25c. As a first method, the hologram pattern is determined by applying a light from the light source and a true laser light source 11 positioned at the position of the virtual laser light source to position the light sensing film on the hologram module 13 and the recording disturbance fringe, Has the same wavelength as that of the true laser light source 11. The hologram pattern determined by this method is not the theoretical form aberration (astigmatism and coma) of diffraction. The second method uses computer analysis software. Such computer analysis software is already available and well known. For example, the "Code V" of the American Optical Research Association is a formula for calculating the hologram pattern for two light sources (in this example, a true laser light source 11 and one virtual light source 12a, 12b, 12c). (Coefficient of polynomial). The hologram pattern that theoretically does not form diffraction aberration (astigmatism and coma aberration) is determined by the polynomial obtained. If the aberrations of the eyepiece 18 and the objective lens 19 are taken into account using the above software, the eyepiece 18 and the objective lens 19 data such as the radius of curvature, lens thickness, spherical coefficients are obtained from the optical pickup apparatus. It is entered to simulate the configuration. As this simulation, the equation is a hologram to be formed on the hologram module by the light source located at the position of the optical disk 23 and the light spots 25a, 25b, 25c and having no aberration and the light beam from the true laser light source 11. It is obtained by showing a pattern. The hologram pattern determined from the above equation can remove the diffraction aberration and the aberration of the eyepiece 18 and the objective lens 19.
[38] 4 is a schematic diagram illustrating a method of determining diffractive hologram patterns 15a, 15b and 15c, respectively, using optical elements. The half mirror 35a is located at an intermediate position of the optical path from the true laser light source 11 to the non-diffractive hologram pattern 14 so as to partially reflect the light downward. The half mirrors 35b, 35c,... Are also located at intermediate positions in the optical path of the reflected light to partially reflect the light towards the diffractive hologram patterns 15a, 15b,... Transfer downwards. The bottom half mirror among the half mirrors 35a, 35b, 35c, ... is displaced by the full mirror to transmit light without transmitting downward. In this method, a plurality of virtual laser light sources 12a, 12b, 12c having characteristics matching the true laser light source 11 are formed. The disturbing fringe to be formed at the position of the diffraction hologram by the luminous flux from the true laser light source 11 and the virtual laser light sources 12a, 12b, 12c is used as the diffraction hologram pattern 15a. For example, to record the diffractive hologram pattern 15a, the photosensitive material is coated on the hologram module 13 and exposed to the diffraction fringe pattern. The diffraction hologram pattern thus obtained can eliminate or eliminate astigmatism and coma aberration of diffraction.
[39] FIG. 5 shows another method of forming a plurality of light sources having characteristics consistent with a true laser light source using the pinhole member 50 at the positions of the half mirrors 35a, 35b, 35c shown in FIG. The light emitted from the true laser light source 11 is transformed by the eyepiece 18 at a parallel luminous flux applied to the output from the pinhole member 50 and the pinholes 51a, 51b, 51c, 51d. The light output from each pinhole is equivalent to the light output from the virtual laser light source. By using the light output from each pinhole, the diffraction hologram pattern of the hologram module 13 is determined.
[40] 6A-6C are graphs and diagrams illustrating a method for improving tracking servo light spots. The light transmitted through the non-diffraction hologram pattern 14 shown in FIG. 2 is used with the tracking servo to read the data on the track of the optical disc. Along with the tracking servo light spot, the light spot is required to have a uniform intensity over the entire spot area. However, as shown in Fig. 6A, the light dispersion intensity incident on the non-diffraction hologram pattern 14 of the hologram module 13 from the true laser light source 11 has a peak shape with a peak at the center. This intensity distribution can be improved by using a phase hologram pattern. That is, deep grooves of the phase hologram pattern, and a larger amount of non-diffracted light (zero-order light) can be reduced and a larger amount of diffracted light can be increased using a reduced amount of non-diffracted light, such as diffracted light. . In addition, wider valleys (grooves) can be made equal to heel (nan-groove) widths, reducing a greater amount of zero order light and more diffracted light amount can be increased using a reduced amount with diffracted light. have. As shown in Fig. 6B, the depth of the groove 54 is made small at a position far from the center of the optical axis to reduce the amount of zero-order light and to direct the reduced light amount toward the other direction. Instead of adjusting the depth of the grooves 54, the depths of the grooves 54 may be the same and may be the ratio of each non-groove width to the total width of the adjacent grooves 54 of each pair. Where the groove is set to a1> a2> a3> a4> a5> a6, ...,> an, while a1, a2, a3, a4, a5, a6, ..., an The ratio from the center of the optical axis to the position up to the far position in this order. In the above method, as shown in Fig. 6C, the light intensity distribution can be made uniform in a certain range with respect to the optical axis center in the radial direction. The intensity distribution of incident light can be flattened by using the diffractive hologram pattern 14 with the groove 54 as shown in FIG. 6B. If the tracking servo signal is generated from the reflected light of the light spot formed by the light of uniform intensity, this tracking servo signal is stable even if the objective lens is subjected to the tracking shift.
[41] The virtual laser light sources 12a, 12b, 12c of the optical pickup device shown in Figs. 1 and 2 are arranged only on one side of the true laser light source 11. Instead, they may be arranged on both sides of the true laser light source 11. In this case, the virtual laser light sources 12a, 12b, 12c are arranged on both sides of the true laser light source 11 substantially symmetrically with the true laser light source 11. Moreover, although the non-diffraction and diffraction hologram patterns 14, 15a, 15b, and 15c of the optical pickup apparatus shown in Figs. 1 and 2 are arranged with holograms only on the side of the semiconductor laser 10, they are not provided with the hologram module 13 (The diffraction hologram pattern 15a on the semiconductor laser 10 side and the diffraction hologram pattern 15b on the eyepiece 18, etc.) or on the hologram module 13 only on the eyepiece 18 side. have. Furthermore, although the diffraction hologram patterns 15a, 15b, and 15c of the diffraction hologram module 13 of the hologram module 13 of the optical pickup shown in Figs. 1 and 2 are spaced apart in the column direction, they are arranged in the column direction. Are partially nested.
[42] The optical pickup apparatus of the present invention minimizes the aberration caused by the optical element in the optical path from the true laser light source to the recording medium. Therefore, it is possible to form a light spot having a shape and light intensity suitable for recording / reading data on the recording medium, and a plurality of light spots on the recording medium.
[43] The optical pickup apparatus of the present invention has a hologram member that uniformly provides the intensity of the light spot that lowers the intensity from the center region toward the peripheral region. Therefore, it is possible to form light spots on the recording medium, and to form light intensities with little variation, which is suitable for servo operation.

权利要求:
Claims (19)
[1" claim-type="Currently amended] In the optical pickup device 20,
A single calm laser light source 11;
A hologram member (13) for diffracted light emitted from said true laser light source to form at least one virtual laser light source;
A light spot which forms a plurality of light spots 24, 25a to 25c on a track of the recording medium 23 and forms an optical element 19 for receiving light from the hologram member 13,
The hologram patterns 15a to 15c of the hologram member 13 cause diffracted light to be caused by the optical elements 13, 18, 19 in the optical path from the true laser light source 11 to the recording medium 23. And an optical pickup apparatus which is determined to give an inverse aberration of aberration.
[2" claim-type="Currently amended] The method of claim 1,
The column direction of the hologram patterns (15a to 15c) of the hologram member (13) is aligned in the long axis direction of the field pattern of the true laser light source (11).
[3" claim-type="Currently amended] The method according to claim 1 or 2,
The hologram member 13 is a phase hologram member, and the hologram pattern for diffraction corresponding to each of the virtual laser light sources 12a to 12c reduces the intensity of the diffracted light that is not used for forming the light spot and reduces the amount of light. An optical pickup apparatus, characterized in that it is determined to be used as diffracted light for spot formation.
[4" claim-type="Currently amended] The method according to any one of the preceding claims,
The light spot 24 on the recording medium 23 formed by the non-diffracted light from the true laser light source 11 is used for servo operation, and the hologram member 13 has a uniform intensity in the entire light spot area. And a hologram pattern (14) providing a servo light spot (24).
[5" claim-type="Currently amended] In the optical pickup device,
A single calm laser light source 11;
A light spot which forms a servo light spot on the recording medium 23 and forms an optical element for receiving the light from the true laser light source 11 via the hologram member 13,
The hologram member (13) has a hologram pattern (14) which provides a servo light spot of uniform intensity in the entire servo light spot area.
[6" claim-type="Currently amended] The method of claim 1,
The holographic pattern is a phase hologram pattern having a binary or saw blade groove or an amplitude hologram pattern having a black and white disturbing fringe.
[7" claim-type="Currently amended] The method of claim 1,
And a hologram pattern is recorded on the hologram member on one side of the true laser light source.
[8" claim-type="Currently amended] The method of claim 1,
And a hologram pattern is recorded on the hologram pattern on the corresponding side of the true laser light source.
[9" claim-type="Currently amended] The method of claim 1,
And a hologram pattern arranged at predetermined intervals in a column direction between the true laser light source and the virtual laser light source.
[10" claim-type="Currently amended] The method of claim 1,
And the hologram pattern is partially overlapped and arranged in a column direction of the true laser light source and the virtual laser light source.
[11" claim-type="Currently amended] The method of claim 3, wherein
The diffractive hologram pattern has a curved pattern.
[12" claim-type="Currently amended] The method of claim 4, wherein
And the diffractive hologram pattern has a plurality of grooves and the amount of light not to be diffracted is adjusted according to the depth of the groove (54).
[13" claim-type="Currently amended] The method of claim 4, wherein
The diffractive hologram pattern has a plurality of grooves (54) and the amount of light not to be diffracted is adjusted in accordance with the width of the width of the groove (54).
[14" claim-type="Currently amended] The method of claim 1,
And the true laser light source is a semiconductor laser having a single laser chip coupled therein.
[15" claim-type="Currently amended] The method of claim 1,
Wherein each hologram pattern gives diffracted light of different aberrations.
[16" claim-type="Currently amended] The method of claim 1,
And each hologram pattern gives diffracted light of the same aberration.
[17" claim-type="Currently amended] In a method of forming a plurality of virtual laser light sources 12a, 12b, 12c by forming a diffractive hologram pattern on a hologram member using light from an optical element,
The first optical element partially reflects light from the true laser light source downwards and arranges the first optical element 35a in the optical path from the true laser light source 11 to the non-diffractive hologram pattern 14. Wow;
The n optical element partially reflects the partially reflected light towards the hologram member and reflects the afterglow downward, and n (n is a positive integer) within the optical path of the partially reflected light. Arranging c);
Arranging an optical element for reflecting the afterglow toward the hologram member.
[18" claim-type="Currently amended] The method of claim 17,
And the first and n optical elements are half mirrors, and in the last step the optical elements are full mirrors.
[19" claim-type="Currently amended] In a method for forming a plurality of virtual light sources 12a, 12b, 12c ... by forming a diffraction hologram pattern on a hologram member using light emitted from a pinhole,
Modifying the light from the true laser light source 11 by the eyepiece 47 to parallel light;
Arranging one member (50) with at least one pinhole in an optical path of parallel light.

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JP3518684B2|2004-04-12|Objective lens design method, objective lens, objective lens manufacturing method, multi-wavelength optical system, optical head, and optical disk device

同族专利:

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公开号 | 公开日

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EP1060472B1|2002-05-15|

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US7050207B1|2006-05-23|

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EP1060472A1|2000-12-20|

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JPH11238246A|1999-08-31|

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WO1999042994A1|1999-08-26|

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TW417106B|2001-01-01|

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CN1290392A|2001-04-04|

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MY123260A|2006-05-31|

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KR100368493B1|2003-01-24|

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CN1114205C|2003-07-09|

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DE69901491T2|2002-12-19|

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JP3362768B2|2003-01-07|

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DE69901491D1|2002-06-20|

引用文献:

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公开号 | 申请日 | 公开日 | 申请人 | 专利标题

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法律状态:
1998-02-19|Priority to JP10/52657

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1998-02-19|Priority to JP05265798A

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1999-02-12|Application filed by 오카 마코토, 가부시키가이샤 캔우드

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2001-09-10|Publication of KR20010086251A

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2003-01-24|Application granted

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2003-01-24|Publication of KR100368493B1

优先权:

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申请号 | 申请日 | 专利标题

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JP10/52657|1998-02-19|

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JP05265798A|JP3362768B2|1998-02-19|1998-02-19|Optical pickup device|