JP4479463B2 - Optical pickup device and optical disk device - Google Patents

Description

  The present invention relates to an optical pickup apparatus and an optical disk apparatus that are preferably used in an optical disk apparatus mounted on an electronic device such as a personal computer or a notebook computer.

  Conventionally, various optical discs such as DVD (Digital Versatile Disc), CD-R (Writable Compact Disc), CD-RW (Rewritable Compact Disc) have been developed as optical recording media. In a DVD, information is recorded or reproduced by a laser beam having a wavelength of about 650 nm. On the other hand, in CD-R and CD-RW, information is recorded or reproduced by laser light having a wavelength of about 780 nm. An optical disc apparatus that records or reproduces information on a plurality of types of optical discs has been proposed.

  Also, in such an optical disk apparatus for recording or reproducing information on a plurality of types of optical disks, a plurality of laser elements having different wavelengths are arranged adjacent to one package (so-called hybrid type two-wavelength semiconductor laser) In addition, a semiconductor laser element (so-called monolithic two-wavelength semiconductor laser) in which light sources having a plurality of wavelengths are integrated on one semiconductor substrate has been proposed. The optical system using these two-wavelength semiconductor lasers can reduce the cost, for example, by sharing the optical components set separately from the optical system using the light source corresponding to each wavelength.

  However, in these two-wavelength semiconductor lasers, the distance between the emission points of the two wavelengths is about 110 μm in both the hybrid type and the monolithic type, and the optical axes of the two light sources inevitably shift. For this reason, for example, by using a parallel plate on which a wavelength-selective film is formed, the optical paths of laser beams of two wavelengths are matched [see (Patent Document 1). ]. Alternatively, the arrangement of the two-wavelength semiconductor lasers is devised, and the optical system is configured so as to preferentially reduce the aberration of light from the light source that is less likely to achieve a predetermined performance [see (Patent Document 2). ] The light source that is less likely to produce a predetermined performance is made to coincide with the optical axis of the optical system [refer to (Patent Document 3). ]is doing.

FIG. 7 shows a schematic diagram of an optical system of a conventional optical pickup device. However, for the sake of simplicity, the return path optical system for detecting the return light from the optical disk and the monitor optical system for controlling the light quantity are omitted. Here, the configurations of (Patent Document 1) to (Patent Document 3) are also shown. The two-wavelength semiconductor laser light source 1 includes a light emitting point 2 having a wavelength λ1 (650 nm) for DVD and a light emitting point 3 having a wavelength λ2 (780 nm) for CD. The light emitting point 2 of the wavelength λ1 that is difficult to achieve a predetermined performance is made to coincide with the optical axis of the optical system in order to reduce aberrations preferentially. The parallel plate 31 reflects the light with the wavelength λ1 and transmits the light with the wavelength λ2, the substrate 31b that transmits the light, and the second wavelength selective film 31c that reflects the light with the wavelength λ2. And a thick substrate 31d. By adjusting the thickness of the substrate 31b and the incident angle of the laser beam, the optical path of the laser beam having the wavelength λ1 and the optical path of the laser beam having the wavelength λ2 are matched. The collimating lens 6 converts the light emitted from the light emitting points 2 and 3 into substantially parallel light, and the objective lens 11 condenses the light converted into substantially parallel light onto the optical disk 12.
JP 2000-99983 A JP 2001-148136 A JP 2002-25103 A

  In recent years, there has been a strong demand for optical disc apparatuses to record as well as reproduce on a DVD and record at a high speed on a CD. In order to perform recording as well as reproduction on a DVD, it is necessary to reduce the diameter of the focused spot on the optical disk, so the optical magnification must be increased. On the other hand, in order to cope with recording at a high speed on a CD, it is necessary to keep the optical magnification low in order to keep the light use efficiency high. However, in the conventional configuration using a two-wavelength semiconductor laser, since the light emitting points are close to each other, it is impossible to achieve both recording as well as reproduction on a DVD and recording at a high speed on a CD. It was.

  The present invention solves such a conventional problem, and includes a light source in which a plurality of light emitting points having different wavelengths are provided close to each other, and light from any light emitting point can be recorded and reproduced at high speed. An object of the present invention is to provide an optical pickup device capable of performing both.

In order to solve the conventional problems, an optical pickup device of the present invention includes a first light emitting point that emits light having a first wavelength, and second light emission that emits light having a second wavelength longer than the first wavelength. A light source in which the first light emitting point and the second light emitting point are provided close to each other, light receiving means for receiving the light reflected by the optical disc and generating an electrical signal, the first light emitting point, An optical system for condensing the light respectively emitted from the second light emitting point onto the optical disc and guiding the light reflected by the optical disc to the light receiving means, the optical system having a light transmitting member, and transmitting the light The member includes a surface facing the light source and a surface not facing the light source, a filter is formed on the surface not facing the light source, and the filter is formed on the surface of the light transmission member. Light incident from the light emitting point and the second light emitting point A wavelength selective separation film that reflects each with a different reflectance, and a total reflection film that is formed on a part of the surface of the wavelength selective separation film and totally reflects light incident from the first light emission point and the second light emission point The total reflection film is formed so as to avoid the optical axis of the light emitted from the light source, the light incident on the filter is reflected by the filter to change the light intensity distribution, and the The intensity distribution of the light is different between the first wavelength and the second wavelength, and the surface facing the light emitting point is not parallel to the surface not facing the light emitting point and is shifted from the optical axis of the optical system. The astigmatism of the light emitted from the light emitting point is tilted in a direction to make it smaller than when the surface on which the filter is formed and the surface facing the light emitting point are parallel to each other. The light intensity distribution is changed by reflecting light incident on the filter from the first light emission point and the second light emission point by the filter, and the light intensity distribution is made different between the first wavelength and the second wavelength. Therefore, it is possible to optimize the diameter of the light condensing spot and the light intensity distribution of the light emitted from each light emitting point. Further, by forming a filter on a surface that does not face the light emitting point, it is possible to prevent the wavefront aberration from deteriorating. Further, since the surface facing the light emitting point is not parallel to the surface not facing the light emitting point, interference of light coming out of the light transmitting member can be prevented. Furthermore, the astigmatism of the light emitted from the light emitting point at a position shifted from the optical axis of the optical system is made smaller than when the surface on which the filter is formed and the surface facing the light emitting point are parallel to each other. Astigmatism can be reduced by tilting in the direction.

As described above, the optical pickup device of the present invention can optimize the diameter of the focused spot and the light intensity distribution on the optical disc for each light of each wavelength. Further, it is possible to prevent the wavefront aberration from deteriorating and to prevent interference of light coming out of the light transmitting member. Furthermore, astigmatism can be reduced. For this reason, light from any light emitting point can be recorded and reproduced at high speed.

According to a first aspect of the present invention, there is provided a light source provided with a plurality of light emitting points having different wavelengths close to each other, light receiving means for receiving light reflected by an optical disc and generating an electrical signal, and the light emitting points. An optical system that focuses the emitted light onto an optical disk and guides the light reflected by the optical disk to the light receiving means; the optical system includes a light transmitting member; and the light transmitting member includes the light emitting point and the light emitting point. It is composed of an opposing surface and a surface that does not oppose the light emitting point, and the surface that does not oppose the light emitting point is formed with a filter that converts light emitted from each light emitting point into a predetermined light intensity distribution, The surface facing the light emitting point is not parallel to the surface not facing the light emitting point, and the filter is formed with astigmatism of light emitted from the light emitting point at a position shifted from the optical axis of the optical system. Opposite the light emitting point Doo is an optical pickup device characterized by inclined in a direction smaller than that parallel, to a diameter and light intensity distribution of the focused spot on the optical disc with optimum respectively for each light for each wavelength Can do . Further, it is possible to prevent the wavefront aberration from deteriorating and to prevent interference of light coming out of the light transmitting member. Furthermore, astigmatism can be reduced. For this reason, light from any light emitting point can be recorded and reproduced at high speed.

A second invention is an optical pickup device according to claim 1, a rotary drive means for rotating the optical disk, an optical disk apparatus which includes a moving means or released closer to the optical pickup device with respect to said rotary drive means Thus, an optical disc apparatus capable of recording and reproducing light of any wavelength that can be emitted from the light source can be obtained.

(Embodiment 1)
An optical pickup device according to Embodiment 1 of the present invention will be described with reference to the drawings. 1 is a schematic diagram of an optical system of an optical pickup device according to Embodiment 1 of the present invention, FIG. 2 (a) is an enlarged top view of a filter unit according to Embodiment 1, and FIG. 2 (b) is an enlarged front view. 3A is a diagram comparing the light intensity distribution with and without the filter on the aperture surface of the objective lens, and FIG. 3B is a diagram comparing the light intensity distribution with and without the filter on the optical disk. It is.

  First, the configuration will be described. A two-wavelength semiconductor laser light source 1 which is a light source provided with a plurality of light-emitting points having different wavelengths close to each other includes a light-emitting point 2 having a wavelength λ1 (650 nm) for DVD and a light-emitting point 3 having a wavelength λ2 (780 nm) for CD. . The two-wavelength semiconductor laser light source 1 may be a so-called hybrid two-wavelength semiconductor laser or a so-called monolithic two-wavelength semiconductor laser. Further, a light source having a light emitting point having three or more wavelengths may be used. The interval between the light emitting point 2 and the light emitting point 3 is about 0.05 mm to about 0.15 mm. In the first embodiment, a monolithic type two-wavelength semiconductor laser in which the interval between the emission points of two wavelengths is about 110 μm is used. The diffraction grating 4 is formed by forming a diffraction grating on the surface or inside of an optical member, and separates the light emitted from the light emitting point 3 into three lights used in the three-beam tracking method. The integrated prism 5 is composed of an optical member having a plurality of inclined surfaces 5a to 5c provided therein, and a polarization separation film (not shown) corresponding to the wavelength is formed on the inclined surface.

  The collimating lens 6 and the objective lens 11 which is a bifocal objective lens are each made of optical glass or optical plastic. Light emitted from the light emitting points 2 and 3 is made into substantially parallel light by the collimating lens 6 and condensed by the objective lens 11 so as to focus on the position of the optical disc 12 corresponding to each wavelength. In the first embodiment, the line connecting the center of the collimating lens 6 and the center of the objective lens 11 and its extension are called the optical axis of the optical system. As the bifocal objective lens 11, a combination of a condensing lens and a Fresnel lens or a hologram lens, a combination in which a condensing lens for DVD is provided with aperture limiting means during CD reproduction, or the like can be used.

  The light transmitting member 7 is made of optical glass or optical plastic. The filter 8 is formed on the surface 7 a that does not face the light emitting point 2 and the light emitting point 3 of the light transmitting member 7. The light transmitting member 7 has a surface 7 a and a surface 7 b facing the light emitting point 2 and the light emitting point 3. The surface 7a and the surface 7b are not parallel so that the light that has passed through the light transmitting member 7 does not cause interference. Further, the surface 7a and the surface 7b perpendicular to the plane composed of the optical axis, the light emitting point 2 and the light emitting point 3 are not parallel but non-parallel, so that the light emitting point 2 and the light emitting point 3 which are not on the optical axis of the optical system. Astigmatism of the light emitted from can be reduced. On the other hand, if such light interference and astigmatism do not become a problem, the manufacturing cost can be reduced by making the surfaces 7a and 7b parallel.

  The filter 8 includes a wavelength selective polarization separation film 8a formed on the surface 7a of the light transmission member 7, and a total reflection film 8b formed on the surface of the wavelength selection polarization separation film 8a corresponding to a predetermined light intensity distribution. Yes. The wavelength selective polarization separation film 8a is made of a dielectric multilayer film. In the first embodiment, the design of the film characteristics of the wavelength selective polarization separation film 8a is, for example, about 50% P-polarized reflectance at wavelength λ1, almost 100% S-polarized reflectance, and 90% P-polarized reflectance at wavelength λ2. The S-polarized light reflectance at the wavelength λ1 and the wavelength λ2 was set to be almost 100%. However, this number varies depending on the constants of the parts constituting the optical system and the design constants of the optical system, and the optimum film characteristics differ depending on the optical system. The total reflection film 8b is made of a metal film or a dielectric multilayer film. The total reflection film 8b has a predetermined size and shape at a position corresponding to the central portion of the light emitted from the light emission point 2 and the light emission point 3. A region 8c in which no is formed is provided. In the first embodiment, the region 8c is a region near the optical axis of the optical system.

  The rising prism 9 is a prism for raising the optical axis that has been in a plane substantially parallel to the surface of the optical disk 12 until then substantially perpendicular to the surface of the optical disk 12, and may be a mirror. The hologram element 10 is composed of a polarization hologram 10a and a quarter wavelength plate 10b. The polarization hologram 10a is made of a material having wavelength selectivity so as to act only on light having the wavelength λ1. The quarter wavelength plate 10b has a refractive index and a thickness so as to act on both wavelengths λ1 and λ2. The hologram element 10 is fixed to a common member (not shown) together with the objective lens 11 and moves together with the objective lens 11.

  The optical disk 12 is CD, CD-ROM, CD-R / RW, DVD is DVD-ROM, DVD ± R / RW, DVD-RAM, etc., except for CD and DVD, except for read-only media All can be recorded and played back. Further, not only the combination of the CD system and the DVD system but also the combination of so-called Blu-ray, HDDVD, etc. does not lose generality.

  The front light monitor 13 is a sensor that receives a part of the light emitted from the light emitting point 2 and the light emitting point 3, converts the light amount into an electric signal, and outputs it. This electrical signal is sent to a control circuit (not shown) that controls the drive circuit (not shown) of the two-wavelength semiconductor laser light source 1 so that the light amount of the condensed spot condensed on the optical disk 12 is constant. The light receiving sensor 14 is a light receiving element that receives reflected light from the optical disk 12 and converts the light into an electric signal for generating an RF signal, a tracking error signal, a focus error signal, and the like.

  Next, the optical path will be described. The light emitted from the light emitting point 2 passes through the diffraction grating 4 and the integrated prism 5 and enters the collimating lens 6. The light is converted into substantially parallel light by the collimating lens 6, is reflected by the filter 8 through the light transmitting member 7, passes through the light transmitting member 7 again, and enters the rising prism 9. Further, the optical disc 12 is focused through the rising prism 9, the hologram element 10 and the objective lens 11.

  In general, if the ratio of the light intensity at the center of the aperture of the objective lens 11 to the light intensity at the end of the aperture is large as in the case of no filter in FIG. ) Without filter.

  The light incident on the filter 8 is P-polarized light. About 15% of the light 15b incident on the region 8c where the total reflection film 8b is not formed is reflected to become the light 16b toward the optical disk 12, and the remaining about 50% of the light is The light 17 is transmitted through the wavelength selective polarization separation film 8 a and becomes incident on the front light monitor 13. The light 15a incident outside the region 8c is reflected by the total reflection film 8b so that the total amount of light is reflected to become the light 16a toward the optical disc 12. As a result, by reflecting with the filter 8 as shown in FIG. 3A, the light intensity distribution on the aperture surface of the objective lens 11 is converted from a broken line to a distribution with a lowered central portion as shown by a solid line. When this light is condensed by the optical disk 12 and focused, the light intensity distribution of the condensed spot is concentrated in a narrower area as shown by the solid line in FIG. 3B. That is, the condensing spot is narrowed down further. This phenomenon is called a super-resolution phenomenon. By optimizing the light intensity distribution on the aperture surface of the objective lens 11 according to the optical system, the focused spot can be narrowed down, and the rise of the peripheral portion called a side lobe can be suppressed low.

  The filter 8 functions as a beam splitter that separates the light emitted from the light emitting point 2 into light that is reflected and incident on the optical disk 12 and that is transmitted and incident on the front light monitor 13. As described above, the light emitted from the light emitting point 2 can be used efficiently by using the light that does not go to the optical disk 12 for light amount control.

  In the first embodiment, the light incident on the filter 8 is transmitted through the light transmitting member 7 and reflected by the wavelength selective polarization separation film 8a formed on the flat surface 7a, thereby preventing the aberration from deteriorating. It is out. If the filter 8 is configured such that light incident on the filter 8 is incident without passing through the light transmitting member 7, a total reflection film 8b is formed on the surface of the light transmitting member 7, and the wavelength selective polarization separation film 8a is formed on the surface. It becomes the structure which forms. As a result, a step due to the total reflection film 8b occurs on the surface of the wavelength selective polarization separation film 8a, so that the reflected light acts as an aberration to deteriorate the quality of the condensed spot or prevent the condensed spot from being narrowed down. Or In the first embodiment, the aberration is not deteriorated from the beginning. However, if the influence is small, the light transmitting member 7 may be omitted.

  Further, the polarization direction of the light is set so as to pass through the hologram element 10 without being influenced by the polarization hologram 10a, and the light is converted from linearly polarized light to circularly polarized light by the quarter wavelength plate 10b.

  The light reflected by the optical disk 12 passes through the objective lens 11, the hologram element 10, the rising prism 9, the light transmission member 7, the filter 8, and the collimating lens 6 and enters the integrated prism 5. When transmitting through the hologram element 10 again, the quarter wavelength plate 10b converts the circularly polarized light to linearly polarized light that is perpendicular to the forwardly polarized light, that is, S-polarized light. The polarization hologram 10a separates the signal light component corresponding to the RF signal, tracking error signal, focus error signal, and the like. The filter 8 is designed to reflect all S-polarized light, and the light intensity distribution does not change.

  The polarization separation film provided on the inclined surface 5a in the integrated prism 5 transmits the P-polarized light emitted from the light emitting point 2 and the light emitting point 3, and reflects the S-polarized light emitted from the light emitting point 2 and reflected by the optical disk 12. Such a polarization separation film configuration is adopted. Therefore, the light incident on the integrated prism 5 is reflected by the polarization separation film provided on the inclined surface 5 a and enters the light receiving sensor 14. Each signal light component separated by the polarization hologram 10 a and incident on the light receiving sensor 14 is converted into various electric signals by the light receiving sensor 14.

  The light emitted from the light emitting point 3 passes through the diffraction grating 4 and the integrated prism 5 and enters the collimating lens 6. The light is converted into substantially parallel light by the collimating lens 6, is reflected by the filter 8 through the light transmitting member 7, passes through the light transmitting member 7 again, and enters the rising prism 9. Further, the optical disc 12 is focused through the rising prism 9, the hologram element 10 and the objective lens 11.

  At this time, the light incident on the filter 8 is P-polarized light, and 92 to 93% of the light 15b incident on the region 8c where the total reflection film 8b is not formed is reflected to become the light 16b toward the optical disc 12, and the remaining 7 to 8% of the light is transmitted through the wavelength selective polarization separation film 8 a and becomes light 17 incident on the front light monitor 13. The light 15a incident outside the region 8c is reflected by the total reflection film 8b so that the total amount of light is reflected to become the light 16a toward the optical disc 12. Accordingly, the light intensity distribution toward the optical disk 12 is different from the case of the light emission point 2 and the difference in reflectance between the opening center portion and the opening end portion of the objective lens 11 is small, so that the distribution without the filter of FIG. Close to. Therefore, the light intensity distribution of the condensing spot on the optical disk 12 is also close to the distribution without the filter in FIG. Also at this time, the filter 8 functions as a beam splitter that separates the light emitted from the light emitting point 3 into the light reflected and incident on the optical disc 12 and the light incident on the front light monitor 13. As described above, the light emitted from the light emitting point 3 can be used efficiently by using the light which does not go to the optical disk 12 for the light amount control. Since the light emitted from the light emitting point 3 has a low optical magnification, it is more efficient to use and is more suitable for recording at high speed.

  Further, when passing through the hologram element 10, this wavelength λ2 is not affected by the polarization hologram 10a, so that it is transmitted as it is, and is converted from linearly polarized light to circularly polarized light by the quarter wavelength plate 10b.

  The light reflected by the optical disk 12 passes through the objective lens 11, the hologram element 10, the rising prism 9, the light transmission member 7, the filter 8, and the collimating lens 6 and enters the integrated prism 5. When transmitting through the hologram element 10 again, the quarter wavelength plate 10b converts the circularly polarized light to linearly polarized light that is perpendicular to the forwardly polarized light, that is, S-polarized light. Since the wavelength λ2 is not affected by the polarization hologram 10a, it passes through the polarization hologram 10a as it is. The filter 8 is designed to reflect all S-polarized light, and the light intensity distribution does not change.

  The polarization separation film provided on the inclined surface 5b in the integrated prism 5 transmits the light emitted from the light emitting points 2 and 3, and reflects the light emitted from the light emitting point 3 and reflected by the optical disk 12. Adopts a simple film configuration. Therefore, the light incident on the integrated prism 5 is reflected by the polarization separation film provided on the inclined surface 5b, separated by the hologram element provided on the inclined surface 5c, and the separated light is incident on the light receiving sensor 14, It is converted into various electric signals.

  In the first embodiment, the filter 8 is formed on the light transmitting member 7 as a beam splitter. However, the present invention is not limited to this configuration. For example, the filter 8 is provided on the surface 9a of the rising prism 9 that does not face the light emitting point 2, the light emitting point 3 and the optical disc 12, and the filter 8 of the light transmitting member 7 is removed to remove the surface 7b. It is good also as a structure which provides a polarization separation film in this.

  As described above, in the first embodiment of the present invention, the light intensity distribution of the spots collected on the optical disk 12 is converted by converting the light emitted from the respective light emitting points having different wavelengths into the respective predetermined light intensity distributions. It can be optimized for each wavelength of light. Therefore, the so-called super-resolution phenomenon is generated by converting the light from a certain light emitting point into a predetermined light intensity distribution, and compared with the case where the light is not converted into such a predetermined light intensity distribution. The diameter can be reduced, and so-called side lobes, which are the rise of the surrounding light intensity distribution, can be reduced. Therefore, the aberration of the condensed spot condensed on the optical disk 12 can be suppressed low. On the other hand, since the light emitting points that do not require such conversion are not converted, the light utilization efficiency is not reduced. In this way, an optimum condensing spot can be realized for the light from each light emitting point without adding new independent optical components. For this reason, an optical pickup device using a light source provided with a plurality of light emitting points having different wavelengths that can perform both recording and reproduction at a high speed of light from any light emitting point while taking advantage of low cost. Can be realized.

(Embodiment 2)
An optical pickup device according to Embodiment 2 of the present invention will be described with reference to the drawings. FIG. 4 is a schematic diagram of an optical system of the optical pickup device according to the second embodiment of the present invention, and FIG. 5 is an enlarged view of the filter unit according to the second embodiment. In the second embodiment, the filter 8 is configured to transmit the light emitted from the light emitting points 2 and 3 and to enter the optical disk 12.

  First, the configuration will be described. In the first embodiment, the filter 8 is formed on the light transmitting member 7. However, in the second embodiment, the filter 8 is formed on the hologram element 10, and the beam splitter 18 is installed instead of the light transmitting member 7 and the filter 8. Has been. Since other configurations are the same as those of the first embodiment, the description thereof is incorporated.

  The hologram element 10 is made of optical glass or the like between a substrate 10c on the two-wavelength semiconductor laser light source 1 side and a substrate 10d on the optical disk 12 side, and the polarization hologram 10a on the two-wavelength semiconductor laser light source 1 side and 1 / on the optical disk 12 side. The configuration includes a four-wave plate 10b. In the second embodiment, the hologram element 10 includes a filter 8 including a wavelength selective polarization transmission film 8d and a total transmission film 8e between the polarization hologram 10a and the substrate 10c. The hologram element 10 including the filter 8 is fixed to a common member (not shown) together with the objective lens 11 as in the first embodiment, and moves together with the objective lens 11. The filter 8 only needs to be closer to the two-wavelength semiconductor laser light source 1 than the quarter-wave plate 10b, and may be formed on the light source side surface of the substrate 10c or the surface of the polarization hologram 10a on the optical disk 12 side. .

  The wavelength-selective polarized light transmitting film 8d is a dielectric multilayer film and is produced around the optical axis of the optical system. The design of the film characteristics of the wavelength-selective polarizing transmission film 8d is, for example, about 50% P-polarized light transmittance at wavelength λ1, almost 100% S-polarized light transmittance, almost 100% P-polarized light transmittance and S-polarized light transmittance at wavelength λ2. It was made to become. However, this number varies depending on the constants of the parts constituting the optical system and the design constants of the optical system, and the optimum film characteristics differ depending on the optical system. The total transmission film 8e is made of a dielectric multilayer film, and is continuously formed outside the wavelength selection polarization transmission film 8d on the same surface as the wavelength selection polarization transmission film 8d in order to eliminate the step generated by the wavelength selection polarization transmission film 8d. It is formed.

  The beam splitter 18 has a configuration in which a polarization separation film 18b is formed on the surface of the substrate 18a made of optical glass or optical plastic on the two-wavelength semiconductor laser light source 1 side. The polarization separation film 18b is made of a dielectric multilayer film. The light emitted from the light emission points 2 and 3 is partially transmitted, and most of the remaining light is reflected toward the optical disk 12, and reflected by the optical disk 12. The designed light is totally reflected and directed to the light receiving sensor 14.

  Next, the optical path will be described. Light emitted from the light emitting points 2 and 3 is converted into substantially parallel light by the collimating lens 6 as in the first embodiment, and enters the beam splitter 18. The light transmitted through the beam splitter 18 enters the front light monitor 13. The light reflected by the beam splitter 18 is raised in the direction of the optical disk 12 by the rising prism 9 and enters the hologram element 10 provided with the filter 8. The light incident on the hologram element 10 passes through the filter 8 and enters the polarization hologram 10a. At this time, since the light emitted from the light emitting point 2 is P-polarized light, the light transmitted through the wavelength selective polarization transmission film 8d is about 50%, and the light intensity distribution at the aperture surface of the objective lens 11 is shown in FIG. And the light intensity distribution on the optical disc 12 is the distribution with the filter shown in FIG. On the other hand, since the light emitted from the light emitting point 3 is also P-polarized light, the light transmitted through the wavelength selective polarization transmission film 8d is almost 100%, and the light intensity distribution at the aperture surface of the objective lens 11 is shown in FIG. The distribution without the filter of FIG. 3A and the light intensity distribution on the optical disk 12 is the distribution without the filter of FIG. The light transmitted through the filter 8 and the polarization hologram 10 a is converted from P-polarized light to circularly-polarized light by the quarter-wave plate 10 b, and is condensed on the optical disk 12 by the objective lens 11.

  The light reflected by the optical disk 12 is converted from circularly polarized light to S polarized light by dropping the quarter wavelength plate 10 b in the hologram element 10 again, and enters the filter 8. Both the light emitted from the light emitting point 2 and the light emitted from the light emitting point 3 are S-polarized light, so that the filter 8 transmits almost 100%, the beam splitter 18 reflects almost 100%, passes through the collimating lens 6, and passes through the light receiving sensor. Head to 14.

  The filter 8 is not provided in the hologram element 10, but the surface of the diffraction grating 4 facing the surface where the actual diffraction grating is provided, the surface 9b of the rising prism 9 facing the two-wavelength semiconductor laser light source 1, or the optical disk 12 may be provided on the surface 9c facing the surface 12 or the like. Thus, when the filter 8 is used for transmission, the degree of freedom in design is high. When the filter 8 is provided on the surface of the diffraction grating 4 opposite to the surface on which the actual diffraction grating is provided, the light reflected by the optical disk 12 enters the light receiving sensor 14 without passing through the filter 8. Therefore, the wavelength selective polarization transmission film 8d may be a wavelength selection transmission film that transmits about 50% of the light emitted from the light emission point 2, for example, and transmits almost 100% of the light emitted from the light emission point 3, and the total transmission film 8e is also used. A film that transmits almost 100% of the light emitted from the light emitting points 2 and 3 may be used.

  As described above, the same effects as in the first embodiment can be obtained in the second embodiment by adopting the above-described configuration. Further, when the filter 8 is provided in the hologram element 10, since it moves with the objective lens 11, the recording / reproducing characteristics can be further improved.

(Embodiment 3)
FIG. 6 shows a perspective view of the optical disk apparatus according to Embodiment 3 of the present invention. In FIG. 6, the casing 21 is configured by combining an upper casing 21a and a lower casing 21b. The tray 22 is provided in the casing 21 so as to freely appear and disappear. The tray 22 is provided with a spindle motor 23 and an optical pickup device 24 which are rotational driving means for rotating the optical disk 12. The optical pickup device 24 includes an optical system having the filter 8 shown in the first or second embodiment, and performs at least one of an operation of writing information to the optical disc 12 or reading information. The light intensity distribution on the optical disk 12 at that time is as shown in FIG. In the tray 22, there is a feed drive system (not shown) which is a moving means for moving the optical pickup device 24 toward and away from the spindle motor 23. The bezel 25 is provided on the front end surface of the tray 22, and is configured to close the entrance and exit of the tray 22 when the tray 22 is stored in the housing 21. There are circuit boards (not shown) inside the casing 21 and the tray 22, and signal processing ICs, power supply circuits, and the like are mounted. An external connector 26 (not shown) is connected to a power / signal line provided in an electronic device such as a computer. Then, power is supplied into the optical disk apparatus via the external connector 26, an external electric signal is guided into the optical disk apparatus, or an electric signal generated by the optical disk apparatus is sent to an electronic device or the like. The optical disc apparatus equipped with the optical pickup device 24 including the optical system having the filter 8 shown in the first embodiment or the second embodiment as described above can record at high speed on the optical disc 12 used at any wavelength. Playback can also be performed.

  As described above, the optical pickup apparatus and the optical disk apparatus of the present invention can perform recording and reproduction at a high speed both in the CD system and the DVD system using a two-wavelength semiconductor laser light source, and can be used in electronic devices such as personal computers and notebook computers. It can use suitably for an apparatus.

Schematic of the optical system of the optical pickup device in Embodiment 1 of the present invention (A) is an enlarged top view of the filter part of Embodiment 1, (b) is an enlarged front view. (A) is a diagram comparing the light intensity distribution with and without the filter on the aperture surface of the objective lens, and (b) is a diagram comparing the light intensity distribution with and without the filter on the optical disc. Schematic of the optical system of the optical pickup device in Embodiment 2 of the present invention The enlarged view of the filter part of Embodiment 2. The perspective view of the optical disk apparatus in Embodiment 3 of this invention Schematic diagram of optical system of conventional optical pickup device

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Light emission point of 2 wavelength semiconductor laser light source 2 Light emission point of wavelength (lambda) 1 (650 nm) 3 Light emission point of wavelength (lambda) 2 (780 nm) 4 Diffraction grating 5 Integrated prism 6 Collimator lens 7 Light transmissive member 8 Filter (beam splitter)
8a Wavelength selective polarization separation film 8b Total transmission film 9 Rising prism 10 Hologram element 10a Polarization hologram 10b 1/4 wavelength plate 11 Objective lens 12 Optical disk 13 Front light monitor 14 Light receiving sensor

Claims (2)

A first light emitting point that emits light of a first wavelength;
A second light emitting point that emits light having a second wavelength longer than the first wavelength;
A light source in which the first light emitting point and the second light emitting point are provided close to each other;
A light receiving means for receiving the light reflected by the optical disc and generating an electrical signal;
An optical system for condensing the light emitted from each of the first light emitting point and the second light emitting point onto an optical disc and guiding the light reflected by the optical disc to the light receiving means;
The optical system has a light transmission member,
The light transmission member is composed of a surface facing the light source and a surface not facing the light source,
A filter is formed on the surface not facing the light source,
The filter is formed on a surface of the light transmission member and reflects light incident from the first light emission point and the second light emission point with different reflectances, and a surface of the wavelength selective separation film. A total reflection film that is formed in part and totally reflects light incident from the first light emission point and the second light emission point;
The total reflection film is formed so as to avoid the optical axis of the light emitted from the light source , changes the light intensity distribution by reflecting the light incident on the filter with the filter, and the first wavelength and the Different light intensity distribution from the second wavelength,
The surface facing the light emitting point is not parallel to the surface not facing the light emitting point, and the filter is formed with astigmatism of light emitted from the light emitting point at a position shifted from the optical axis of the optical system. An optical pickup device, wherein the surface is tilted in a direction to make it smaller than when the surface facing the light emitting point is parallel. An optical pickup device according to claim 1;
Rotation driving means for rotating the optical disc;
An optical disc apparatus comprising moving means for moving the optical pickup device closer to or away from the rotation driving means.

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