Now, some embodiments of an optical pickup according to this invention will be described in detail by referring to the accompanying drawings. It should be noted, however, that the present invention is not limited to the following embodiments and that various modifications and improvements may be made within a scope of this invention.
As shown in
As shown in
It is desired that the diffractive lens structure of the first objective lens 10 be designed so that a diffracted light 16 of first diffraction order (m1=1) from a beam 15 for CD 11 having a wavelength λ1 and a diffracted light 18 of second diffraction order (m3=2) from a beam 17 for the first next generation DVD having a wavelength λ3 satisfy the following requirement for the ratio of wavelengths multiplied by diffraction orders:
0.75≦(λ1×m1)/(λ3×m3)≦0.99 (1)
that is,
0.75≦(λ1×1)/(λ3×2)≦0.99.
Substituting into the above expression the center values of the laser wavelengths currently in use, i.e., the wavelength for CD λ1=785 nm and the wavelength for HD λ3=405 nm, the resultant ratio of wavelengths is (λ2×1)/(λ3×2)=(785×1)/(405×2)=785/810≈0.97. This satisfies the above design condition (1).
As shown in
It is desired that the diffractive lens structure be designed so that a diffracted light 26 of second diffraction order (m2=2) from a beam 25 for DVD 21 having a wavelength λ2 and a diffracted light 28 of third diffraction order (m4=3) from a beam 27 for the second next generation DVD such as BD 22 having a wavelength λ4 satisfy the following requirement for the ratio of wavelengths multiplied by diffraction orders:
0.75≦(λ4×m4)/(λ2×m2)≦0.99 (2)
that is,
0.75≦(λ4×3)/(λ2×2)≦0.99.
Substituting into the above expression the center values of the laser wavelengths currently in use, i.e., the wavelength for DVD λ2=660 nm and the wavelength for BD λ4=405 nm, the resultant ratio of wavelengths is (λ4×3)/(λ2×2)=(405×3)/(660×2)=1215/1320≈0.92. This satisfies the above design condition (2).
A CD beam 32 emitted from the CD laser 31 passes through the lens 33, a diffraction grating 34, a polarization beam splitter 35 and a half waveplate 36 and is reflected by a polarization beam splitter 37. Then, the beam passes through a lens 38, which forms a spherical aberration correction means 30, and is reflected by a mirror 39. It then passes through a quarter waveplate 40 and enters an objective lens 10 which focuses it on the CD 11, as explained in connection with
After being reflected by the CD 11, the beam passes through the objective lens 10 and the quarter waveplate 40 and is reflected by the mirror 39. It then passes through the lens 38, the polarization beam splitter 37 and a lens 41 before entering a photodetector 42.
An HD beam 44 emitted from the HD laser 43 passes through a lens 45 and is reflected by the polarization beam splitter 35. It then passes through the half waveplate 36 and is reflected by the polarization beam splitter 37. Then it passes through the lens 38, which forms the spherical aberration correction means 30, and is reflected by the mirror 39. The beam then passes through the quarter waveplate 40 and enters the objective lens 10 which focuses the beam on the HD 12, as explained in connection with
After being reflected from the HD 12, the light passes through the objective lens 10 and the quarter waveplate 40 and is reflected by the mirror 39. It then passes through the lens 38, polarization beam splitter 37 and lens 41 and enters the photodetector 42.
A DVD beam 47 emitted from the DVD laser 46 passes through a lens 48, a diffraction grating 49, a polarization beam splitter 50 and a half waveplate 51 and is reflected by a polarization beam splitter 52. It then passes through a lens 53, which forms the spherical aberration correction means 30, and is reflected by a mirror 54. The light then passes through a quarter waveplate 55 and enters an objective lens 20 which focuses it on the DVD 21, as explained in connection with
After being reflected by the DVD 21, the light passes through the objective lens 20 and the quarter waveplate 55 and is reflected by the mirror 54. It then passes through the lens 53, the polarization beam splitter 52 and a lens 56 and enters a photodetector 57.
A BD beam 59 emitted from the BD laser 58 passes through a lens 60 and is reflected by the polarization beam splitter 50. It then passes through the half waveplate 36 and is reflected by the polarization beam splitter 52. Then it passes through the lens 53, which forms the spherical aberration correction means 30, and is reflected by the mirror 54. It further passes through the quarter waveplate 55 and enters the objective lens 20, which focuses it on the BD 22, as explained in connection with
After being reflected by the BD 22, the light passes through the objective lens 20 and the quarter waveplate 55 and is reflected by the mirror 54. It then passes through the lens 53, the polarization beam splitter 52 and the lens 56 before entering the photodetector 57.
The spherical aberration correction means 30 comprises the lens 38 and the lens 53 and is designed to be able to change the spherical aberration correction. The lens 38, in combination with the objective lens 10, corrects the spherical aberrations of the CD 11 and the HD 12 well. The lens 53, in combination with the objective lens 20, corrects the spherical aberrations of the DVD 21 and the BD 22 well.
To omit the lens 38, the design needs to satisfy the following condition in stead of the condition of equation (1).
0.75≦(λ1×m1)/(λ3×m3)≦0.87 (3)
That is, in the case of the first embodiment, the following condition must be met.
0.75≦(λ1×1)/(λ3×2)≦0.87
Where the condition of equation (3) is met, if the lens 38 is used rather than being omitted, the degree of freedom in the spherical aberration correction design for the objective lens 10 increases, making it possible to better correct the spherical aberration.
To omit the lens 53, the design needs to satisfy the following condition in stead of the condition of equation (2).
0.75≦(λ4×m4)/(λ2×m2)≦0.87 (4)
That is, in the case of the first embodiment, the following condition must be met.
0.75≦(λ4×3)/(λ2×2)≦0.87
If the lens 53 is used rather than being omitted even when the condition of equation (4) is met, the degree of freedom in the spherical aberration correction design for the objective lens 10 increases, making it possible to better correct the spherical aberration.
Although in the first embodiment the wavelength of the laser beam for reading and writing the next-generation DVDs is set at 405 nm, it is not limited to this wavelength. For example, a laser beam with a wavelength of 400-410 nm or 440-450 nm may be used.
In the second embodiment, the CD is supposed to have a wavelength λ1 of 785 nm and the HD a wavelength λ3 of 445 nm. In this case, the ratio of wavelengths is
(λ1×1)/(λ3×2)=(785×1)/(445×2)=785/890≈0.88
This is close to the value of the design condition (3) for the wavelength ratio, so this embodiment can correct the spherical aberration better than the first embodiment.
When the wavelength λ3 is changed from 405 nm to 445 nm, the numerical aperture of the HD of the objective lens 10 needs to be changed. Since the wavelength λ and the numerical aperture NA are inversely proportional to each other, if the numerical aperture NA=0.65 when the wavelength λ3=405 nm, then the numerical aperture for the wavelength λ3=445 nm is given by
NA=(0.65×445)/405=0.714
In the third embodiment, the CD is supposed to have a wavelength λ1 of 785 nm and the HD a wavelength λ3 of 473 nm. In this case, the ratio of wavelengths is
(λ1×1)/(λ3×2)=(785×1)/(473×2)=785/946≈0.83
This satisfies the design condition (3) for the wavelength ratio, so this embodiment can correct the spherical aberration better than the second embodiment.
The numerical aperture NA for the wavelength λ3=473 nm therefore is
NA=(0.65×473)/405=0.759
Although in the first embodiment, the diffractive lens structure of the second compatible objective uses a diffracted light of second diffraction order (m2=2) from a beam for DVD with a wavelength λ2 and a diffracted light of third diffraction order (m4=3) from a beam for second next-generation DVD with a wavelength λ4, this invention is not limited to this structure. The spherical aberration correction can further be improved by changing a combination of diffraction orders.
In the fourth embodiment, a combination of diffraction orders is m2=3 and m4=4.
Using the center values of the laser wavelengths currently in use, i.e., the wavelength for DVD λ2=660 nm and the wavelength for BD λ4=405 nm, the resultant ratio of wavelengths multiplied by the diffraction orders is
(λ4×m4)/(λ2×m2)=(405×4)/(660×3)=1620/1980≈0.82. This satisfies the above design condition (4).
As described above, the optical pickup according to this invention has two compatible objectives and a spherical aberration correction means, the two compatible objectives being a first compatible objective having a diffractive lens structure capable of reading and writing two kinds of optical discs—CD and first next-generation DVD—and a second compatible objective having a diffractive lens structure capable of reading and writing two kinds of optical discs—DVD and second next-generation DVD. The diffractive lens structure of the first objective is designed so that a diffracted light of diffraction order m1 from a beam for CD with a wavelength λ1 and a diffracted light of diffraction order m3 from a beam for first next-generation DVD satisfy the following requirement for a ratio of the wavelengths multiplied by the diffraction orders:
0.75≦(λ1×m1)/(λ3×m3)≦0.99 (1)
The first compatible objective has a wavelength dependency such that, when combined with the spherical aberration correction means, the first objective can form good wave fronts for the two kinds of optical discs. The diffractive lens structure of the second compatible objective is designed so that a diffracted light of diffraction order m2 from a beam for DVD with a wavelength λ2 and a diffracted light of diffraction order m4 from a beam for second next-generation DVD satisfy the following requirement for a ratio of the wavelengths multiplied by the diffraction orders:
0.75≦(λ4×m4)/(λ2×m2)≦0.99 (2)
The second compatible objective has a wavelength dependency such that, when combined with the spherical aberration correction means, the second compatible objective can form good wave fronts for the two kinds of optical discs. The optical pickup according to this invention can correct spherical aberrations of the diffracted light of diffraction orders determined by the diffractive lens structures of the first and second compatible objectives and also focus them on the respective disc recording surfaces. The optical pickup also has a high light utilization. With this invention, an compatible optical pickup can be provided which can perform read/write operations on four kinds of optical discs—CDs, DVDs, first next-generation DVDs and second next generation DVDs.
The embodiments of the optical pickup according to the present invention have been described in detail. It is noted that this invention is not limited to these embodiments and that various improvements and modifications may be made without departing from the spirit and scope of this invention.
While in the above embodiments the first objective is constructed as a CD-HD compatible objective capable of reading and writing both CD and HD and the second objective is constructed as a DVD-BD compatible objective capable of reading and writing both DVD and BD, this invention is not limited to this construction. For example, the first objective may be constructed to focus a diffracted light from a laser beam of wavelength λ1 on a layer of CD in which information is recorded and also to focus a diffracted light from a laser beam of wavelength λ4 on a layer of BD in which information is recorded. The second objective may be constructed to focus a diffracted light from a laser beam of wavelength λ2 on a layer of DVD in which information is recorded and also to focus a diffracted light from a laser beam of wavelength λ3 on a layer of HD DVD in which information is recorded.
In the above embodiments, while a laser beam source for reading and writing the HD DVD and a laser beam source for reading and writing the BD are provided separately, a single laser beam source may be shared.
With this invention, the optical pickup can perform the reading and writing operations on a plurality of kinds of optical discs that use different wavelengths.
Number | Date | Country | Kind |
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2007-173288 | Jun 2006 | JP | national |