USPatent applicationPatented

Optical head unit and optical information writing/reading device

Granted 10 Jul 2007 · 2 office actions

Current assignee: NEC Corporation · originally AT&T Company

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Attorney: Attorney · Log in to unlock

Inventors: Ryuichi Katayama · Examiner: Gautam R. Patel · AU 2627 · TC 2600

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Abstract

An optical head unit is provided including a first light source emitting a light with a first wavelength, a second light source emitting a light with a second wavelength, and a third light source emitting a light with a third wavelength. The optical head unit also includes a first objective lens irradiating the light emitted from the first light source onto an optical recording medium, a second objective lens irradiating the light emitted from the second light source or the light emitted from the third light source onto an optical recording medium, and a photodetector receiving a reflected light from the optical recording medium.

Description

9 parts
›BACKGROUND OF THE INVENTION · 1 of 2

1. Field of the Invention

The present invention relates to an optical head unit and optical information writing/reading device, and more particularly, to an optical head unit and an optical information writing/reading device having a plurality of objective lenses.

2. Description of the Related Art

A recording density of an optical information writing/reading device is inversely proportional to a square of the diameter of a focal spot formed on an optical recording medium by an optical head unit. In other words, the smaller the diameter of the focal spot, the higher the recording density. The diameter of the focal spot is proportional to a wavelength of a light source and is inversely proportional to a numerical aperture of an objective lens. In other words, the shorter the wavelength of the light source and the higher the numerical aperture of the objective lens, the smaller the diameter of the focal spot. On the other hand, when an optical recording medium (optical disc) is tilted to an objective lens, the shape of a focal spot is fluctuated due to coma aberration, resulting in deterioration of the writing/reading characteristic. The coma aberration is inversely proportional to the wavelength of a light source and is proportional to the cube of the numerical aperture of the objective lens and the thickness of a protective layer of an optical recording medium. When the thicknesses of protective layers of optical recording media are the same, the shorter the wavelength of the light source and the higher the numerical aperture of the objective lens, the margin of the tilt of the optical recording medium with respect to the writing/reading characteristic is narrower.

In an optical information writing/reading device which shortens the wavelength of a light source and increases the numerical aperture of an objective lens to increase the recording density, the thickness of a protective layer of an optical recording medium is smaller to secure the margin of the tilt of the optical recording medium with respect to the write/read characteristic. For example, in a standard CD (compact disc) having a capacity of 650 MB, the wavelength of a light source is 780 nm, the numerical aperture of an objective lens is 0.45, and the thickness of a protective layer of an optical disc is 1.2 mm. In a standard DVD (digital versatile disc) having a capacity of 4.7 GB, the wavelength of a light source is 650 nm, the numerical aperture of an objective lens is 0.6, and the thickness of a protective layer of an optical disc is 0.6 mm.

In a typical optical head, an objective lens is designed to cancel a spherical aberration to an optical disc having a protective layer having a certain thickness. When writing and reading are performed onto/from optical discs having protective layers having different thicknesses, the spherical aberration remains and correct writing and reading cannot be performed. Accordingly, there is proposed an optical head unit having a compatible function which can perform writing and reading onto/from both of an optical disc of the DVD standard and an optical disc of the CD standard. Such kind of optical head units are classified into one using a single objective lens and one using a plurality of objective lenses. The optical head unit using a plurality of objective lenses has a construction slightly more complicated than that of the optical head unit using a single objective lens. However, the respective objective lenses can be optimally designed for the optical discs of the respective standards, so that the writing/reading performance to the optical discs of the respective standards is excellent.

As an example of a prior art optical head unit using a plurality of objective lenses, which can perform writing and reading onto/from both of an optical disc of the DVD standard and an optical disc of the CD standard, Japanese Published Application 2000-242943 discloses an optical head unit shown in FIG. 1 .

As shown in FIG. 1 , an optical head unit 101 in the prior art has a first optical system 102 a , a second optical system 102 b , a first objective lens 103 a mounted on a first actuator 104 a, and a second objective lens 103 b mounted on a second actuator 104 b.

The first optical system 102 a and the second optical system 102 b have a semiconductor laser, not shown, as a light source. A photodetector, not shown, receives a light from an optical disc 105 of the DVD standard or the CD standard. The wavelength of an emitted light of the semiconductor laser in the first optical system 102 a is 650 nm, and the wavelength of an emitted light of the semiconductor laser in the second optical system 102 b is 780 nm.

The emitted light from the semiconductor laser in the first optical system 102 a is incident upon the first objective lens 103 a and is focused onto the optical disc 105 of the DVD standard having a protective layer having a thickness of 0.6 mm. A reflected light from the optical disc 105 passes through the first objective lens 103 a in the reverse direction to be received by the photodetector in the first optical system 102 a . In addition, the emitted light from the semiconductor laser in the second optical system 102 b is incident upon the second objective lens 103 b and is focused onto the optical disc 105 of the CD standard having a protective layer having a thickness of 1.2 mm. A reflected light from the optical disc 105 passes through the second objective lens 103 b in the reverse direction to be received by the photodetector in the second optical system 102 b.

The first objective lens 103 a has a spherical aberration canceling a spherical aberration caused when the light with a wavelength of 650 nm passes through the protective layer having a thickness of 0.6 mm of the optical disc 105 . The second objective lens 103 b has a spherical aberration canceling a spherical aberration caused when the light with a wavelength of 780 nm passes through the protective layer having a thickness of 1.2 mm of the optical disc 105 .

›BACKGROUND OF THE INVENTION · 2 of 2

The optical head unit 101 is moved between the innermost circumference and the outermost circumference of the optical disc 105 in the direction of the arrows of FIG. 1 along two rails 106 a and 106 b arranged in parallel with each other.

In FIG. 1 , the numeral 131 a denotes a first optical path connecting the first optical system 102 a and the first objective lens 103 a , and the numeral 131 b denotes a second optical path connecting the second optical system 102 b and the second objective lens 103 b.

In recent years, to increase the recording density, there has been proposed a next-generation standard in which the wavelength of a light source is shorter, the numerical aperture of an objective lens is higher, and the thickness of a protective layer of an optical recording medium (optical disc) is smaller. For example, with the name of Blu-ray Disc (BD), there has been proposed a next-generation standard having a capacity of 23.3 GB in which the wavelength of a light source is 405 nm, the numerical aperture of an objective lens is 0.85, and the thickness of a protective layer (cover layer) of an optical disc is 0.1 mm. Accordingly, what is desired is an optical head unit having a compatible function which can perform writing and reading onto/from any of an optical disc of such next-generation standard and conventional optical discs of the DVD standard and the CD standard. However, there has not yet been an optical head unit using a plurality of objective lenses which can perform writing and reading onto/from any of the optical disc of the next-generation standard and the conventional optical discs of the DVD standard and the CD standard.

›SUMMARY OF THE INVENTION

To overcome the problems in the prior art described above, and to overcome other problems that will become apparent to one of ordinary skill in the art upon reading and understanding the present specification, the present invention discloses an optical head unit and optical information writing/reading device.

The present invention provides an optical head unit having a plurality of objective lenses and an optical information writing/reading device, which can write and read information onto/from optical discs of any standard.

According to a first aspect of the present invention, an optical head unit comprises a first light source emitting a light with a first wavelength, a second light source emitting a light with a second wavelength, a third light source emitting a light with a third wavelength, a first objective lens irradiating the light emitted from the first light source onto an optical recording medium, a second objective lens irradiating the light emitted from the second light source or the light emitted from the third light source onto an optical recording medium, and a photodetector receiving a reflected light from the optical recording medium.

›BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a plan view showing the schematic construction of a prior art optical head unit.

FIG. 2 is a plan view showing the schematic construction of an optical head unit of a first embodiment of the present invention.

FIG. 3 is a view showing the construction of a first optical system used in the optical head unit of FIG. 2 .

FIG. 4 is a view showing the construction of a second optical system used in the optical head unit of FIG. 2 .

FIG. 5( a ) is a view showing the construction of an objective lens used in the first optical system of the optical head unit of FIG. 2 , and FIG. 5( b ) is a view showing the construction of an objective lens used in the second optical system of the optical head unit of FIG. 2 .

FIGS. 6( a ) and ( b ) are views showing the constructions of photodetectors used in the optical head unit of FIG. 2 and light spots.

FIG. 7 is a diagram showing the relation between the angle deviation between the tracks of an optical disc and the division lines of the photodetectors and the offsets (calculated values) of focus error signals (astigmatism signals) with it in the optical head unit of FIG. 2 .

FIG. 8 is a diagram showing the relation between the angle deviation between the tracks of an optical disc and the division lines of the photodetectors and the modulation factors (calculated values) of track error signals (push-pull signals) with it in the optical head unit of FIG. 2 .

FIG. 9 is a view showing the position relation between the centers of the objective lenses and the center of the optical disc in the optical head unit of FIG. 2 .

FIG. 10 is an explanatory view showing the construction of a diffraction optical device used in the optical head unit of FIG. 2 .

FIG. 11 is a plan view showing the schematic construction of an optical information writing/reading device of a second embodiment of the present invention.

›DETAILED DESCRIPTION OF THE INVENTION · 1 of 5

A schematic construction of an optical head unit 1 of a first embodiment of the present invention is shown in FIG. 2 . As shown in FIG. 2 , the optical head unit 1 has a first optical system 2 a , a second optical system 2 b , a first actuator 4 a , a second actuator 4 b , a first objective lens 3 a mounted on the first actuator 4 a , and a second objective lens 3 b mounted on the second actuator 4 b . The first optical system 2 a and the second optical system 2 b each have a semiconductor laser as a light source, and a photodetector receiving a reflected light from an optical disc 5 of the next-generation standard, the DVD standard or the CD standard. An illustrative wavelength of an emitted light of the semiconductor laser in the first optical system 2 a is 405 nm. An illustrative wavelength of an emitted light of the semiconductor laser in the second optical system 2 b is 650 nm or 780 nm. As indicated by the arrows in FIG. 2 , the optical head unit 1 is moved between the innermost circumference and the outermost circumference of the optical disc 5 along two rails 6 a and 6 b arranged in parallel with each other.

The emitted light (wavelength of 405 nm) from the semiconductor laser in the first optical system 2 a is incident via a first optical path 31 a upon the first objective lens 3 a to be focused onto the optical disc 5 . A reflected light from the optical disc 5 passes through the first objective lens 3 a in the reverse direction to be received by the photodetector in the first optical system 2 a.

The emitted light (wavelength of 650 nm) from one of the semiconductor lasers in the second optical system 2 b is incident via a second optical path 31 b upon the second objective lens 3 b to be focused onto the optical disc 5 . A reflected light from the optical disc 5 passes through the second objective lens 3 b in the reverse direction to be received by the photodetector in the second optical system 2 b . The emitted light (wavelength of 780 nm) from the other of the semiconductor lasers in the second optical system 2 b is incident via the second optical path 31 b upon the second objective lens 3 b to be focused onto the optical disc 5 . A reflected light from the optical disc 5 passes through the second objective lens 3 b in the reverse direction to be received by the photodetector in the second optical system 2 b.

The first objective lens 3 a has a spherical aberration canceling a spherical aberration caused when the light with a wavelength of 405 nm passes through a protective layer having a thickness of 0.1 mm and is optimized for the optical recording medium of the next-generation standard. To this, the second objective lens 3 b has a spherical aberration substantially canceling a spherical aberration caused when the light with a wavelength of 650 nm passes through a protective layer having a thickness of 0.6 mm and has a spherical aberration substantially canceling a spherical aberration caused when the light with a wavelength of 780 nm passes through a protective layer having a thickness of 1.2 mm. In other words, the spherical aberration of the second objective lens 3 b is set to substantially cancel a spherical aberration caused when the light with a wavelength of 650 nm passes through the protective layer having a thickness of 0.6 mm and to substantially cancel a spherical aberration caused when the light with a wavelength of 780 nm passes through the protective layer having a thickness of 1.2 mm. In this way, the second objective lens 3 b is not optimized for only the optical disc of the DVD standard or only the optical disc of the CD standard. However, its remaining spherical aberration is within the allowable range for any of the DVD standard and the CD standard. Thus, the second objective lens 3 b can correctly write and read information onto/from the optical disc of any of the DVD standard and the CD standard.

The construction of the first optical system 2 a is shown in FIG. 3 . The emitted light with a wavelength of 405 nm from a semiconductor laser 7 a is divided into three lights of a zero order light and ± first order diffraction lights by a diffraction optical device 8 a . These three lights are collimated by a collimator lens 9 a to be incident as P polarized light upon a polarization beam splitter 10 a . Almost of these lights pass through the polarization beam splitter 10 a . Thereafter, they pass through a ¼ wave plate 11 a to be converted from a linearly polarized light to a circularly polarized light, and further pass through a relay lens 12 a and a relay lens 12 b to be irradiated upon the optical disc 5 by the first objective lens 3 a.

The reflected lights (wavelength of 405 nm) from the optical disc 5 pass through the first objective lens 3 a in the reverse direction, and then pass through the relay lens 12 b and the relay lens 12 a in the reverse direction. Further, they pass through the ¼ wave plate 11 a to be converted from a circularly polarized light to a linearly polarized light which the polarization direction is orthogonal to that in the going path. They are then incident as S polarized light upon the polarization beam splitter 10 a for reflection of almost of them, and pass through a cylindrical lens 13 a and a lens 14 a to be received by a photodetector 15 a.

The photodetector 15 a of the first optical system 2 a is arranged in about the middle of two focal lines of the cylindrical lens 13 a and the lens 14 a.

Generally, when the thickness of a protective layer of an optical disc is deviated from the design value, a spherical aberration caused by the thickness deviation of the protective layer fluctuates the shape of the focal spot on the optical disc, resulting in deterioration of the writing/reading characteristic. The spherical aberration is inversely proportional to the wavelength of a light source and is proportional to the biquadrate of the numerical aperture (NA) of an objective lens. The shorter the wavelength of the light source and the higher the numerical aperture of the objective lens, the margin of the thickness deviation of the protective layer of the optical disc with respect to the writing/reading characteristic is narrower. For example, when the wavelength of the semiconductor laser 7 a as the light source is 405 nm and the numerical aperture of the objective lens 3 a is 0.85, the margin of the thickness deviation of the protective layer is insufficient. The thickness deviation of the protective layer of the optical disc 5 may be corrected. When any one of the relay lens 12 a and the relay lens 12 b is moved in its optical axis direction by the actuator, not shown, the magnification of the first objective lens 3 a is changed to vary the spherical aberration. The position of the optical axis direction of any one of the relay lenses 12 a and 12 b is adjusted to cause a spherical aberration canceling a spherical aberration caused by the thickness deviation of the protective layer of the optical disc 5 by the first objective lens 3 a . The thickness deviation of the protective layer of the optical disc 5 can be corrected to eliminate adverse affection on the writing/reading characteristic.

›DETAILED DESCRIPTION OF THE INVENTION · 2 of 5

The construction of the second optical system 2 b is shown in FIG. 4 . The emitted light with a wavelength of 650 nm from a semiconductor laser 7 b is divided into three lights of a zero order light and ± first order diffraction lights by a diffraction optical device 8 b . These three lights are collimated by a collimator lens 9 b to be incident as the S polarized light upon a polarization beam splitter 10 b . Almost all of these lights are reflected by the polarization beam splitter 10 b, and almost all of them pass through a polarization beam splitter 10 c . Thereafter, they pass through a ¼ wave plate 11 b to be converted from a linearly polarized light to a circularly polarized light and are irradiated onto the optical disc 5 by the second objective lens 3 b.

The reflected lights (wavelength of 650 nm) from the optical disc 5 pass through the second objective lens 3 b in the reverse direction, and then pass through the ¼ wave plate 11 b to be converted from a circularly polarized light to a linearly polarized light which the polarization direction is orthogonal to that in the going path. Almost all of the reflected lights pass through the polarization beam splitter 10 c to be incident as the P polarized light upon the polarization beam splitter 10 b . Almost all of them pass therethrough, thereby passing through a cylindrical lens 13 b and a lens 14 b to be received by a photodetector 15 b.

In addition, the emitted light with a wavelength of 780 nm from a semiconductor laser 7 c is divided into three lights of a zero order light and ± first order diffraction lights by a diffraction optical device 8 c . These three lights are collimated by a collimator lens 9 c to be incident as the S polarized light upon a polarization beam splitter 10 c . Almost all of these lights are reflected by the polarization beam splitter 10 c . They pass through the ¼ wave plate 11 b to be converted from a linearly polarized light to a circular polarized light and are irradiated onto the optical disc 5 by the second objective lens 3 b.

The reflected lights (wavelength of 780 nm) from the optical disc 5 pass through the second objective lens 3 b in the reverse direction, and then pass through the ¼ wave plate 11 b to be converted from a circular polarized light to a linearly polarized light which the polarization direction is orthogonal to that in the going path. The reflected lights are incident as the P polarized light upon the polarization beam splitter 10 c so that almost all of them pass therethrough. Almost all of them pass through the polarization beam splitter 10 b , thereby passing through the cylindrical lens 13 b and the lens 14 b to be received by the photodetector 15 b.

The photodetector 15 b of the second optical system 2 b is arranged in about the middle of two focal lines of the cylindrical lens 13 b and the lens 14 b.

FIGS. 5( a ) and 5 ( b ) show illustrative examples of the first objective lens 3 a and the second objective lens 3 b , respectively. The first objective lens 3 a has a numerical aperture of 0.85. As shown in, FIG. 5( a ), the first objective lens 3 a has two lenses in two groups of a first lens 16 a and a second lens 16 b . As a specific example of such objective lens having two lenses in two groups, for example, there is one described in Japanese Journal of Applied Physics, Vol. 36, pp. 456–459.

The first objective lens 3 a can also be constructed by a single lens. As a specific example of an objective lens having a single lens, there is one described in International Symposium on Optical Memory-2001, Technical Digest, pp. 26–27.

The light with a wavelength of 405 nm incident upon the first objective lens 3 a is focused onto the optical disc 5 a of the next-generation standard having the protective layer having an illustrative thickness of 0.1 mm to form an optimum light spot.

In the second objective lens 3 b , the numerical aperture to the light with the wavelength of 650 nm is 0.6, and the numerical aperture to the light with a wavelength of 780 nm is 0.45. It may be constructed by a diffraction-refraction combined lens formed with a diffraction grating on a first surface. As a specific example of such objective lens having a diffraction-refraction combined lens, there is one described in Optical Design and Fabrication 2000, Proceedings, pp. 93–96.

The light with a wavelength of 650 nm incident upon the second objective lens 3 b is focused onto the optical disc 5 b of the DVD standard having the protective layer having a thickness of 0.6 mm to form a light spot. The light with a wavelength of 780 nm incident upon the second objective lens 3 b is focused onto the optical disc 5 c of the CD standard having the protective layer having a thickness of 1.2 mm to form a preferable light spot.

The first objective lens 3 a is optimally designed to the optical disc of the next-generation standard and can obtain writing/reading performance sufficient for the optical disc of the next-generation standard having a narrow writing/reading margin. On the other hand, the second objective lens 3 b is not optimally designed for only the optical disc of the DVD standard or the optical disc of the CD standard but is designed for both. The optical disc of the DVD standard and the optical disc of the CD standard have a relatively wide writing/reading margin.

The construction of the photodetector 15 a of the first optical system 2 a is shown in FIG. 6( a ). The photodetector 15 a has, for the zero order light, light reception parts 18 a , 18 b , 18 c and 18 d divided into four by a division line in parallel with the radius direction of the optical disc 5 and a division line in parallel with the tangent direction of the optical disc 5 , and for the +1 order diffraction light, light reception parts 18 e and 18 f divided into two by a division line in parallel with the radius direction of the optical disc 5 , and for the −1 order diffraction light, light reception parts 18 g and 18 h divided into two by a division line in parallel with the radius direction of the optical disc 5 . The radius direction is a direction along which the optical head unit moves from an innermost portion of the optical disc to an outermost portion of the optical disc. The tangent direction is perpendicular to the radius direction. In addition, the light reception parts are in order of the tangent direction. In FIG. 2 , the parallel direction with the rail is the radius direction.

›DETAILED DESCRIPTION OF THE INVENTION · 3 of 5

The zero order light of three reflected lights from the optical disc 5 forms a light spot 17 a on the four light reception parts 18 a , 18 b , 18 c and 18 d . The +1 order diffraction light of the reflected lights forms a light spot 17 b on the two light reception parts 18 e and 18 f . The −1 order diffraction light of the reflected lights forms a light spot 17 c on the two light reception parts 18 g and 18 h.

Electric signal outputs obtained from the eight light reception parts 18 a to 18 h of the photodetector 15 a are expressed as V 18 a to V 18 h , respectively. A focus error signal is obtained from operation of (V 18 a +V 18 d )−(V 18 b +V 18 c ) by a known “astigmatism method”. A track error signal is obtained from operation of (V 18 a +V 18 b )−(V 18 c +V 18 d )−K [(V 18 e +V 18 g )−(V 18 f +V 18 h ) (K is a constant.) by a known “difference push-pull method”. An RF signal (data signal) from the optical disc 5 is obtained from operation of (V 18 a +V 18 b +V 18 c +V 18 d ).

The construction of the photodetector 15 b of the second optical system 2 b is the same as shown in FIG. 6( a ).

In addition, in this embodiment, when the optical head unit 1 is moved between the innermost circumference and the outermost circumference of the optical disc 5 , distance La between a straight line including a track of the center of the first objective lens 3 a and the center O of the optical disc 5 may be shorter than distance Lb between the straight line including the track of the center of the second objective lens 3 b and the center O of the optical disc 5 as shown in FIG. 2 . In other words, La<Lb may be set.

When the optical head unit 1 is moved between the innermost circumference and the outermost circumference of the optical disc 5 and the straight line including the track of the center of the objective lens 3 a or 3 b does not pass through center O of the optical disc 5 , the angle between the tracks of the optical disc 5 and the division lines of the photodetectors 15 a, 15 b (division lines in parallel with the tangent direction of the optical disc 5 ) is changed according to the radius of the optical disc 5 where the center of the objective lens 3 a or 3 b is positioned. When the angle is deviated from 0°, offset occurs in the focus error signal of the “astigmatism method” and the modulation factor of the track error signal of the “push-pull method” is lowered.

FIG. 7 shows results calculated by standardizing, by sum signals, the offsets of the focus error signals of the “astigmatism method” with angle deviation between the tracks of the optical disc 5 and the division lines of the photodetectors 15 a , 15 b (division lines in parallel with the tangent direction of the optical disc 5 ) in the optical discs 5 of the next-generation standard using a blue light, the DVD standard, and the CD standard. In addition, FIG. 8 shows results calculated by standardizing, by sum signals, the modulation factors of the track error signals of the “push-pull method” with the angle deviation in the optical discs 5 of these three standards.

In FIG. 7 and FIG. 8 , a, curved line of the next-generation standard (blue) mostly corresponds with a curved line of the DVD standard.

As shown in FIG. 8 , the modulation factor of the track error signal is not lowered to about 20° of angle deviation. As shown in FIG. 7 , the offsets of the focus error signals are increased in proportion to increase of angle deviation. Comparing a slope of the curved line of the next-generation standard, the DVD standard, with the CD standard in a scope of 0° to 25° of angle deviation, the offsets of the focus error signals in the next-generation standard (blue) and the DVD standard are about ¾ of the offset of the focus error signal in the CD standard. However, the allowable value of the offset of the focus error signal is generally proportional to the wavelength of the light source and is inversely proportional to the square of the numerical aperture of the objective lens. The allowable values of the offsets of the focus error signals in the next-generation standard and the DVD standard are, for example, about 15% and about 47% of the allowable value of the offset of the focus error signal in the CD standard, respectively. Accordingly, the percentage of the offset of the focus error signal caused with the angle deviation to its allowable value is the largest in the next-generation standard. Therefore, the less angle deviation amount in the next-generation standard, the more effective to avoid a decrease in the focus error signal as compared to the angle deviation amount in the DVD standard or the CD standard.

According to setting the position of the objective lens, the angle deviation amount between the tracks of the optical disc 5 of the next-generation standard and the division line of the photodetector is smaller than that between the tracks of the optical discs 5 of the DVD standard and the CD standard and the division line of the photodetector.

FIG. 9 shows the position relation between the centers of the objective lenses and the center O of the optical disc 5 .

As shown in FIG. 9 , the distance between straight line L including the tracks of the centers of the objective lenses when the optical head unit 1 is moved between the innermost circumference and the outermost circumference of the optical disc 5 and the center of the optical disc 5 is D, and the radiuses of the innermost circumference and the outermost circumference of the optical disc 5 are R min and R max , respectively. The angle deviation amounts between the tracks of the innermost circumference and the outermost circumference of the optical disc 5 and the division line of the photodetector 15 a (see FIG. 6 ) are θ min and θ max , respectively, by the following equations.

sin θ min =D/R min , sin θ max =D/R max

The division line of the photodetector 15 a may be tilted with respect to the direction orthogonal to the tracks of the centers of the objective lenses (that is, the straight line L) by (θi min +θ max )/2 as a photodetector 15 c shown in FIG. 6( b ). Accordingly, both of the angle deviation amounts between the tracks of the innermost circumference and the outermost circumference of the optical disc 5 and the division line of the photodetector 15 c can be reduced to (θ max −θ min )/2.

›DETAILED DESCRIPTION OF THE INVENTION · 4 of 5

The light spots 17 d , 17 e and 17 f of FIG. 6( b ) correspond to the light spots 17 a , 17 b and 17 c of FIG. 6( a ), respectively. The light reception parts 18 i to 18 p of FIG. 6( b ) correspond to the light reception parts 18 a to 18 h of FIG. 6( a ), respectively. The construction shown in FIG. 6( b ) is the same as the construction shown in FIG. 6( a ) except that the two division lines in parallel with the radius direction and the tangent direction of the optical disc 5 are tilted with respect to the direction orthogonal to the tracks of the centers of the objective lenses (that is, the straight line L) by (θ min +θ max )/2.

In the same manner, the photodetector 15 b may be replaced by the construction shown in FIG. 6( b ).

In a case that the straight line L including the tracks of the centers of the objective lenses 3 a , 3 b when the optical head unit 1 is moved between the innermost circumference and the outermost circumference of the optical disc 5 does not pass through the center of the optical disc 5 , the angle between the track of the optical disc 5 and the focal spot row on the optical disc 5 is changed according to the radius of the optical disc 5 where the centers of the objective lens 3 a, 3 b are positioned. Therefore, the phase between the push-pull signal of the new order light and that of the ±1 order diffraction lights may be compensated according to the angle between the track of the optical disc 5 and the focal point row on the optical disc 5 to avoid a change of an amplitude of the track error signal by the “difference push-pull method”. Instead, a diffraction optical device formed with the grating pattern shown in FIG. 10 may be used as the diffraction optical device 8 a.

The diffraction grating pattern of FIG. 10 is divided into four areas 19 a , 19 b , 19 c and 19 d by a straight line in parallel with the radius direction of the optical disc 5 and a straight line in parallel with the tangent direction of the optical disc 5 passing through the optical axis of an incident light. The phases of the gratings in the areas 19 a , 19 d and the phases of the gratings in the areas 19 b , 19 c are shifted from each other by π/2. In other words, the phase of the grating in the area 19 a is shifted from the phase of the grating in the area 19 b by π/2 and is also shifted from the phase of the grating in the area 19 c by π/2. The phase of the grating in the area 19 d is shifted from the phase of the grating in the area 19 b by π/2 and is also shifted from the phase of the grating in the area 19 c by π/2.

According to the diffraction grating pattern as shown in FIG. 10 , the amplitude of the push-pull signals of the ± first order diffraction lights from the diffraction optical device 8 a as the sub beam is always 0. Therefore, the amplitude of the track error signal of the “difference push-pull method” is not changed as described in Japanese Journal of Applied Physics, Vol. 38, pp. 1761–1767.

Similar to this, as the diffraction optical devices 8 b , 8 c of the second optical system 2 b, the diffraction optical device formed with the grating pattern shown in FIG. 10 may be used.

As described above, the optical head unit 1 of the first embodiment of the present invention is provided with the first objective lens 3 a , the first optical system 2 a , the second objective lens 3 b , and the second optical system 2 b . When the protective layer of the optical disc 5 has a first thickness corresponding to the next-generation standard, the semiconductor laser (first light source) 7 a of the first optical system 2 a and the first objective lens 3 a are used. When the protective layer of the optical disc 5 has a second thickness corresponding to the DVD standard, the semiconductor laser (second light source) 7 b of the second optical system 2 b and the second objective lens 3 b are used. When the protective layer of the optical disc 5 has a third thickness corresponding to the CD standard, the semiconductor laser (third light source) 7 c of the second optical system 2 b and the second objective lens 3 b are used. Further, the wavelength of the emitted light of the semiconductor laser 7 a corresponds to the next-generation standard. The wavelength of the emitted light of the semiconductor laser 7 b may correspond to the DVD standard, the wavelength of the emitted light of the semiconductor laser 7 c may correspond to the CD standard. Therefore, information can be written or read onto/from any of the optical discs. Information can be written or read, not only onto/from conventional optical recording media of the DVD standard and the CD standard, but also onto/from an optical recording medium of the next-generation standard using a blue light.

FIG. 11 shows the schematic construction of an optical information writing/reading device of a second embodiment of the present invention.

The optical information writing/reading device is constructed by adding a first writing/reading circuit 22 a , a second writing/reading circuit 22 b , a third writing/reading circuit 22 c , a switching circuit 21 , and a control circuit 20 , to the optical head unit 1 of the above-described first embodiment.

The first writing/reading circuit 22 a generates an input signal to the semiconductor laser 7 a provided in the first optical system 2 a based on a write signal to the optical disc 5 of the next-generation standard. It generates a read signal from the optical disc 5 based on an output signal from the photodetector 15 a provided in the first optical system 2 a.

The second writing/reading circuit 22 b generates an input signal to the semiconductor laser 7 b provided in the second optical system 2 b based on a write signal to the optical disc 5 of the DVD standard. It generates a read signal from the optical disc 5 based on an output signal from the photodetector 15 b provided in the second optical system 2 b.

The third writing/reading circuit 22 c generates an input signal to the semiconductor laser 7 c provided in the second optical system 2 b based on a write signal to the optical disc 5 of the CD standard. It generates a read signal from the optical disc 5 based on an output signal from the photodetector 15 b provided in the second optical system 2 b.

›DETAILED DESCRIPTION OF THE INVENTION · 5 of 5

The switching circuit 21 switches a transmission path of the input signal from the first writing/reading circuit 22 a to the semiconductor laser 7 a of the first optical system 2 a , a transmission path of the input signal from the second writing/reading circuit 22 b to the semiconductor laser 7 b of the second optical system 2 b , and a transmission path of the input signal from the third writing/reading circuit 22 c to the semiconductor laser 7 c of the second optical system 2 b . In addition, it switches a transmission path of the output signal from the photodetector 15 a of the first optical system 2 a to the first writing/reading circuit 22 a , a transmission path of the output signal from the photodetector 15 b of the second optical system 2 b to the second writing/reading circuit 22 b , and a transmission path of the output signal from the photodetector 15 b of the second optical system 2 b to the third writing/reading circuit 22 c.

The control circuit 20 controls the operation of the switching circuit 21 as follows. When the optical disc 5 of the next-generation standard is inserted into the optical information writing/reading device, it is detected to transmit an input signal from the first writing/reading circuit 22 a to the semiconductor laser 7 a and an output signal from the photodetector 15 a to the first writing/reading circuit 22 a . When the optical disc 5 of the DVD standard is inserted thereinto, an input signal is transmitted from the second writing/reading circuit 22 b to the semiconductor laser 7 b and an output signal is transmitted from the photodetector 15 b to the second writing/reading circuit 22 b . When the optical disc 5 of the CD standard is inserted thereinto, an input signal is transmitted from the third writing/reading circuit 22 c to the semiconductor laser 7 c and an output signal is transmitted from the photodetector 15 b to the third writing/reading circuit 22 c.

As described above, the optical information writing/reading device of the second embodiment of the present invention includes the above-described optical head unit 1 of the first embodiment of the present invention and switches and uses the optical systems and the writing/reading circuits depended upon the kind of the optical disc 5 inserted. Therefore, information can be written or read onto/from the optical disc 5 corresponding to any kinds of optical discs.

The previous description of embodiments is provided to enable a person skilled in the art to make and use the present invention. Moreover, various modifications to these embodiments will be readily apparent to those skilled in the art, and the generic principles and specific examples defined herein may be applied to other embodiments without the use of inventive faculty. Therefore, the present invention is not intended to be limited to the embodiments described herein but is to be accorded the widest scope as defined by the limitations of the claims and equivalents.

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16 claims

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Classifications

16 codes
IPC · International Patent Classification
Section G — Physics
  • G11B7/131
  • G11B7/1374
  • G11B7/133
  • G11B7/1378
  • G11B7/1353
  • G11B7/1376
  • G11B7/1365
  • G11B7/1275
  • G11B7/1356
  • G11B7/135
  • G11B7/125
  • G11B7/09
  • G11B7/00
  • G11B7/13
USPC · US Patent Classification
369/44.37369/112.24

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⤢ drag to zoomJan 2004Jul 2004Jan 2005Jul 2005Jan 2006Jul 2006Jan 2007Jul 2007USPTOApplicantRestriction requirementResponse after non-final
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1,343 days filing → grant
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Gautam R. Patel
art unit 2627 · TC 2600
Citations: 10 back · 1 forward

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