Dynamic information storage or retrieval – Specific detail of information handling portion of system – Radiation beam modification of or by storage medium
Reexamination Certificate
2000-11-15
2004-09-28
Patel, Gautam R. (Department: 2655)
Dynamic information storage or retrieval
Specific detail of information handling portion of system
Radiation beam modification of or by storage medium
C369S124120, C369S124030, C369S053190, C369S112240
Reexamination Certificate
active
06798731
ABSTRACT:
CROSS-REFERENCE TO RELATED APPLICATIONS
This application claims the benefit of Korean Application No. 00-519 filed Jan. 6, 2000, in the Korean Patent Office, the disclosure of which is incorporated herein by reference.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to an optical pickup apparatus for recording/reproducing information on/from a high density optical disk so that coma and spherical aberration due to changes in the thickness of the optical disk can be corrected, and more particularly, to an optical pickup apparatus in which a main light spot and an auxiliary light spot having spherical aberration are allowed to be formed on an optical disk and aberration can be corrected based on the main light spot and the auxiliary light spot received by a photodetector.
2. Description of the Related Art
In general, an optical pickup apparatus records or reproduces information recorded on or from an optical disk. With high densification of optical disks, light emitted from a light source is required to have a shorter wavelength while the numerical aperture (NA) of the light increases. Thus, when the optical pickup apparatus records/reproduces information on/from the optical disk, if the optical disk is inclined, that is, if the surface of the optical disk on which information is recorded is inclined with respect to the optical axis, a coma aberration is generated due to the inclination. Also, spherical aberration is generated due to the shorter wavelength of the light source due to the high densification of the optical disk, a high NA, and a change in the thickness of the optical disk and the wavelength accompanied by the accommodation of the compatibility with a low density optical disk.
Here, since coma aberration W
31
satisfies Equation 1, a coma aberration due to the inclination of the optical disk increases in an optical pickup with a high NA compared with coma aberration in an optical pickup with a relatively low NA with respect to the same inclination of the optical disk.
W
31
∝NA
3
[Equation 1]
Also, the recording capacity of the optical disk is determined by the wavelength &lgr; of the light emitted from the light source and the NA of an objective lens, as shown in Equation 2.
Diameter of focused spot ∝&lgr;/
NA
[Equation 2]
Also, spherical aberration W
40d
generated due to a deviation &Dgr;d in the thickness of the optical disk is defined by Equation 3.
W
40
d
=
n
2
-
1
8
n
3
(
NA
)
4
Δ
d
λ
[
Equation
3
]
Here, n denotes the refractive index of the substrate of the optical disk and d denotes the thickness of the substrate.
Thus, according to Equation 2, when it is desirable to set the recording density of the optical disk to 15 gigabytes or greater, a light source emitting light having a short wavelength of about 410 nm and an objective lens having an NA of 0.6 or greater are required to be adopted. However, when the NA of the objective lens is increased in order to increase the recording density of the optical disk, the spherical aberration W
40d
generated due to the deviation &Dgr;d in the thickness of the optical disk drastically increases because the spherical aberration is proportional to NA to the fourth power, (NA)
4
.
Referring to
FIG. 1
, a conventional optical disk aberration correcting apparatus to correct coma and spherical aberration includes an objective lens
3
for primarily focusing incident light and a focusing lens
5
for secondarily focusing the light focused by the objective lens
3
to form a spot on an optical disk
1
.
When the optical disk
1
is inclined in one direction, coma aberration is corrected by driving the focusing lens
5
in the inclined direction. Also, when the spherical aberration due to the thickness deviation &Dgr;d of the optical disk
1
is to be corrected, as shown in
FIG. 2
, the spherical aberration is corrected by adjusting an interval between the focusing lens
5
and the objective lens
3
.
In the conventional optical disk aberration correcting apparatus having the above structure, since it is necessary to drive the objective lens and the focusing lens in a direction to control the tracking and focusing of a light spot, drive the focusing lens to be inclined, and drive the objective lens and the focusing lens to adjust the interval therebetween, the structure of the actuator is complicated.
SUMMARY OF THE INVENTION
To solve the above problems, it is an object of the present invention to provide an optical pickup apparatus which can correct spherical aberration due to a change in the thickness of the optical disk and a change in the wavelength and coma aberration due to inclination of the optical disk, by forming at least two light spots on the optical disk.
Additional objects and advantages of the invention will be set forth in part in the description which follows, and, in part, will be obvious from the description, or may be learned by practice of the invention.
Accordingly, to achieve the above and other objects, there is provided an optical pickup apparatus comprising a light source for emitting light, an optical path changer which changes a proceeding path of incident light, an objective lens which focuses incident light to form a light spot on an optical disk, and a light splitter, provided on the optical path between the light source and the optical path changer, which splits incident light into at least two light beams including first and second light beams so that at least two light spots including a main light spot having no aberration and an auxiliary light spot having a predetermined spherical aberration are formed on the optical disk. A photodetector including first and second light receiving portions respectively receives the first and second light beams reflected by the optical disk and passing through the optical path changer. A signal processing portion, including a delay which delays the phase of a second signal in order to synchronize a first signal and the second signal which are detected and optoelectrically converted by the first and second light receiving portions, compensating for the deviation in the thickness of the optical disk from the first and second signals which are synchronized with each other.
Advantageous features of the present invention is that, in order to correct for aberrations, it is not necessary to either drive the objective lens, the focusing lens in a direction to control the tracking and focusing of a light spot, to drive the focusing lens to be inclined, or to drive the objective lens and the focusing lens to adjust the interval therebetween.
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Kenji Yamamoto et al., “0.8-Numerial-Aperture Two-Element Objective Lens for the Optical Disk”, Jpn. J. Appl. Phys. vol. 36 (1997), pp. 456-459, Part 1, No. 1B, Jan. 1997.
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Ahn Young-man
Chung Chong-sam
Kim Tae-kyung
Suh Hea-jung
Patel Gautam R.
Samsung Electronics Co,. Ltd.
Staas & Halsey , LLP
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