An exemplary embodiment for performing the present invention will be described in detail with reference to the attached drawings.
In
The structure shown in
In
A photodetector (LPC-PD) 6 for receiving a light beam reflected by the non-polarizing beam splitter (NBS) 4 to control the emission power of the semiconductor laser 1 is provided. A light beam passing through the ¼ wavelength plate (QWP) 8 is incident on an expander lens 9. The expander lens 9 is used to correct spherical aberration caused in an objective lens 11 or an SIL 12, and constructed such that a distance between two lenses of the beam expander can be controlled according to the spherical aberration.
The light beam from the expander lens 9 is incident on the objective lens 11 of an optical head portion 10. The optical head portion 10 includes the objective lens 11 and the SIL 12. As described above, the optical head portion 10 is mounted on a biaxial actuator (not shown) for integrally driving the two lenses in a focus direction and a tracking direction. The tracking control circuit 23 controls the biaxial actuator in the tracking direction to perform tracking control. A gap servo circuit (not shown) controls the biaxial actuator in an optical axis direction to perform gap servo control.
In this embodiment, the object lens 11 of NA=0.7 and the SIL 12 which is a hemispherical lens of NA=2 are combined with each other to set NAeff to 1.4.
Here, only when a distance between a bottom surface of the SIL 12 and the optical disk 13 is equal to or shorter than a fraction of 405 nm which is a light source wavelength, for example, when the distance is a short distance of 100 nm or less, a light beam from the bottom surface of the SIL 12 acts on a recording surface as evanescent light. Therefore, it is possible to realize recording or reproduction with a light spot diameter of NAeff. In order to maintain this distance, the gap servo control is employed.
The light beam reflected on the optical disk 13 becomes reversed circularly polarized light and is incident on the SIL 12 and the objective lens 11 to be converted into a parallel light beam again. Then, the light beam passes through the expander lens 9 and the ¼ wavelength plate (QWP) 8 to be converted into linearly polarized light in a direction orthogonal to the direction of the polarized light which goes to the optical disk 13, and a resultant light beam is reflected by the polarizing beam splitter (PBS) 7. The reflected light beam is incident on a ½ wavelength plate (HWP) 14 and a polarizing plane thereof is rotated by 45°.
An S-polarized light component of the light beam whose polarizing plane is rotated 45° by the ½ wavelength plate (HWP) 14 is reflected by a polarizing beam splitter (PBS) 15 and focused on a photodetector (PD1) 17 through a lens 16. Therefore, an RF output 18 including information on the optical disk 13 is generated.
On the other hand, a P-polarized light component of the light beam whose polarizing plane is rotated by 45° through the ½ wavelength plate (HWP) 14 passes through the polarizing beam splitter (PBS) 15 and is reflected on a mirror 19. The reflected light beam is focused on a two-divided photodetector (PD2) 21 through a lens 20. A tracking error 22 is obtained from an output of the two-divided photodetector (PD2) 21. The tracking error 22 is generated by, for example, a push-pull method.
A light beam of NAeff<1 which does not cause total reflection, of the light beam reflected on the bottom surface of the SIL 12, is reflected as circularly polarized light reversed from that at the time of incidence similarly as in the case of the reflected light on the optical disk 13. In the case of a light beam of NAeff≧1 which causes total reflection, a phase difference δ expressed by Expression (1) is generated between a P-polarized light component and an S-polarized light component. Therefore, the light beam is shifted from the circularly polarized light to become elliptically polarized light. After passing through the ¼ wavelength plate (QWP) 8, the light beam includes a polarized light component in the same direction as that of the polarized light which goes to the optical disk 13.
The polarized light component passes through the polarizing beam splitter (PBS) 7 and is reflected by the non-polarizing beam splitter (NBS) 4. Then, the reflected light is detected by a photodetector (PD3) 25 through a lens 24. A gap error signal 26 is obtained from on an output of the photodetector (PD3) 25.
Here, in the present invention, as illustrated in
When a target threshold value is set in advance, the gap servo circuit (not shown) controls the biaxial actuator (not shown) based on the gap error signal 26 to perform the gap servo control. Therefore, a distance between the bottom surface of the SIL 12 and the optical disk 13 can be maintained at a desirable distance of 100 nm or less by the gap servo control. The gap error signal 26 can be normalized using an output of the photodetector (LPC-PD) 6 for controlling the emission power of the semiconductor laser 1.
When the optical head portion 10 is moved in a radius direction by, for example, a radial runout of the optical disk 13, a light spot moves on the two-divided photodetector (PD2) 21, so that an offset is generated in the tracking error signal 22.
A light spot moves even on the two-part photodetector (PD3) 25. Therefore, as illustrated in
(A−B)/(A+B)=LenP.error Expression (2)
In the tracking control circuit 23, calculation is performed for correcting the offset of the tracking error 22 by the optical head portion position signal 27, using a k-factor (coefficient). That is, calculation is performed for removing the offset from the tracking error, using the following expression. The coefficient k is adjusted so as to remove the offset from the tracking error signal.
Tracking Error TE=PushPull-k·LenP.error Expression (3)
In Expression (3), “PushPull” corresponds to the tracking error signal 22 and is obtained from an output of the two-divided photodetector (PD2) 21 by a conventionally known push-pull method. In addition, “k·LenP.error” corresponds to the position signal 27 of the optical head portion. The offset is removed from the tracking error signal by subtracting “k·LenP.error” from “PushPull”.
The tracking control circuit 23 performs the tracking control using the corrected tracking error signal. In this case, as described above, the optical head portion 10 including the objective lens 11 and the SIL 12 is mounted on the biaxial actuator (not shown), so that the tracking control circuit 23 controls the biaxial actuator based on the corrected tracking error signal to perform the tracking control.
Therefore, when the tracking control is to be performed, the tracking error signal with no offset is used, so that the accurate tracking control can be performed without depending on, for example, the radial runout of the optical disk. Similarly as in the conventional case, the gap servo circuit (not shown) controls the biaxial actuator (not shown) based on the gap error signal 26. Thus, the gap servo control is performed so as to make the interval between the SIL 12 and the optical disk 13 constant.
It is desirable to defocus the light beam incident on the two-divided photodetector (PD3) 25. Therefore, the position detection sensitivity for the optical head portion can be improved.
The optical head portion position signal 27 can be used for track jump. That is, by controlling the actuator using on the position signal, access to a desirable track is possible without always locating the actuator at a long distance from a neutral position in the case of track jump, so that it is unlikely to deteriorate the optical performance at the time of recording and reproduction.
According to the present invention, correction of the tracking error signal including the offset enables the light spot to be positioned at an accurate position relative to a track, even when the center of the SIL and the center of the objective lens are deviated from the center of the optical axis.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2006-156066, filed Jun. 5, 2006, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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2006-156066 | Jun 2006 | JP | national |