Optical pickup
A technology of lasers and optical discs, applied in the direction of instruments, optics, diffraction gratings, etc., can solve problems such as insufficient luminous efficiency and reduced light quantity of servo signals, and achieve the effect of small light loss and reduced number of components
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Embodiment approach 1
[0048] Next, the optical pickup of Embodiment 1 will be described with reference to FIGS. 1 to 7 .
[0049] As shown in FIG. 1 , light emitted from a semiconductor laser 1 is converted by a collimator lens 2 into a parallel beam having an effective beam diameter φeff (2 mm in this embodiment). Then, after passing through the diffraction grating 3 and the light splitting element 4, the spherical aberration compensating element 5 composed of two lenses magnifies the effective beam diameter by m times. In the present embodiment, since m=1.5, the effective beam diameter of the light passing through the spherical aberration compensating element 5 becomes φeff·m=3 millimeters (mm). Furthermore, after the reflection mirror 6 changes the optical path, it is guided to the objective lens 7 of the 2-piece group, and converged on the optical disk 8 .
[0050] After passing through the objective lens 7, the reflected light from the optical disc 8 travels on the optical path opposite to th...
Embodiment approach 2
[0070] Next, refer to FIG. 8 to FIG. 11 of Embodiment 2 of the gate surface.
[0071] As shown in FIG. 8, the light emitted from the semiconductor laser 1 passes through the diffraction grating 3 and the beam splitter 4, and is collimated by the collimator lens 2 into an effective beam diameter φeff (2 mm in this embodiment). Then, the spherical aberration compensating element 5 composed of two lenses enlarges the effective beam diameter by m times. In the present embodiment, since m=1.5, the effective beam diameter of the light passing through the spherical aberration compensating element 5 becomes φeff·m=3 millimeters (mm). Furthermore, after the reflection mirror 6 changes the optical path, it guides to the objective lens 7 of the 2-piece set, and makes it converge on the optical disc 8 .
[0072] The reflected light from the optical disk 8 passes through the objective lens 7 , travels on the optical path opposite to the incident light, is collected by the collimator lens 2 ...
Embodiment approach 3
[0085] An optical pickup according to Embodiment 3 will be described with reference to FIGS. 12A to 14 .
[0086] In this embodiment, as shown in FIG. 12A , the diffraction grating 3 is arranged in the converging optical path as in Embodiment 2. Therefore, for example, if L=8.1 mm and x=4.5 mm, it is the same as Embodiment 2 and also forms φgr = 1.1 mm. Assuming that the horizontal component θ / / =9 degrees of the FFP half-value total width of the light emitted by the semiconductor laser 1, and the vertical component θ⊥=18 degrees, then the irradiation area becomes an ellipse with a minor axis of 0.7 millimeters and a major axis of 1.43 millimeters in the Y direction. shape. Furthermore, the effective diameter (φgr) of the diffraction grating becomes the shape of the center portion of the laser irradiation area. In this embodiment, the semiconductor laser 1 of Embodiments 1 and 2 is rotated by 90 degrees around the optical axis. By rotating in this way, the polarization axis ...
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