Optical pickup device-use optical element, coupling lens and optical pickup device
A technology of optical pickup and relay lens, which is applied in the direction of light beam guiding device, optical recording/reproduction, optical recording head, etc., which can solve the problems of not considering the diffraction efficiency and the inability to ensure the luminous flux of the light spot, etc.
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Embodiment 1
[0286] Table 1 shows lens data of an optical element (objective lens) as an example suitable for the above-mentioned embodiment. As can be seen from Table 1, in the objective lens, a diffraction structure is provided in a region (referred to as a common region) where light beams from the first semiconductor laser, the second semiconductor laser, and the third semiconductor laser pass. In addition, if a change occurs in which the wavelength of the light source becomes longer, the diffractive structure has an optical characteristic that makes spherical aberration more insufficient in the light beam passing through the diffractive structure. This embodiment corresponds to the optical elements described in items 6 and 7. Here, hereafter (including the lens data of the table), it is stipulated that E (for example, 2.5×E-3) represents a power multiplier of 10 (for example, 2.5×10 -3 ).
[0287]
[0288] The specifications of this embodiment are as follows:
[0289] (1) Light s...
Embodiment 2
[0299] Table 2 shows lens data of an optical element (objective lens) as an example suitable for the above-mentioned embodiment. As can be seen from Table 2, in the objective lens, a diffraction structure is provided in a region (referred to as a common region) where light beams from the first semiconductor laser, the second semiconductor laser, and the third semiconductor laser pass. In addition, if a change occurs in which the wavelength of the light source becomes longer, the diffractive structure has an optical characteristic that makes spherical aberration more insufficient in the light beam passing through the diffractive structure. This embodiment corresponds to the optical element described in Item 11.
[0300]
[0301] Aspheric coefficient
[0302]
[0303] The specifications of this embodiment are as follows:
[0304] (1) Light source wavelength λ1 of the first semiconductor laser: 407nm
[0305] (2) The number n1(n1A) of the maximum diffraction efficiency w...
Embodiment 3
[0314] Table 3 shows lens data of an optical element (objective lens) as an example suitable for the above-mentioned embodiment. As can be seen from Table 3, in the objective lens, a diffraction structure is provided in a region (referred to as a common region) where light beams from the first semiconductor laser, the second semiconductor laser, and the third semiconductor laser pass. In addition, if a change occurs in which the wavelength of the light source becomes longer, the diffractive structure has an optical characteristic that makes spherical aberration more insufficient in the light beam passing through the diffractive structure. This embodiment corresponds to the optical element described in Item 11.
[0315]
[0316] The specifications of this embodiment are as follows:
[0317] (1) Light source wavelength λ1 of the first semiconductor laser: 407nm
[0318] (2) The number n1(n1A) of the maximum diffraction efficiency when the light beam from the first semicondu...
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