Laminated wave plate and optical pickup using the same
View Patent ↗A conventional broadband quarter-wave plate has not completely solved the wavelength dependence and has different efficiencies of shifting the phase by 90 ° depending on the wavelengths, and therefore has a problem that it cannot fulfill the strict specifications on the optical characteristics which are demanded of a wave plate from a viewpoint of the optical efficiency and the like in an optical pickup device compatible with a plurality of different wavelengths. To provide a wave plate which completely functions as a quarter-wave plate with respect to a plurality of different wavelengths and an optical pickup using that wave plate to solve the problem, the present invention provides a laminated wave plate, wherein a wave plate with a phase difference α and a wave plate with a phase difference β with respect to monochromatic light with a wavelength λ are laminated in such a way that directions of optical axes of said plates intersect each other, so that the laminated wave plate, as a whole, functions as a quarter-wave plate, and which is characterized in that a relationship between the α and the β satisfies the following formulas: (3/2)×π≠α−2×π×( m −1) π≠β−2×π×( n −1), wherein: each of m and n is a positive integer.
1. A laminated wave plate, comprising a first wave plate with a phase difference α and a second wave plate with a phase difference β both with respect to monochromatic light having a wavelength λ, said wave plates being laminated together in such a way that directions of optical axes of said wave plates intersect each other, so that the laminated wave plate, as a whole, functions as a quarter-wave plate with respect to lights having two or more different wavelengths, wherein:
said first wave plate satisfies the following formula:
(3/2)×π≠α−2 ×π×m
said second wave plate satisfies the following formula:
π≠β−2 ×π×n
a relationship between said α and β satisfies the following formula:
β−2 ×π×n <α−2 ×π×m;
said α and β respectively satisfy the following formulas:
α>2 ×π×m , and
β>2 ×π×n
wherein each of m and n is a positive integer; and
said optical axes of said first and second wave plates cross each other at an angle not equal to 90°.
2. An optical pickup device constructed in such a way that a first linearly polarized light with a first wavelength and a second linearly polarized light with a second wavelength, output from a light source, pass a wave plate, wherein
said wave plate is a laminated wave plate in which a first wave plate with a phase difference α and a second wave plate with a phase difference β with respect to monochromatic light having a wavelength λ are laminated in such a way that directions of optical axes of said wave plates intersect each other, so that the laminated wave plate, as a whole, functions as a quarter-wave plate with respect to lights having two or more different wavelengths. and wherein:
said first wave plate satisfies the following formula:
(3/2)×π≠α−2 ×π×m
said second wave plate satisfies the following formula:
π≠β−2 ×π×n
a relationship between said α and β satisfies the following formula:
β−2 ×π×n<α− 2 ×π×m;
said α and β respectively satisfy the following formulas:
α>2 ×πm , and
β>2 ×π×n
wherein each of m and n is a positive integer; and
said optical axes of said first and second wave plates cross each other at an angle not equal to 90°.
3. The optical pickup device according to claim 2 , wherein said two different wavelengths comprise 650 nm and 785 nm.
4. The laminated wave plate according to claim 1 , wherein
said wavelength λ is 785 nm;
the phase difference α of said first wave plate is 1695°; and
the phase difference β of said second wave plate is 850°.
5. The laminated wave plate according to claim 4 , wherein said laminated wave plate functions as a quarter-wave plate with respect to wavelengths of 655 nm and 785 nm.