Optical device, projector, manufacturing method, and manufacturing support apparatus
View Patent ↗A light source unit ( 110 ) emits linearly polarized laser light of a given wavelength. A wave plate ( 121 ) transmits the laser light emitted from the light source unit ( 110 ) and has a phase delay axis of which the direction is adjusted to about 0 degrees with respect to the polarization direction ( 101 ) of the laser light. A liquid crystal cell ( 123 ) transmits laser light that has passed through the wave plate ( 121 ) and by a switchable rotation amount, rotates the polarization direction ( 101 ) of the laser light transmitted through the liquid crystal cell ( 123 ). A wave plate ( 125 ) transmits laser light that has passed through the liquid crystal cell ( 123 ); and further has a phase delay axis of which the direction is adjusted to about 0 degrees with respect to the polarization direction ( 101 ) of the laser light.
1. An optical device comprising:
a liquid crystal cell that transmits laser light that is in a state of polarization of a given direction and of a given wavelength, the liquid crystal cell being capable of shifting a direction of a director with respect to the given direction by rotating the direction of the director parallel to a substrate surface;
a wave plate that transmits laser light emitted from the liquid crystal cell, the wave plate having a phase delay axis set in an arbitrary direction; and
a control circuit that cyclically shifts the direction of the director, wherein
the optical device outputs the laser light that has passed through the wave plate and the liquid crystal cell,
the laser light includes a plurality of beams of laser light differing in wavelength, and
a thickness of the wave plate is adjusted to a thickness that causes a laminated wave plate composed of the wave plate and the liquid crystal cell to operate, in a vicinity of each of the differing wavelengths, as a quarter wave plate.
2. The optical device according to claim 1 , wherein
the laser light includes a beam of light having a wavelength λ1 and a beam of light having a wavelength λ2 different from the wavelength λ1,
the wave plate has a thickness d1 and a refractive index Δn1 (λ) that changes depending on a wavelength λ of light passing through the wave plate,
the liquid crystal cell has a thickness d2 and a refractive index Δn2 (λ) that changes depending on a wavelength λ of light passing through the liquid crystal cell, and
the thickness d1 of the wave plate is adjusted when an angle between a phase delay axis of the wave plate and a phase delay axis of the liquid crystal cell is Ψ so that an equation below yields ±π/2×(2n−1) (n denotes a natural number) when λ=λ1 and when λ=λ2
arccos [cos 2 Ψ cos {2π·Δ n 1(λ)· d 1/λ+π·Δ n 2(λ)· d 2/λ}+sin 2 Ψ cos {2π·Δ n 1(λ)· d 1/λ−π·Δ n 2(λ)· d 2/λ}]×2.
3. The optical device according to claim 2 , wherein
the refractive index Δn1 (λ) is approximated by A1+A2/λ 2 +A3/λ 4 +A4/λ 6 . . . +Am/λ^(2(m−1)) (A1, A2, A3, . . . Am denote coefficients specific to a material of the wave plate and m denotes a natural number) and the refractive index Δn2 (λ) is approximated by B1+B2/λ 2 +B3/λ 4 +B4/λ 6 . . . +Bm/λ^(2(m−1)) (B1, B2, B3, . . . Bm denote coefficients specific to a material of the liquid crystal cell).
4. The optical device according claim 1 , wherein
a second wave plate identical in configuration to the wave plate is disposed upstream to a side of the liquid crystal cell where laser light is incident.
5. The optical device according claim 1 , wherein
any one among the wave plate and the second wave plate is a liquid crystal element to which voltage can be applied.
6. The optical device according claim 1 , comprising a mirror that reflects back to the liquid crystal cell, the laser light that has passed through the liquid crystal cell, wherein
the wave plate transmits the laser light before the laser light is incident to the liquid crystal cell and transmits the laser light that has been reflected by the mirror and that has again passed through the liquid crystal cell.
7. The optical device according claim 1 , wherein
the direction of the director can be shifted to 67.5 degrees and to 112.5 degrees with respect to the given direction.
8. The optical device according claim 1 , wherein
the direction of the director can be shifted to 0 degrees and to 45 degrees with respect to the given direction.
9. The optical device according claim 1 , further comprising a light source unit that emits the laser light in the state of polarization of the given direction and having a given wavelength, wherein
the light source unit includes:
light sources that emit respective beams of red laser light, green laser light, and blue laser light; and
a light-combining unit that combines the beams of laser light emitted respectively from the light sources.
10. An optical device comprising:
a liquid crystal cell that transmits laser light that is in a state of polarization of a given direction and of a given wavelength, the liquid crystal cell being capable of shifting a direction of a director with respect to the given direction by rotating the direction of the director parallel to a substrate surface;
a wave plate that transmits laser light emitted from the liquid crystal cell, the wave plate having a phase delay axis set in an arbitrary direction; and
a control circuit that cyclically shifts the direction of the director, wherein
the optical device outputs the laser light that has passed through the wave plate and the liquid crystal cell,
the laser light includes a plurality of beams of laser light differing in wavelength, and
a thickness of the liquid crystal cell is adjusted to a thickness that causes a laminated wave plate composed of the wave plate and the liquid crystal cell to operate, in a vicinity of each of the differing wavelengths, as a half wave plate.
11. The optical device according to claim 10 , wherein
the laser light includes a beam of light having a wavelength λ1 and a beam of light having a wavelength λ2 different from the wavelength λ1,
the wave plate has a thickness d1 and a refractive index Δn1 (λ) that changes depending on a wavelength λ of light passing through the wave plate,
the liquid crystal cell has a thickness d2 and a refractive index Δn2 (λ) that changes depending on a wavelength λ of light passing through the liquid crystal cell, and
the thickness d2 of the liquid crystal cell is adjusted when an angle between a phase delay axis of the wave plate and a phase delay axis of the liquid crystal cell is Ψ so that an equation below yields ±π×(2n−1) (n denotes a natural number) when λ=λ1 and when λ=λ2
arccos [cos 2 Ψ cos {2π·Δ n 1(λ)· d 1/λ+π·Δ n 2(λ)· d 2/λ}+sin 2 Ψ cos {2 n·Δn 1(λ)· d 1/λ−π·Δ n 2(λ)· d 2/λ}]×2.
12. The optical device according to claim 11 , wherein
the refractive index Δn1(λ) is approximated by A1+A2/λ 2 +A3/λ 4 +A4/λ 6 . . . +Am/λ^(2(m−1)) (A1, A2, A3, . . . Am denote coefficients specific to a material of the wave plate and m denotes a natural number) and the refractive index Δn2 (λ) is approximated by B1+B2/λ 2 +B3/λ 4 +B4/λ 6 . . . +Bm/λ^(2(m−1)) (B1, B2, B3, . . . Bm denote coefficients specific to a material of the liquid crystal cell).
13. The optical device according claim 10 , wherein
a second wave plate identical in configuration to the wave plate is disposed upstream to a side of the liquid crystal cell where laser light is incident.
14. The optical device according claim 10 , wherein
any one among the wave plate and the second wave plate is a liquid crystal element to which voltage can be applied.
15. The optical device according claim 10 , comprising a mirror that reflects back to the liquid crystal cell, the laser light that has passed through the liquid crystal cell, wherein
the wave plate transmits the laser light before the laser light is incident to the liquid crystal cell and transmits the laser light that has been reflected by the mirror and that has again passed through the liquid crystal cell.
16. The optical device according claim 10 , wherein
the direction of the director can be shifted to 67.5 degrees and to 112.5 degrees with respect to the given direction.
17. The optical device according claim 10 , wherein
the direction of the director can be shifted to 0 degrees and to 45 degrees with respect to the given direction.
18. A manufacturing method of an optical device that includes a liquid crystal cell that transmits a plurality of laser light beams that are in a state of polarization of a given direction and have differing wavelengths, the liquid crystal being capable of shifting a direction of a director with respect to the given direction, the optical device further including a wave plate that has a phase delay axis set in an arbitrary direction and that transmits the laser light that has passed through the liquid crystal cell, the optical device outputting the laser light that has passed through the wave plate and the liquid crystal cell, the manufacturing method comprising:
a first determining step of determining a thickness of the liquid crystal cell;
a second determining step of determining an angle between a phase delay axis of the wave plate and a phase delay axis of the liquid crystal cell; and
a third determining step of determining based on the thickness of the liquid crystal cell determined at the first determining step and on the angle between the phase delay axes determined at the second step, a thickness of the wave plate to be a thickness that causes a laminated wave plate composed of the wave plate and the liquid crystal cell to work as a quarter wave plate for respective wavelengths of emitted beams of light.
19. The manufacturing method according to claim 18 , wherein
the wave plate has a refractive index Δn1(λ) that changes depending on a wavelength λ of light passing through the wave plate,
the liquid crystal cell has a refractive index Δn2 (λ) that changes depending on a wavelength λ of light passing through the liquid crystal cell, and
at the third determining step, a thickness d1 of the wave plate is determined based on a thickness d2 of the liquid crystal cell determined at the first determining step and on an angle Ψ between the phase delay axes determined at the second step, so that an equation below yields ±π/2×(2n−1) (n denotes a natural number) when κ=λ1 and when λ=λ2
arccos [cos 2 Ψ×cos {2π·Δ n 1(λ)· d 1/λ+π·Δ n 2(λ)· d 2/λ}+sin 2 Ψ cos {2π·Δ n 1(λ)· d 1/λ−π·Δ n 2(λ)· d 2/λ}]×2.
20. A manufacturing method of an optical device that includes a liquid crystal cell that transmits a plurality of laser light beams that are in a state of polarization of a given direction and have differing wavelengths, the liquid crystal being capable of shifting a direction of a director with respect to the given direction, the optical device further including a wave plate that has a phase delay axis set in a predetermined direction and that transmits the laser light that has passed through the liquid crystal cell, the optical device outputting the laser light that has passed through the wave plate and the liquid crystal cell, the manufacturing method comprising:
a first determining step of determining a thickness of the wave plate;
a second determining step of determining an angle between a phase delay axis of the wave plate and a phase delay axis of the liquid crystal cell; and
a third determining step of determining based on the thickness of the wave plate determined at the first determining step and on the angle between the phase delay axes determined at the second step, a thickness of the liquid crystal cell to be a thickness that causes a laminated wave plate composed of the wave plate and the liquid crystal cell to work as a half wave plate for respective wavelengths of emitted beams of light.
21. The manufacturing method according to claim 20 , wherein
the wave plate has a refractive index Δn1(λ) that changes depending on a wavelength λ of light passing through the wave plate,
the liquid crystal cell has a refractive index Δn2 (λ) that changes depending on a wavelength λ of light passing through the liquid crystal cell, and
at the third determining step, a thickness d2 of the liquid crystal cell is determined based on a thickness d1 of the wave plate determined at the first determining step and on an angle Ψ between the phase delay axes determined at the second step, so that an equation below yields ±π×(2n−1) (n denotes a natural number) when λ=λ1 and when λ=λ2
arccos [cos 2 Ψ cos {2π—Δ n 1(λ)· d 1/λ+π·Δ n 2(λ)· d 2/λ}+sin 2 Ψ cos {2π·Δ n 1(λ)· d 1/λ−π·Δ n 2(λ)· d 2/λ}]×2.