Methods and apparatuses for reducing stray light emission from an eyepiece of an optical imaging system
US-12025802-B2 · Jul 2, 2024 · US
US2016334635A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2016334635-A1 |
| Application number | US-201615149245-A |
| Country | US |
| Kind code | A1 |
| Filing date | May 9, 2016 |
| Priority date | May 15, 2015 |
| Publication date | Nov 17, 2016 |
| Grant date | — |
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A diffractive optical element ( 1 ) includes a first diffraction grating ( 21 ) including a first grating surface ( 21 a ) and a first grating wall surface ( 21 b ), a second diffraction grating ( 31 ) including a second grating surface ( 31 a ) and a second grating wall surface ( 31 b ), and a thin film ( 11 ) provided between the first grating wall surface and the second grating wall surface and being in contact with both of the first and second grating wall surfaces, an extinction coefficient of the thin film with respect to a wavelength λ in a use wavelength band is not greater than 0.0005, and with respect to the wavelength λ, refractive indices of materials of the thin film, the first diffraction grating, and the second diffraction grating, a relative diffractive index difference of the thin film and the first diffraction grating, and a width of the thin film satisfy predetermined conditions.
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What is claimed is: 1 . A diffractive optical element comprising: a first diffraction grating including a first grating surface and a first grating wall surface; a second diffraction grating including a second grating surface and a second grating wall surface; and a thin film provided between the first grating wall surface and the second grating wall surface, the thin film being in contact with both of the first grating wall surface and the second grating wall surface, wherein an extinction coefficient of the thin film with respect to a wavelength λ in a use wavelength band is not greater than 0.0005, and wherein expressions below are satisfied: n 1 >n 2 >n 3 , 0.005<Δ<0.045, and 0.5 ≦W/W C ≦2.0, where n 1 , n 2 , and n 3 are refractive indices of materials of the thin film, the first diffraction grating, and the second diffraction grating, respectively, with respect to the wavelength λ, Δ is a relative diffractive index difference of the thin film and the first diffraction grating, and W is a width of the thin film between the first grating wall surface and the second grating wall surface, and where Δ and W C are defined as follows: Δ = n 1 2 - n 2 2 2 n 1 2 W C = W C , TE + W C , TM 2 W C , TE = 1 κ C tan - 1 ( δ C κ C ) W C , TM = 1 κ C tan - 1 ( n 1 2 δ C n 3 2 κ C ) κ C = k 0 n 1 2 - n 2 2 δ C = k 0 n 2 2 - n 3 2 k 0 = 2 π / λ . 2 . The diffractive optical element according to claim 1 , wherein an expression below is satisfied: 0≦( n eq −n 2 )× d/λ< 0.3, where d is a grating height of each of the first diffraction grating and the second diffraction grating, and n eq is an equivalent refractive index of propagation light that is propagated inside the thin film, wherein the equivalent refractive index n eq is defined as follows: n eq = n eq , TE + n eq , TM 2 n eq , TE = β TE / k 0
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