Skew mirrors, methods of use, and methods of manufacture

US10185069B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10185069-B2
Application numberUS-201715849532-A
CountryUS
Kind codeB2
Filing dateDec 20, 2017
Priority dateAug 24, 2015
Publication dateJan 22, 2019
Grant dateJan 22, 2019

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Abstract

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An optical reflective device referred to as a skew mirror, having a reflective axis that need not be constrained to surface normal, is described. Examples of skew mirrors are configured to reflect light about substantially constant reflective axes across a relatively wide range of wavelengths. In some examples, a skew mirror has substantially constant reflective axes across a relatively wide range of angles of incidence. Exemplary methods for making and using skew mirrors are also disclosed. Skew mirrors include a grating structure, which in some examples comprises a hologram.

First claim

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We claim: 1. Apparatus comprising: a grating medium; a grating structure residing in the grating medium, wherein: the grating structure is configured to reflect first incident light, the first incident light being incident upon the grating medium at a specific site and having a first wavelength and a first internal angle of incidence relative to a grating medium surface normal; the first incident light is principally reflected by the grating medium as first reflected light, the first reflected light having the first wavelength and a first internal angle of reflection relative to the surface normal; the first incident light and the first reflected light are bisected by a first reflective axis having a first reflective axis angle relative to the surface normal; the grating structure is further configured to reflect second incident light, the second incident light being incident on the grating medium at the specific site and having a second wavelength and a second internal angle of incidence relative to the surface normal; the second incident light is principally reflected by the grating medium as second reflected light, the second reflected light having the second wavelength and a second internal angle of reflection relative to the surface normal; the second incident light and the second reflected light are bisected by a second reflective axis having a second reflective axis angle relative to the surface normal; the first internal angle of incidence is the same as the second internal angle of incidence; the first reflective axis is non-zero relative to the surface normal; the first wavelength differs from the second wavelength; and the first reflective axis angle differs from the second reflective axis angle. 2. The apparatus of claim 1 , wherein the first reflective axis angle differs from the second reflective axis angle by 0.25 degrees or less. 3. The apparatus of claim 2 , wherein the first incident light is offset from the first reflective axis by at least 1.0 degree. 4. The apparatus of claim 1 , wherein the first wavelength differs from the second wavelength by a wave fraction of at least 0.005. 5. The apparatus of claim 1 , wherein: the grating structure comprises a plurality of volume holograms; each of the volume holograms in the plurality of volume holograms spatially overlaps at least one other volume holograms in the plurality of volume holograms; and the grating medium is at least 70 μm thick. 6. The apparatus of claim 5 , wherein: the plurality of volume holograms includes at least four holograms; and each of the volume holograms in the plurality of volume holograms at least partially spatially overlaps all others of the plurality of volume holograms. 7. The apparatus of claim 6 , wherein adjacent |ΔK G | for the at least four holograms has a mean value that resides between 5.0×10 3 and 1.0×10 7 radians per meter (rad/m). 8. The apparatus of claim 1 , wherein: the grating structure comprises at least 9 volume holograms; each of the at least 9 volume holograms at least partially spatially overlaps at least one other of the at least 9 volume holograms; and the grating medium is at least 200 μm thick. 9. The apparatus of claim 1 , wherein the first reflective axis differs from the surface normal by at least 4.0 degrees. 10. The apparatus of claim 9 , wherein the first reflective axis differs from the surface normal by at least 9.0 degrees. 11. A method of making the apparatus of claim 1 , the method comprising: creating the grating structure by recording multiple volume holograms in the grating medium, wherein: each of the multiple volume holograms is recorded using a first recording beam and a second recording beam, each of the first and second recording beams including a collimated, plane wave beam, and the first recording beam having the same wavelength as the second recording beam; each of the multiple volume holograms is recorded with the first recording beam being incident upon the grating medium at a unique first recording beam internal angle relative to the surface normal and the second recording beam being incident upon the grating medium at a unique second recording beam internal angle relative to the surface normal; each of the multiple volume holograms is recorded with the first recording beam and the second recording beam being symmetrical about a skew axis; each of the multiple volume holograms at least partially spatially overlaps at least one other of the multiple holograms; the skew axes of the multiple volume holograms have substantially constant skew angles relative to the surface normal; and the skew axes of the multiple volume holograms have a mean skew angle that is substantially identical to both the first reflective axis angle and the second reflective axis angle. 12. The method of claim 11 , wherein each of the multiple volume holograms at least partially spatially overlaps all others of the multiple volume holograms. 13. A method of making an apparatus, the method comprising: creating a grating structure in a grating medium by recording multiple volume holograms in the grating medium, wherein: each of the multiple volume holograms is recorded using a first recording beam and a second recording beam, each of the first and second recording beams including a collimated, plane wave beam, and the first recording beam having a same wavelength as the second recording beam; each of the multiple volume holograms is recorded with the first recording beam being incident upon the grating medium at a unique first recording beam internal angle relative to a surface normal of the grating medium and the second recording beam being incident upon the grating medium at a unique second recording beam internal angle relative to the surface normal; each of the multiple volume holograms is recorded with the first recording beam and the second recording beam being symmetrical about a skew axis, the skew axis having a skew axis angle relative to the surface normal; each of the multiple volume holograms at least partially spatially overlaps at least one other of the multiple holograms; and the skew axes of the multiple volume holograms are substantially constant and have a non-zero mean skew axis angle relative to the surface normal. 14. The method of claim 13 , wherein each of the multiple volume holograms at least partially spatially overlaps all others of the multiple volume holograms. 15. The method of claim 14 , wherein: the multiple volume holograms includes at least 9 holograms; and all of the unique first recording beam internal angles collectively span a range of at least 6.4 degrees. 16. The method of claim 15 , wherein: adjacent |ΔK G | for the at least 9 holograms has a mean value that resides between 5.0×10 3 and 1.0×10 7 rad/m. 17. The method of claim 15 , wherein: adjacent |ΔK G | for the at least 9 holograms has a mean value that resides between 1.0×10 4 and 1.0×10 6 rad/m. 18. The method of claim 13 , wherein: the grating structure is configured to reflect first incident light, the first incident light being incident upon the grating medium at a specific site and having a first wavelength and a first internal angle of incidence relative to grating medium surface normal; the first incident light is principally reflected by the grating medium as first reflected light, the first reflected light having the first wavelength and a first internal angle of reflection relative to the surface normal; the first incident light and the first reflected light are bisected by a f

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What does patent US10185069B2 cover?
An optical reflective device referred to as a skew mirror, having a reflective axis that need not be constrained to surface normal, is described. Examples of skew mirrors are configured to reflect light about substantially constant reflective axes across a relatively wide range of wavelengths. In some examples, a skew mirror has substantially constant reflective axes across a relatively wide ra…
Who is the assignee on this patent?
Akonia Holographics Llc, Akonia Holographics Llc
What technology area does this patent fall under?
Primary CPC classification G02B5/32. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Jan 22 2019 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 2 related publications on this page (citations in our corpus or others sharing the same primary CPC).