Off-axis three-mirror optical system with freeform surfaces
US-9846298-B2 · Dec 19, 2017 · US
US11650402B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11650402-B2 |
| Application number | US-202016999222-A |
| Country | US |
| Kind code | B2 |
| Filing date | Aug 21, 2020 |
| Priority date | Jan 15, 2020 |
| Publication date | May 16, 2023 |
| Grant date | May 16, 2023 |
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A freeform surface off-axial three-mirror imaging system is provided. The freeform surface off-axial three-mirror imaging system comprises a primary mirror, a secondary mirror, and a compensating mirror. The primary mirror, the secondary mirror, and the compensating mirror are located adjacent and spaced away from each other. A surface shape of each of the primary mirror and the secondary mirror is a quadric surface. The primary mirror is used as an aperture stop. A surface shape of the compensating mirror is a freeform surface. A light emitted from a light source is reflected by the primary mirror, the secondary mirror, and the compensating mirror to form an image on an image plane.
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What is claimed is: 1. A freeform surface off-axial three-mirror imaging system, comprising: a primary mirror, a secondary mirror, and a compensating mirror, wherein the primary mirror, the secondary mirror and the compensating mirror are located adjacent and spaced away from each other, a surface shape of each of the primary mirror and the secondary mirror is a quadric surface, the primary mirror is an aperture stop, a surface shape of the compensating mirror is a freeform surface, a light emitted from a light source is reflected by the primary mirror, the secondary mirror, the compensating mirror to form an image on an image plane, and an F-number of view of the freeform surface off-axial three-mirror imaging system is 5; a first three-dimensional rectangular coordinates system (X, Y, Z) is defined by a location of the secondary mirror, a vertex of the secondary mirror is an origin of the three-dimensional rectangular coordinates system (X, Y, Z), a reflective surface of the compensating mirror is an xy polynomial freeform surface; and an xy polynomial equation is z ( x , y ) = c ( x 2 + y 2 ) 1 + 1 - ( 1 + k ) c 2 ( x 2 + y 2 ) + ∑ i = 1 N A i x m y n , wherein z represents surface sag, c represents surface curvature, k represents conic constant, while Ai represents an ith term coefficient; and the reflective surface of compensating mirror is a fourth-order polynomial freeform surface of xy without odd items of x; and an equation of the fourth-order polynomial freeform surface of xy is: z ( x , y ) = c ( x 2 + y 2 ) 1 + 1 - ( 1 + k ) c 2 ( x 2 + y 2 ) + A 2 y + A 3 x 2 + A 5 y 2 + A 7 x 2 y + A 9 y 3 + A 1 0 x 4 +
Optical design, e.g. procedures, algorithms, optimisation routines · CPC title
off-axis or unobscured systems in which not all of the mirrors share a common axis of rotational symmetry, e.g. at least one of the mirrors is warped, tilted or decentered with respect to the other elements · CPC title
having a focussing action, e.g. parabolic mirror · CPC title
on-axis systems with at least one of the mirrors having a central aperture · CPC title
with curved faces · CPC title
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