Athermalized diffractive optical elements

• US 5,745,289 A
• Filed: 06/21/1996
• Issued: 04/28/1998
• Est. Priority Date: 06/21/1996
• Status: Expired due to Term

• Current Assignee: Eastman Kodak Company
• Original Assignee: Eastman Kodak Company
• Inventors: Hamblen, David P.
• Primary Examiner(s): Dzierzynski, Paul M.
• Assistant Examiner(s): Juba, Jr., John
• Application Number:
  US08/668,166
• Time in Patent Office: 676 Days
• Field of Search: 359/356, 359/565, 359/569, 359/570, 359/571, 359/575, 359/742, 359/900
• US Class Current: 359/565
• CPC Class Codes: G02B 5/1876 Diffractive Fresnel lenses; Zone plates; Kinoforms G02B5/1842, G02B5/1847 take precedence; optical systems having diffractive correction means G02B27/0037; Fresnel lenses operating by refraction G02B3/08
• CPC Class Codes: G02B 5/1895 such optical elements having dioptric power
• CPC Class Codes: Y10S 359/90 Methods

Abstract

A diffractive optical element, ("DOE"), and particularly a diffractive lens having annular zones about an optical axis and known as a Fresnel zone plate or kinoform lens, is athermalized so that its effective focal length ("EFL") does not shift substantially with temperature over a temperature range by, respectively, increasing and decreasing the zone widths with respect to widths which are optimized to focus at the EFL at room temperature. Half of the zones (alternate, adjacent zones) provide the correct EFL for the expanded condition of the lens at the hot end of the temperature range; the other half of the zones provide correct EFL for the contracted condition of the lens at the cold end of the temperature range. The exact spacings and zone widths are obtained, in the same manner as a diffractive lens is corrected for spherical and chromatic aberration, from the coefficients of the equation governing the phase shift through the lens as a function of radial distance from the optical axis, by averaging the aberration properties at the hot and cold ends of the range, the net effect of which is to dictate the spacing of alternate, successive zones which are slightly greater and less than the zone spacings optimized at room temperature, respectively.

Claims

1. A method of manufacturing an optical element from a light transmissive body of material, subject to changes in dimension with temperature, which method comprises the steps of

determining the nominal location of a plurality of lines on a surface of said body to define the nominal widths of successive zones of a diffractive optical element (DOE);

specifying an actual spacing between adjacent ones of said lines which define the zones of said DOE, said actual spacing being a function of the dimensional changes of said material with temperature such that at least some of the zones of said DOE approach their nominal widths in response to temperature changes in an amount sufficient to athermalize said DOE across a range of temperature; and

forming zones on a surface of said body in accordance with said actual spacing, wherein

said nominal zone widths are determined at a certain temperature between the lower, colder temperature and the upper, hot temperature ends of said range; and

said actual spacings define at least some zones of increased width and some zones of decreased width, with respect to said nominal zone widths at said certain temperature.

2. The method according to claim 1 wherein said step of specifying actual spacing is carried out by sufficiently increasing and decreasing the widths of successive alternate zones, respectively, thereby athermalizing said DOE over said range.

3. The method according to claim 2 wherein said certain temperature is room temperature.

4. The method according to claim 2 wherein said forming step is carried out by blazing said surface to form ramps having sloping portions between steps, which steps define said lines and said sloping portions defining the widths of said zones.

5. The method according to claim 1 wherein said DOE is a diffractive lens having an effective focal length (EFL) along an optical axis, and said forming step is carried out to form said zones as annular zones about said axis.

6. The method according to claim 5 wherein said step of specifying an actual spacing is carried out by sufficiently increasing and decreasing the widths of alternate successive zones which are radially spaced at successively larger radial distances from said optical axis, respectively.

7. The method according to claim 5 wherein spacing between said lines in a radial direction defines annular zones of width having said spacing of said lines, and said step of specifying an actual spacing is carried out to define at least some zones of increased width and some zones of decreased width with respect to the width thereof at a certain temperature between the upper, hot end of said range and the lower, cold end or said range to maintain the EFL approximately constant over said range.

8. The method according to claim 6 wherein said certain temperature is room temperature.

9. The method according to claim 6 wherein said step of specifying an actual spacing is carried out to form said zone widths with spacing sufficient to focus an image over a field in a plane at said EFL, which plane is perpendicular to said optical axis, thereby providing an athermalized, diffractive field lens.

10. The method according to claim 6 wherein said step of specifying an actual spacing is carried out to provide alternate zone widths such that they are of such widths as to provide said EFL, respectively, at the hot and cold ends of said range.

11. The method according to claim 7 wherein said forming step is carried out by blazing said surface to form ramps having sloping portions between steps, which steps define said lines, and said sloping portions defining the widths of said zones.

12. The method according to claim 7 further comprising the step of forming a curved surface on a surface of said body opposite to the surface on which said diffractive lens is formed, thereby providing a hybrid refractive/diffractive lens.

13. The method according to claim 7 further comprising the step of forming said surface with a given curvature to define a base curvature of said diffractive lens.

14. The method according to claim 13 further comprising the step of forming a curved surface on a surface of said body opposite to the surface on which said diffractive lens is formed, thereby providing a hybrid refractive/diffractive lens.

15. The method according to claim 7 wherein said forming step is carried out to provide less than 20 zones at successively increasing spacing from said optical axis.

16. The method according to claim 7 wherein the phase shift through said diffractive lens as a function of radial distance, r, from the optical axis is

17. A diffractive optical element (DOE) which comprises a light transmissive body of material subject to changes in dimension with temperature, a plurality of lines on a surface of said body which define a grating having a plurality of zones, successive ones of which zones are adjacent each other, and the spacings between said lines which define the widths zones differing from each other in an amount sufficient to athermalize said DOE across a range of temperature, wherein at least some of the zones have a width greater than their nominal zone widths at a certain temperature, and at least some of the zones have a width less than their nominal zone widths at said certain temperature, said certain temperature being between the lower, cold temperature and the upper, hot temperature ends of said range.

18. The element according to claim 17 wherein the widths of alternate successive zones are respectively increased and decreased, with respect to said nominal zone widths at said certain temperature, in an amount sufficient to athermalize said DOE over said temperature range.

19. The element according to claim 18 wherein said certain temperature is room temperature.

20. The element according to claim 17 wherein said DOE is a diffractive lens having an effective focal length (EFL) along an optical axis, and said zones are annular zones around said axis.

21. The lens according to claim 20 wherein spacing between said lines in a radial direction defines annular zones of width having said spacing of said lines, and said spacing is sufficient to increase and decrease the width of said zones with respect to the width thereof at a certain temperature between the upper, hot end of said range and the lower, cold end of said range to maintain the EFL approximately constant to over said range.

22. The lens according to claim 20 wherein said widths of successive adjacent zones which are radially spaced at successively larger radial distances from said optical axis, respectively, are increased and decreased with respect to said width at said certain temperature.

23. The lens according to claim 22 wherein said certain temperature is room temperature.

24. The lens according to claim 21 wherein said zone widths are defined by such widths as to focus an image over a field in a plane at said EFL, which plane is perpendicular to said optical axis, thereby providing an athermalized, diffractive field lens.

25. The lens according to claim 21 wherein said alternate widths are such that they provide said EFL, respectively, at the hot and cold ends of said range.

26. The lens according to claim 21 wherein said surface is blazed to form ramps having sloping portions between steps, which steps define said lines and said sloping portions defining the widths of said zones.

27. The lens according to claim 21 wherein said body has opposite surfaces, one of which is a curved surface and the other of which is a surface on which said diffractive lens is formed, thereby providing a hybrid refractive/diffractive lens.

28. The lens according to claim 27 wherein said other surface has a given curvature and defines a base curvature of said diffractive lens.

29. The lens according to claim 21 wherein said spacing provides less than 20 zones at successively increasing spacing from said optical axis.

30. The lens according to claim 17 wherein the phase shift through said diffractive lens as a function of radial distance, r, from the optical axis is