Dual-wavelength phase-shift interference aspheric surface measurement method and device based on partial compensation method
A technology of phase-shift interference and measurement method, which is applied in the field of high-precision measurement of optical aspheric surface error, can solve the problems of increasing the difficulty and cycle of instrument design, shorten the cycle of instrument design, reduce the difficulty and cost of system design, and achieve high The effect of precision reconstruction
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[0064] Example 1: Measurement of large asphericity ellipsoid surface.
[0065] The implementation device of this embodiment is as figure 2 As shown, the working wavelength λ output by the first laser (1) and the second laser (2) 1 And λ 2 Respectively 532nm and 556nm, the resulting equivalent synthetic wavelength λ eq It is 12.325μm, and the maximum measurable difference between adjacent optical path differences is 6.162μm.
[0066] In this embodiment, the transparent aperture D of the tested ellipsoidal surface (13) is 580mm, and the curvature radius of the aspheric surface is R 0 It is -1179.447mm, the relative diameter of aspheric surface is D / R 0 The maximum asphericity of the tested ellipsoid relative to the vertex sphere and the best reference sphere is 281.85μm and 67.80μm, respectively, which is a fairly large aspherical surface. This embodiment is in large aspherical surface The additional facet error of the ellipsoid produces a steep wavefront.
[0067] The glass material ...
Example Embodiment
[0079] Example 2: Parabolic measurement with large surface error.
[0080] In this embodiment, the tested aspheric surface (13) is a parabolic surface with large surface error, its clear aperture D is 108mm, and the vertex radius of curvature R 0 -1727.2mm, the relative diameter of the paraboloid is D / R 0 1 / 16, the maximum asphericity of the tested parabola relative to the vertex sphere and the best reference sphere are 0.206μm and 0.052μm, respectively, which is a shallow aspheric surface.
[0081] The glass material of the partial compensation mirror (12) designed to compensate for the parabola is K9, and the curvature radius of the front and rear surfaces is r 1 And r 2 They are 760mm and -4965mm respectively, which are also a simple double convex lens. The thickness of the partial compensation mirror (12) is 20mm, and the distance between the partial compensation mirror (12) and the measured aspheric surface (13) is 2985mm.
[0082] Using the method proposed by the present inventi...
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