Method for measuring spherical aberration of confocal system
A measurement method and spherical aberration technology, applied in the direction of testing optical performance, etc., can solve problems such as difficulty in improving measurement accuracy, and achieve the effects of improving anti-environmental interference ability, improving fixed focus sensitivity, and improving the degree of automation
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Embodiment 1
[0040] When the measured system 5 is a plano-convex lens with a diameter of D=76mm, a material of K9 glass, a thickness of b=8mm, and a focal length of f′=500mm, the spherical aberration measurement device of the confocal system is as follows: Figure 4 As shown, the measurement steps are:
[0041] (a) Start the measurement software in the main control computer 13, turn on the laser 20, and the light emitted by the laser 20 is transmitted through the optical fiber 19 to form the point light source 1. The light emitted by the point light source 1 passes through the beam splitter 2, the collimating lens 3 and the annular pupil 4 to form an annular beam with a flat wavefront;
[0042] (b) the plane mirror 7 is placed on the two-dimensional adjustment frame 17, and the plane mirror 7 is adjusted by the two-dimensional adjustment frame 17 so that its surface is perpendicular to the optical axis of the collimating lens 3;
[0043] (c) The system under test 5 is placed between the a...
Embodiment 2
[0053] According to the measured system 5 measured in embodiment 1, the light passing height is h 1 ~ h n The corresponding spherical aberration δL 1 '~δL n ′, it can be obtained by interpolation method that when the normalized light transmission height is 1.0, 0.85, 0.7071, 0.5, 0.3, the spherical aberration corresponding to the measured system 5 is respectively δL a '=-3.1827mm, δL b '=-2.2959mm, δL c '=-1.5989mm, δL d '=-0.7923mm, δL e '=-0.2845 mm. In order to comprehensively and generally express the spherical aberration of the measured system 5 under different light-passing heights, δL is usually taken a ', δL b ', δL c ', δL d ', δL e 'These five representative spherical aberrations describe the structure of the entire beam.
Embodiment 3
[0055] The difference from Embodiments 1 and 2 is that in this embodiment, the annular pupil is replaced by an amplitude-type spatial light modulator, and the parallel beam is converted into an annular beam with a certain light-passing height through the amplitude-type spatial light modulator, and then the The measurement process of the spherical aberration of the system. The switching speed of the ring beam and the degree of automation of the measurement system can be improved by the amplitude-type spatial light modulator.
[0056] This embodiment realizes the measurement of the spherical aberration of the system under test 5 through a series of measures. During the measurement process, the confocal measurement method is used to precisely focus the beam focus of the system under test 5 under different annular pupils, and then measure the spherical aberration of the system under test 5, with high measurement accuracy and strong anti-environmental interference ability .
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