Method for carrying out optical measurement by using full-Mueller matrix ellipsometer
A full Mueller matrix and ellipsometer technology, applied in the field of optical measurement, can solve the problems of complex calibration process, increased system complexity, and complex optical measurement method of full Mueller matrix ellipsometer, etc. Accurate parameters and accurate measurement results
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Embodiment 1
[0028] The method for optical measurement using a full-Müller matrix ellipsometer provided in the first embodiment of the present invention includes the following steps:
[0029] Step 1: See attached figure 1 , The experimental optical path of the full-Müller matrix ellipsometer includes light source 1, ring mirror 2, pinhole 3, first off-axis parabolic mirror 4, polarizer 5, first phase compensator 6, first plane mirror 7 , Sample stage 8, second off-axis parabolic mirror 9, third off-axis parabolic mirror 10, second plane mirror 11, second phase compensator 12, analyzer 13, fourth off-axis parabolic mirror 14, spectrometer 15 And the terminal 16, the sample stage 8 carries an isotropic and uniform reference sample; the optical process of the experimental optical path of the full Muller matrix ellipsometer that can be locally regressed and self-calibrated is
[0030] S out =M A R(A′)R(-C′ 2 )M c2 (δ 2 )R(C′ 2 )×M s ×R(-C′ 1 )M c1 (δ 1 )R(C′ 1 )R(-P′)M p R(P)S in
[0031] which i...
Embodiment 2
[0097] See attached image 3 The difference between the full Muller matrix ellipsometer that can be locally regressed and self-calibrated provided in the second embodiment of the present invention and the full Mueller matrix ellipsometer that can be locally regressed and self-calibrated provided in the first embodiment of the present invention is that the present invention The local regression self-calibration method of the full-Müller matrix ellipsometer that can be locally regressed and self-calibrated provided in the second embodiment further includes the following steps:
[0098] According to each experiment Fourier coefficient α′ 2n , Β′ 2n Get each θ 2n , Here, θ 2n It is an intermediate parameter defined for the convenience of calculation;
[0099] According to each θ 2n Get the initial polarization angle C of the first phase compensator s1 ;
[0100] According to each θ 2n Get the initial polarization angle C of the second phase compensator s2 ;
[0101] According to each θ 2n...
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Abstract
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Application Information
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