A Phase Extraction Method Based on Complementary Error Correction for Phase-shifting Interferometry
A technology of error complementation and phase-shifting interference, which is applied in measuring devices, special data processing applications, instruments, etc., can solve problems such as cumbersome formulas, large amount of calculation, singular phase solution, etc., and achieve the effect of simple and fast calculation
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specific Embodiment approach 1
[0033] Specific embodiment one: a phase-shifting interferometry phase extraction method based on error complementary correction, characterized in that: a phase-shifting interferometry phase extraction method based on error complementary correction is specifically carried out according to the following steps:
[0034] Step 1. The expression form of the traditional five-frame algorithm is:
[0035]
[0036] in, is the phase to be solved, I 1 , I 2 , I 3 , I 4 , I 5 Take the light intensity of each frame sequence corresponding to the phase shift amount of -π, -π / 2, 0, π / 2, and π respectively, and obtain the phase information extracted by the traditional five-frame algorithm;
[0037] Step 2. Use the light intensity of the same frame sequence as the traditional five-frame algorithm to substitute into the constructed new five-frame algorithm to obtain the phase information extracted by the new five-frame algorithm. The constructed five-frame algorithm is in the form of;
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specific Embodiment approach 2
[0041] Specific embodiment two: the difference between this embodiment and specific embodiment one is: the light intensity of the same frame sequence as the traditional five-frame algorithm is used in the step two, that is, the phase shift amount is -π, -π / 2, 0, When π / 2, π (the phase-shift step size is π / 2), the five-frame algorithm form constructed under any step size becomes the form described in formula (2), and the five-frame algorithm form constructed under any step size is:
[0042]
[0043] In the formula: is the phase to be solved, I 1 , I 2 , I 3 , I 4 , I 5 Respectively correspond to the light intensity of each frame sequence when the phase shift step size is β. Other steps and parameters are the same as those in Embodiment 1.
specific Embodiment approach 3
[0044] Specific embodiment three: the difference between this embodiment and specific embodiment one or two is: the phase to be solved described in the formula (3) The specific calculation process is:
[0045] The five-frame light intensity equations under any equal step size in the interference field are shown in formula (4):
[0046]
[0047] In the formula: is the phase to be solved, I is the light intensity of each frame sequence in the interference field, I 1 , I 2 , I 3 , I 4 , I 5 Respectively correspond to the light intensity of each frame sequence when the phase shift step is -2β, -β, 0, β, 2β; A is the DC component of the light intensity, B is the AC component of the light intensity, and β is the phase shift step size;
[0048] Will I 2 with I 4 , I 1 with I 5 Do difference, after trigonometric function and difference product operation, formulas (5) and (6) are respectively obtained after arrangement:
[0049] I 2 -I 4 =2B·sin(φ)·sin(β) (5)
[0050...
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