Method and device for measuring optical system lateral magnification by utilizing uniform-speed moving point target

A technology of lateral magnification and optical system, applied in the field of metering equipment, can solve the problem of low repeatability of lateral magnification measurement, achieve the effect of small error, reduce error and improve repeatability

Active Publication Date: 2012-07-25
HARBIN INST OF TECH
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Problems solved by technology

[0028] The present invention aims at the large distortion optical system of the above-mentioned existing measurement method, which is not suitable for measurement in a large field of view, but in a small field of view, there is the problem of low repeatability of lateral magnification measurement, and the existing measurement device has the problem of separation In view of the problem of focusing, a metho...
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Abstract

The invention relates to a method and a device for measuring optical system lateral magnification by utilizing uniform-speed moving point target, belonging to the field of metering equipment taking an optical method as a characteristic. In the method, a points target is imaged under the uniform-speed motion state, so that a linear image is obtained; and in a frequency domain, a value range of pitch of pixels is found, and because the actual modification transfer function curve relative to a pixel pitch and a theoretical modification transfer function curve have the best contact ratio under the least square condition, and the optical system lateral magnification is calculated by a search algorithm to be obtained. In the device, a sliding block for bearing the point target is arranged on first rails and second rails, a controller controls the sliding block to do uniform-speed motion on the first rails, and at the same time, controls the sliding block to do motion on the second rails, and the motions in the two directions are matched, so that during the motion process, the point target is always focused to be imaged onto the surface of an image senor. By adopting the method and the device to measure the optical system lateral magnification rate, the errors between single-time measurement results can be reduced, and further, the repeatability of the measurement results can be improved.

Application Domain

Technology Topic

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  • Method and device for measuring optical system lateral magnification by utilizing uniform-speed moving point target
  • Method and device for measuring optical system lateral magnification by utilizing uniform-speed moving point target
  • Method and device for measuring optical system lateral magnification by utilizing uniform-speed moving point target

Examples

  • Experimental program(1)

Example Embodiment

[0051] Specific embodiments of the present invention will be further described in detail below in conjunction with the accompanying drawings.
[0052] figure 1 It is a structural schematic diagram of an optical system lateral magnification measuring device utilizing a uniform moving point target; the device includes a point target 1, an optical system 2, an image sensor 3, a slider 4, a first guide rail 5 perpendicular to the optical axis direction, and a controller 7, The point target 1 is imaged onto the surface of the image sensor 3 through the optical system 2; and, the device also includes a second guide rail 6 along the optical axis direction, and the slider 4 carrying the point target 1 is installed on the first guide rail 5 and the second guide rail 5. On the guide rail 6, when the controller 7 controls the slider 4 to move at a constant speed on the first guide rail 5, the controller 7 controls the slider 4 to move on the second guide rail 6, and the movement in the two directions cooperates to make the point target 1 in During the movement, images are always in-focus on the surface of the image sensor 3; the point target 1 is a pinhole with a diameter of 15 μm, and the pixel pitch of the image sensor 3 is 5.6 μm.
[0053] The method for measuring the lateral magnification of an optical system using a uniform moving point target, the flow chart is as follows figure 2 As shown, the method steps are as follows:
[0054] a. Set the moving speed v=8.5mm/s of the point target 1 and the exposure time t=359ms of the image sensor 3, the movement displacement of the point target 1 on the object side can be calculated as: d=v·t=8.5×359× 10 -3 = 3.0515mm;
[0055] b. Under the parameters in step a, the image sensor 3 images the point target 1 moving along the direction of the image sensor 3 lines, and obtains the initial point spread function image, such as image 3. Shown; Keep the exposure time t=359ms of the image sensor 3 unchanged, remove the point target 1, the image sensor 3 images the background, obtains the interference image, and uses the maximum value of the gray value in the interference image as the threshold, the threshold is 10;
[0056] c. From the initial point spread function image obtained in step b, extract the entire line information of the point target 1 swept line as the initial line spread function image, such as Figure 4 As shown, and the gray value of the pixel whose gray value in the initial line spread function image is smaller than the threshold value obtained in step b is corrected to 0, and the corrected line spread function image is obtained, as shown in Figure 5 As shown, the modified line extension function image has n=1280 elements;
[0057] or:
[0058] In the initial point spread function image obtained in step b, the gray value of the pixel whose gray value is smaller than the threshold obtained in step b is corrected to 0, as the corrected point spread function image; and in the corrected point spread function image, the point target The entire line information of the scanned line is extracted as a correction line extension function image, such as Figure 5 As shown, the modified line extension function image has n=1280 elements;
[0059] d. Discrete Fourier transform and modulus are performed on the modified line spread function image obtained in the c step to obtain a modulation transfer function image, which has the same number of elements as the modified line spread function image obtained in the c step Number n=1280, that is, 1280 discrete spectral components, according to the order of spatial frequency from small to large, respectively M 0 , M 1 , M 2 ,...,M 1279 , in this order, the MTF value corresponding to the MTF value reaching the minimum value for the first time is M 42 , its subscript sequence number is i=42, combined with the pixel pitch l=5.6 μm of the image sensor 3, M 41 and M 43 The corresponding spatial frequency values ​​are: f min =(i-1)/(nl)=(42-1)/(1280×5.6×10 -3 )=5.7199lp/mm and f max =(i+1)/(nl)=(42+1)/(1280×5.6×10 -3 ) = 5.9989lp/mm;
[0060] e. According to the modulation transfer function model MTF(f)=|sin c(πfd')|, combined with the spatial frequency range f obtained in step d min = 5.7199 lp/mm and f max =5.9989lp/mm, the value range of the motion displacement of point target 1 in the image space is obtained: d max '=1/f min =nl/(i-1)=1280×5.6×10 -3 /(42-1)=0.1748mm and d min '=1/f max =nl/(i+1)=1280×5.6×10 -3 /(42+1)=0.1667mm;
[0061] f. According to the motion displacement d=3.0515mm of point target 1 in the object space obtained in step a and the value range d of the motion displacement of point target 1 in image space obtained in step e min '=0.1667mm and d max ′=0.1748mm, the calculated value range of the lateral magnification of the optical system 3 is: β min = d min '/d=nl/((i+1)d)=1280×5.6×10 -3 /((42+1)×3.0515)=0.0546 and β max = d max '/d=nl/((i-1)d)=1280×5.6×10 -3 /((42-1)×3.0515)=0.0573;
[0062] g. The value range β of the lateral magnification of the optical system 3 obtained in step f min =0.0546 and βmax =0.0573, divide the lateral magnification of the optical system 3 into N=1000 parts on average, respectively β 1 , β 2 ,...,β 1000 , where β 1 = β min =0.0546, β N = β max =0.0573;
[0063] h. According to the order of spatial frequency from small to large, draw the n=1280 modulation transfer function values ​​obtained in step d into a curve, and select this curve from M 0 Start to the first maximum value, and do not include the M obtained in the dth step 42 , a total of K as comparison data, the K modulation transfer function values ​​are M K1 , M K2 ,...,M KK , substituting the N=1000 optical system 3 lateral magnifications obtained in step g into the following formulas respectively: Among the N=1000 values ​​obtained by this formula, the lateral magnification β of the optical system 3 corresponding to the minimum value is the desired value, and after calculation, β=0.0558.
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