CN115183699B - Method and device for quickly and relatively measuring differential confocal curvature radius of rear-mounted split pupil - Google Patents
Method and device for quickly and relatively measuring differential confocal curvature radius of rear-mounted split pupil Download PDFInfo
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Abstract
The invention discloses a method and a device for quickly and relatively measuring a post-split pupil differential confocal curvature radius, belonging to optical precision measurementThe technical field of measuring. The invention selects a known curvature radius R from the same batch of tested elements 0 Is used as a template S 0 Scanning is carried out at the confocal position to obtain a differential confocal light intensity response curve and a linear section fitting equation thereof; sequentially loading and clamping tested pieces S n Mapping the collected differential light intensity values to a linear segment fitting equation to achieve S n Defocus amount Δz n Is a scanning-free rapid measurement of (1); by Deltaz n And R is 0 Calculating to obtain the curvature radius R of the measured element n . Compared with the existing high-precision curvature radius measuring method, the method can not only keep the advantages of differential confocal high-precision measurement, but also remarkably improve the measuring efficiency and the processing efficiency and precision of a large number of spherical elements.
Description
Technical Field
The invention relates to a method and a device for quickly and relatively measuring a post-spectroscopic pupil differential confocal curvature radius, belonging to the technical field of optical precision measurement.
Background
Spherical optical elements are used in a large number of optical systems for medical inspection, digital cameras, and the like, and thus have a great demand and throughput. The precision of the curvature radius of the spherical optical element directly determines the performance of the optical system, so that the detection precision of the spherical optical element has great significance in the field of optical measurement.
Currently, the measurement methods of the radius of curvature can be divided into two types, contact type and non-contact type:
common contact measurement methods include a template method, a sphere diameter meter method, a three-coordinate method, a laser tracking method and the like. The sample plate method and the sphere diameter meter method are simple and convenient to operate and high in measuring speed. However, the template method is influenced by the precision of the template and the stress variation between the measured mirrors, the measurement precision is not high and is influenced by subjective factors of measurement staff; the measurement accuracy of the ball diameter meter method is only 30ppm, and the measurement accuracy of the method is reduced along with the increase of the curvature radius value. The three-coordinate method is to scan the sphere to be measured to obtain the best fit sphere as the measurement result of the curvature radius, and the measurement precision is 20ppm. However, this method is not suitable for small radius of curvature measurement and the measurement efficiency is low. The radius of the laser tracking ball is measured by the laser tracking method, the radius of curvature of the ball to be measured is calculated, the relative measurement precision is 18ppm, the method is only suitable for measuring spherical elements with large calibers, and the measurement flow is complicated. The contact measurement methods have the inherent defect of being easy to scratch the surface of a measured sample.
Non-contact measurement methods mainly include geometrical optics and interferometry. Geometrical optics methods include knife-edge shading, auto-collimation, and the like. The knife-edge shadow method is used for measuring the curvature radius value, the operation is simple and convenient, but the measurement accuracy is not high, and only 50ppm is needed. The auto-collimation method is only suitable for measuring the curvature radius of a large-caliber element, and the precision is 500ppm when the curvature radius is measured by more than 5 m. For interferometry, it is a high-precision measurement method that is widely used at present. Classical interferometry uses a phase measurement interferometer to fix focus on the cat eye position and the confocal position of the measured spherical surface respectively, so as to obtain the radius of curvature to be measured, and the measurement accuracy can reach 10ppm. On this basis, jan.K et al propose a fast detection method based on wavelength tuning phase shifting for absolute interferometry with a measurement accuracy of 10ppm. However, the interference method has the problems that the posture adjustment process is complicated, the interference fringes are required to be stabilized for a long time after clamping, and the like, and in addition, the interference fringes are extremely easy to be interfered by environmental factors such as air flow, temperature, vibration and the like, so that the method has low efficiency.
The present inventors have provided a laser differential confocal curvature radius measurement method in 2010, which uses the characteristic that an absolute zero point of a differential confocal light intensity response curve corresponds to a measurement beam focus precisely to focus a cat eye position and a confocal position of a measured surface, thereby obtaining a curvature radius to be measured. The accuracy of the method can reach 5ppm, but the method still needs to scan and fix focus at two points of the cat eye position and the confocal position, and also needs to perform a complicated posture adjustment process. The efficiency of the process is therefore to be further improved.
Disclosure of Invention
In order to solve the problem of low efficiency of high-precision measurement of the curvature radius of batch spherical elements, the invention mainly aims to provide a method and a device for quickly and relatively measuring the curvature radius of a rear-mounted split pupil differential confocal curvature, which utilize the rear-mounted split pupil differential accurate focusing to convert the absolute measurement process of the curvature radius into the relative measurement based on a template, so that the advantages of differential confocal high-precision measurement can be maintained, the measurement efficiency can be obviously improved, the curvature radius of the spherical elements can be effectively, quickly and conveniently detected, and the high-efficiency and high-precision processing detection of the batch spherical elements can be realized.
The aim of the invention is achieved by the following technical scheme.
The invention discloses a method for quickly and relatively measuring the radius of curvature of a rear split pupil differential confocal curvature, which can realize quick and high-precision measurement of the radius of curvature of a spherical element and comprises the following specific steps:
step one: selecting templates S in the same batch as the measured lens in the batch elements 0 Nominal value of element parameter of template and N identical batches of measured mirrors S 1 -S N The same applies.
The element parameters include radius of curvature, caliber, surface reflectivity.
Step two: s by utilizing a post-positioned split pupil differential confocal focusing system 0 Scanning near the confocal position, performing differential processing on the acquired light intensity signals to obtain a differential confocal curve, and performing linear fitting on the linear section of the curve to obtain a fitting straight line l diff (z) according to l diff (z) the axial position coordinate of zero will S 0 And the device is precisely positioned at the confocal position, so that precise focusing of the measured element is realized.
Step three: s is taken down from the vertical fixture 0 And sequentially clamps the tested lens S n N=1 to N, the process ensures S by the self gravity of the measured mirror n Is used for repeated spatial positioning. Acquisition card S by utilizing rear-mounted split pupil differential confocal focusing system n The differential light intensity value is mapped to l diff (z) further obtaining the defocus amount Δz n The rapid measurement of the batch of components is ensured.
Step four: by using conversion relation, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n The advantages of differential confocal high-precision measurement can be maintained, the measurement efficiency can be obviously improved, and further the measurement is realizedThe curvature radius of the spherical element is detected efficiently, quickly and conveniently.
Preferably, the implementation method of the fourth step is as follows: by using the conversion relation shown in the following formula, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n 。
Wherein R is 0 For calibrating sample plate S 0 Radius of curvature R of (2) n For the radius of curvature of the sample to be measured, Δz n Represents the sphere center O of the calibration sample plate 0 And the sphere center O of the tested sample n Axial offset between D F The clamping diameter of the supporting clamp is set. The advantage of differential confocal high-precision measurement is reserved, and the measurement efficiency is remarkably improved.
Preferably, the implementation method of the fourth step is as follows: by using the conversion relation shown in the following formula, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n The method can not only keep the advantages of differential confocal high-precision measurement, but also remarkably improve the measurement efficiency, thereby realizing high-efficiency, rapid and convenient detection of the curvature radius of the spherical element.
Wherein R is 0 For calibrating sample plate S 0 Radius of curvature R of (2) n For the radius of curvature of the sample to be measured, Δz n Represents the sphere center O of the calibration sample plate 0 And the sphere center O of the tested sample n Axial offset between D F The clamping diameter of the supporting clamp is set.
The invention discloses a method for quickly and relatively measuring the differential confocal curvature radius of a rear-end split pupil. According toThe detected elliptic light spots are symmetrically provided with virtual pinhole front focus vph1 and back focus vph2 at the two confocal sides of a circular detection area, namely the virtual pinhole, at the optical axis position. Taking gray value integral in the virtual pinholes as detection light intensity, and obtaining a differential confocal response curve by detecting axial light intensity responses of the two virtual pinholes and performing differential processing, wherein the differential light intensity value I of a measured piece is obtained diff (Δz n ) Expressed as:
I diff (Δz n )＝I vph2 (Δz n )-I vph1 (Δz n )
wherein I is vph1 (Δz n ) Represented as the intensity value, I, at the virtual pinhole front focal vph1 vph2 (Δz n ) Is the light intensity value at the virtual pinhole front focal vph2. And obtaining a fitting straight line with a high slope and a long linear range through linear fitting, so as to ensure the curvature radius measurement precision and the measurement range.
The invention discloses a method for quickly and relatively measuring the differential confocal curvature radius of a rear split pupil, which is characterized in that I is set through a threshold value ts And judging whether the defocus amount is in a linear response interval. Template S 0 Light intensity response I of virtual pinhole obtained by scanning vph1 、I vph2 Summing to obtain light intensity response sum I sum ：
I sum ＝I vph1 +I vph2
Wherein I is vph1 Represented as the intensity value, I, at the virtual pinhole front focal vph1 vph2 Is the light intensity value at the virtual pinhole front focal vph2.
As the tested piece S n Collected single point light intensity response sum I sumn >I ts When the differential light intensity value is judged to be in the linear response interval, namely the measured piece is not out of range, and the next measurement can be carried out; as the tested piece S n Collected single point light intensity response sum I sumn <I ts And when the differential light intensity value is judged to be outside the linear response interval, namely the measured piece is out of range, and information that the measured piece cannot be measured is returned. Thus according to I sum Whether or not it is greater than I ts So as to realize the judgment of the over-range.
The invention discloses a method for quickly and relatively measuring the differential confocal curvature radius of a rear split pupil, which adopts a vertical annular clamping structure to ensure that a sample plate and each measured piece can be quickly and stably clamped by self gravity, and ensure that the corresponding weft lines (namely the contact lines of spherical elements and annular clamps) with the same sagittal height on the spherical surface can be repeatedly positioned at the same space position after the spherical elements in the same batch are clamped. For concave sphere measurement, the outer circle of the ring fixture is contacted with the measured sphere; for convex sphere measurements, the inner circle of the ring fixture is in contact with the sphere being measured.
The invention also discloses a device for quickly and relatively measuring the differential confocal curvature radius of the rear split pupil, which is used for realizing the method for quickly and relatively measuring the differential confocal curvature radius of the rear split pupil. The device for quickly and relatively measuring the rear-end split pupil differential confocal curvature radius comprises a rear-end split pupil differential confocal module, a motion control and monitoring module and an attitude adjusting module. The rear-end split pupil differential confocal module uses a D-shaped diaphragm to set a light spot on a CCD detection surface as a virtual pinhole position, and performs differential processing on axial light intensity response of the light spot, so that accurate focusing of a tested element is realized. The rear split pupil differential confocal module comprises a point light source, a collimating mirror, a reflecting mirror, a converging mirror, a D-shaped diaphragm, a microscope objective and a photoelectric detector CCD.
The motion control module drives the screw rod to drive the high-precision air floatation guide sleeve to move along the optical axis direction by using the servo motor, and simultaneously monitors the position information in real time by using the grating ruler to finish scanning and position data acquisition. The motion control module comprises a servo motor, a screw rod, a high-precision air floatation guide sleeve, a high-precision air floatation guide rail and a grating ruler. The gesture adjusting module uses a two-dimensional adjusting frame to adjust the spatial positions of the standard converging mirror and the measured mirror, so that the center of the gesture adjusting frame coincides with the optical axis, and the absolute measuring process of the curvature radius is converted into the relative measurement based on the sample plate. The attitude adjustment process utilizes an annular clamp to quickly and accurately position the measured piece at the confocal position of the specific template. The gesture adjusting module comprises a two-dimensional adjusting frame and an annular clamp.
The beneficial effects are that:
1. the invention discloses a method and a device for quickly and relatively measuring the differential confocal curvature radius of a rear-end split pupil, wherein the method and the device are used for scanning at the confocal position of a spherical element with a known curvature radius, and obtaining a fitting equation of a linear section of the spherical element through differential confocal scanning; then the measured spherical element is clamped, single-point differential light intensity is collected and mapped into a linear section fitting equation, so that the rapid scanning-free measurement of the defocus amount of the measured element is realized, and the problem that the conventional measurement method of the curvature radius of the spherical optical element is difficult to meet the measurement requirements of large batch and high speed is solved.
2. The invention discloses a method and a device for quickly and relatively measuring the differential confocal curvature radius of a rear-end split pupil. The invention converts the absolute measurement process of the radius of curvature into a template-based relative measurement. The invention not only can keep the advantages of differential confocal high-precision measurement, but also can obviously improve the measurement efficiency and the processing efficiency and precision of a large number of spherical elements.
3. The invention discloses a method and a device for quickly and relatively measuring the differential confocal curvature radius of a rear-end split pupil, which adopt a vertical annular clamping structure to ensure that a sample plate and each measured piece can be quickly and stably clamped by self gravity, ensure that the corresponding weft lines (namely the contact lines of the spherical elements and an annular clamp) with the same sagittal height on the spherical surface can be repeatedly positioned at the same space position after the spherical elements in the same batch are clamped, and can realize the quick, high-precision and non-contact detection of the curvature radius of the spherical elements of N pieces only by one-time scanning measurement and N-time single clamping measurement. The invention can solve the problem of low production and manufacturing efficiency of the existing optical element, meet the detection requirements in the large-scale processing and assembling process, and improve the detection efficiency of the curvature radius.
Drawings
FIG. 1 is a flow chart of the post-spectral pupil differential confocal radius of curvature quick relative measurement of the present invention;
FIG. 2 is a schematic diagram of the invention based on post-spectral pupil differential confocal detection;
FIG. 3 is a graph of the radius of curvature versus measured geometry for a concave spherical surface for example 1 of the present invention;
FIG. 4 is a graph of the radius of curvature versus measured geometry for a convex sphere for example 2 of the present invention;
FIG. 5 is a diagram of a method and apparatus for rapid relative measurement of the differential confocal radius of curvature of a post-split pupil for a concave sphere according to embodiment 1 of the present invention;
FIG. 6 is a diagram of a method and apparatus for rapid relative measurement of the differential confocal radius of curvature of a post-split pupil for convex spherical surfaces according to example 2 of the present invention;
wherein: 1-point light source, 2-polarization spectroscope, 3-collimating mirror, 4-reflecting mirror, 5-D diaphragm, 6-microscope objective, 7-optical detector CCD, 8-adjusting frame, 9-converging mirror, 10-clamp, 11-motor, 12-screw rod, 13-grating reading head, 14-air floatation guide sleeve, 15-air floatation guide rail, 16-grating ruler and 17-sample plate S 0 18-element under test S n 19-virtual pinhole front coke vph1, 20-virtual pinhole back coke vph2, 21-front Jiao Guangjiang I vph1 22-rear Jiao Guangjiang I ph2 23-differential confocal light intensity curve, 24-fitting straight line l diff (z), 25-defocus amount Δz, 26-differential confocal single-point light intensity value I diff (Δz)。
Detailed Description
The invention is further described below with reference to the drawings and examples.
Example 1
As shown in FIG. 5, the method and the device for quickly and relatively measuring the differential confocal curvature radius of the rear-end split pupil comprise a rear-end split pupil differential confocal module, a motion control and monitoring module and an attitude adjustment module. The rear-end split pupil differential confocal module uses a D-shaped diaphragm 5 to set a light spot on a CCD detection surface 7 as a virtual pinhole position, and performs differential processing on the axial light intensity response of the light spot, so that accurate focusing of a tested element is realized. The post-split pupil differential confocal module comprises a point light source 1, a collimating lens 3, a reflecting mirror 4, a converging lens 9, a D-shaped diaphragm 5, a microscope objective 6 and a photoelectric detector CCD7.
The motion control module drives the screw rod 12 to drive the high-precision air floatation guide sleeve 14 to move along the optical axis direction by using the servo motor, and simultaneously monitors the position information in real time by using the grating ruler 16 to finish scanning and position data acquisition. The motion control module comprises a servo motor 11, a screw rod 12, a high-precision air floatation guide sleeve 14, a high-precision air floatation guide rail 15 and a grating ruler 16. The attitude adjustment module uses the two-dimensional adjustment frame 8 to adjust the spatial positions of the standard converging mirror 9 and the measured mirror 18 so that the centers of the standard converging mirror and the measured mirror coincide with the optical axis, and converts the absolute measurement process of the curvature radius into the relative measurement based on the template. The attitude adjustment process uses the ring jig 10 to quickly and accurately position the measured piece at the confocal position of the specific template. The gesture adjusting module comprises a two-dimensional adjusting frame 8 and an annular clamp 10.
When the device is used for measuring the curvature radius of batch elements, a post-spectroscopic pupil differential confocal detection technology is adopted to obtain a differential confocal curve, as shown in fig. 2, measuring light reflected by the measured elements passes through the D-shaped diaphragm 5 and the microscope objective 6, and is imaged on the detection surface of the CCD7. The detected elliptical light spot is provided with a circular detection area at the optical axis position, and the front focal vph1 and the rear focal vph2 of the virtual pinhole 19 and the virtual pinhole 20 are symmetrically arranged at the two confocal sides. The gray value integration in the virtual pinholes is used as detection light intensity, the axial light intensity response of the two virtual pinholes is detected and differential processing is carried out, a differential confocal response curve 23 is obtained, and a fitting straight line with high slope and long linear range is obtained through linear fitting, so that the curvature radius measurement precision and the measurement range are ensured.
The method and the device for quickly and relatively measuring the differential confocal curvature radius of the rear-end split pupil adopt a vertical annular clamping 10 structure to ensure that a sample plate and each measured piece can be quickly and stably clamped by self gravity, and ensure that the weft corresponding to the same sagittal height (namely the contact line of the spherical element and the annular clamp) on the spherical surface can be repeatedly positioned at the same space position after the spherical elements of the same batch are clamped. As shown in fig. 5 and 6, the device can measure for concave and convex spherical surfaces. For concave sphere measurement, the outer circle of the ring fixture is in contact with the measured sphere, as shown in fig. 3; for convex sphere measurements, the inner circle of the ring fixture is in contact with the sphere being measured, as shown in fig. 4.
The device is used for respectively placing the calibration sample plate and the element to be measured on the same fixture, and the spherical center position of the device can deviate by delta z in the optical axis direction due to the small difference of the curvature radiuses of the calibration sample plate and the element to be measured n Further according to the defocus amount Deltaz n And obtaining the curvature radius to be measured.
The measurement procedure for the concave sphere is as follows:
step one: a template 17 of the same batch as the measured mirrors is selected from the batch of elements, and the nominal values of the element parameters of the template are the same as those of N measured mirrors 18 of the same batch. The element parameters include radius of curvature, caliber, surface reflectivity.
Step two: scanning is carried out near the confocal position of the sample plate 17 by utilizing a rear-end spectral pupil differential confocal focusing system, differential processing is carried out on the acquired light intensity signals to obtain a differential confocal curve 23, linear fitting is carried out on the linear section of the curve to obtain a fitting straight line 24, the sample plate 17 is accurately positioned at the confocal position according to the axial position coordinates of the 24 zero point, and accurate focusing of the measured element is realized.
Step three: the template 17 is removed from the vertical clamp and the measured lens 18 is sequentially clamped, and the repeated spatial positioning of the measured lens 18 is ensured by the gravity of the measured lens. For concave sphere measurement, the outer circle of the ring fixture is in contact with the sphere to be measured. The differential light intensity value after the tested lens 18 is clamped is collected by a rear-end split pupil differential confocal focusing system and mapped to a fitting straight line 24 to obtain a defocus 25, as shown in fig. 3.
Step four: according to D F Measured as 29.980mm from the radius of curvature R of the calibration template 0 = -39.1042mm and defocus amount Δz 1 =0.0097 mm, usingFormula, R is calculated 1 = -39.0963mm, which is the radius of curvature of the concave spherical surface of the measured element.
Example 2
As shown in fig. 6, the method and the device for measuring the radius of curvature of the convex spherical surface by the rapid relative measurement of the differential confocal curvature radius of the rear split pupil are similar to those of fig. 5.
The measurement procedure for the convex sphere is as follows:
step one: a template 17 of the same batch as the measured mirrors is selected from the batch of elements, and the nominal values of the element parameters of the template are the same as those of N measured mirrors 18 of the same batch. The element parameters include radius of curvature, caliber, surface reflectivity.
Step two: scanning near the confocal position of the template 17 by using a post-spectroscopic pupil differential confocal focusing system, performing differential processing on the acquired light intensity signals to obtain a differential confocal curve 23, performing linear fitting on the linear section of the curve to obtain a fitting straight line 24, and accurately positioning the template 17 at the confocal position according to the axial position coordinates of the 24 zero points.
Step three: the template 17 is removed from the vertical clamp and the measured lens 18 is sequentially clamped, and the repeated spatial positioning of the measured lens 18 is ensured by the gravity of the measured lens. For convex sphere measurements, the inner circle of the ring fixture is in contact with the sphere being measured. The differential light intensity value after the tested lens 18 is clamped is collected by the post-split pupil differential confocal focusing system and mapped to the fitting straight line 24 to obtain the defocus 25, as shown in fig. 4.
Step four: according to D F Measured as 29.986mm from the radius of curvature R of the calibration template 0 =39.1 mm and defocus Δz 2 =0.0303 mm, usingThe formula is given to R 2 = 39.10644mm, which is the radius of curvature of the convex spherical surface of the element under test.
The above description of the embodiments of the invention has been presented in connection with the drawings but these descriptions should not be construed as limiting the scope of the invention, which is defined by the appended claims, and any changes based on the claims are intended to be covered by the invention.
Claims (6)
1. The method for quickly and relatively measuring the differential confocal curvature radius of the rear-mounted split pupil is characterized by comprising the following steps of: comprises the following steps of the method,
step one: selecting templates S in the same batch as the measured lens in the batch elements 0 Nominal value of element parameter of template and N identical batches of measured mirrors S 1 -S N The same;
the element parameters comprise curvature radius, caliber and surface reflectivity;
step two: s by utilizing a post-positioned split pupil differential confocal focusing system 0 Scanning near the confocal position, performing differential processing on the acquired light intensity signals to obtain a differential confocal curve, and performing linear fitting on the linear section of the curve to obtain a fitting straight line l diff (z) according to l diff (z) the axial position coordinate of zero will S 0 The device is precisely positioned at the confocal position, so that precise focusing of the measured element is realized;
step three: s is taken down from the vertical fixture 0 And sequentially clamps the tested lens S n N=1 to N, the process ensures S by the self gravity of the measured mirror n Is used for repeated space positioning; acquisition card S by utilizing rear-mounted split pupil differential confocal focusing system n The differential light intensity value is mapped to l diff (z) further obtaining the defocus amount Δz n The rapid measurement of batch elements is ensured;
step four: by using conversion relation, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n The advantages of differential confocal high-precision measurement can be reserved, the measurement efficiency can be remarkably improved, and further, the curvature radius of the spherical element can be efficiently, quickly and conveniently detected;
the realization method of the fourth step is that,
by using the conversion relation shown in the following formula, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n ；
Wherein R is 0 For calibrating sample plate S 0 Radius of curvature R of (2) n For the radius of curvature of the sample to be measured, Δz n Represents the sphere center O of the calibration sample plate 0 And the sphere center O of the tested sample n Axial offset between D F The clamping diameter of the supporting clamp is the clamping diameter; the advantage of differential confocal high-precision measurement is reserved, and the measurement efficiency is remarkably improved.
2. The post-spectral pupil differential confocal radius of curvature rapid relative measurement method of claim 1, wherein: a differential confocal curve is obtained by adopting a post-spectroscopic pupil differential confocal detection technology, and the measuring light reflected by the measured element passes through a D-shaped diaphragm and a microscope objective lens to be imaged on a CCD detection surface; according to the detected elliptic light spots, symmetrically arranging virtual pinhole front focus vph1 and rear focus vph2 on two confocal sides of a circular detection area, namely a virtual pinhole, at the optical axis position; taking gray value integral in the virtual pinholes as detection light intensity, and obtaining a differential confocal response curve by detecting axial light intensity responses of the two virtual pinholes and performing differential processing, wherein the differential light intensity value I of a measured piece is obtained diff (Δz n ) Expressed as:
I diff (Δz n )＝I vph2 (Δz n )-I vph1 (Δz n )
wherein I is vph1 (Δz n ) Represented as the intensity value, I, at the virtual pinhole front focal vph1 vph2 (Δz n ) Is the light intensity value at the virtual pinhole front focal vph2; and obtaining a fitting straight line with a high slope and a long linear range through linear fitting, so as to ensure the curvature radius measurement precision and the measurement range.
3. The post-spectral pupil differential confocal radius of curvature rapid relative measurement method of claim 1, wherein: setting I by threshold value ts Judging whether the defocus amount is in a linear response interval; template S 0 Light intensity response I of virtual pinhole obtained by scanning vph1 、I vph2 Summing to obtain light intensity response sum I sum ：
I sum ＝I vph1 +I vph2
Wherein I is vph1 Represented as the intensity value, I, at the virtual pinhole front focal vph1 vph2 Is the light intensity value at the virtual pinhole front focal vph2;
as the tested piece S n Collected single point light intensity response sum I sumn >I ts Determining that the differential light intensity value is atIn the linear response interval, namely the measured piece does not exceed the measuring range, the next measurement can be carried out; as the tested piece S n Collected single point light intensity response sum I sumn <I ts When the differential light intensity value is out of the linear response interval, namely the measured piece is out of range, the information that the measured piece cannot be measured is returned at the moment; thus according to I sum Whether or not it is greater than I ts So as to realize the judgment of the over-range.
4. The post-spectral pupil differential confocal radius of curvature rapid relative measurement method of claim 1, wherein: the vertical annular clamping structure is adopted to ensure that the sample plate and each tested piece can be rapidly and stably clamped by means of self gravity, and ensure that the weft corresponding to the same sagittal height on the spherical surface can be repeatedly positioned at the same space position after the spherical surface elements of the same batch are clamped; for concave sphere measurement, the outer circle of the ring fixture is contacted with the measured sphere; for convex sphere measurements, the inner circle of the ring fixture is in contact with the sphere being measured.
5. The post-spectral pupil differential confocal radius of curvature rapid relative measurement method of claim 1, 2, 3 or 4, characterized by: the realization method of the fourth step is that,
by using the conversion relation shown in the following formula, the curvature radius R of the template is calibrated 0 And defocus amount Δz n Calculating the radius of curvature R n The advantages of differential confocal high-precision measurement can be reserved, the measurement efficiency can be remarkably improved, and further, the curvature radius of the spherical element can be efficiently, quickly and conveniently detected;
wherein R is 0 For calibrating sample plate S 0 Radius of curvature R of (2) n For the radius of curvature of the sample to be measured, Δz n Represents the sphere center O of the calibration sample plate 0 And the sphere center O of the tested sample n Axial offset between D F Clamping for supporting clampDiameter.
6. The device for quickly and relatively measuring the differential confocal curvature radius of the rear-mounted split pupil is characterized in that: the system comprises a rear split pupil differential confocal module, a motion control and monitoring module and an attitude adjustment module; the rear-mounted split pupil differential confocal module uses a D-shaped diaphragm to set a light spot on a CCD detection surface as a virtual pinhole position, and performs differential processing on axial light intensity response of the light spot to realize accurate focusing of a detected element; the rear split pupil differential confocal module comprises a point light source, a collimating mirror, a reflecting mirror, a converging mirror, a D-shaped diaphragm, a microscope objective and a photoelectric detector CCD;
the motion control module drives the screw rod by using the servo motor to drive the high-precision air floatation guide sleeve to move along the optical axis direction, and simultaneously monitors the position information in real time by using the grating ruler to finish scanning and position data acquisition; the motion control module comprises a servo motor, a screw rod, a high-precision air floatation guide sleeve, a high-precision air floatation guide rail and a grating ruler; the gesture adjusting module uses a two-dimensional adjusting frame to adjust the spatial positions of the standard converging mirror and the measured mirror, so that the center of the gesture adjusting module coincides with the optical axis, and the absolute measuring process of the curvature radius is converted into the relative measurement based on a template; the gesture adjusting process utilizes an annular clamp to quickly and accurately position the measured piece at the confocal position of the template; the gesture adjusting module comprises a two-dimensional adjusting frame and an annular clamp.
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