CN106768892A - Free surface lens corrugated joining method based on Hartmann shark wavefront sensor - Google Patents
Free surface lens corrugated joining method based on Hartmann shark wavefront sensor Download PDFInfo
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/02—Testing optical properties
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J9/00—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J9/00—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength
- G01J2009/002—Wavefront phase distribution
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Abstract
The invention discloses a kind of free surface lens corrugated joining method based on Hartmann shark wavefront sensor.The present invention obtains the W of full wafer free surface lens using Hartmann shark wavefront sensor measurement1Region, obtains W1First five term coefficient of region wavefront zernike polynomial, then move a certain distance measurement W2Region, obtains W2First five term coefficient of region wavefront zernike polynomial.Selection W1、W2Three points of overlapping region, by W1、W2The wave front aberration in region is showed with zernike polynomial, and solution obtains splicing parameter, and the Ze Nike expansions that the splicing parameter is substituted into Wave-front phase can be by W1、W2The wave front aberration in region shows.The present invention is realized the method spliced using wavefront and obtains the function of full wafer free surface lens wave front aberration, with measurement is quick, simple operation and other advantages.
Description
Technical field
It is freely bent more particularly to based on Shack-Hartmann wavefront sensor the present invention relates to corrugated splicing field
Face eyeglass corrugated joining method.
Background technology
With the development of free form surface technology, using Free-Form Surface Machining technology free surface lens application increasingly
Extensively, progressive multi-focus lens occupy critical role as the representative of free surface lens in high-end ophthalmic lens market.At present, in Europe
Mei Deng developed countries, progressive lenses have occupied larger market ratio, and the sales volume of Japanese market progressive lenses accounts for glasses
The 21% of market, American market this ratio also reaches 60%.
Detection for conventional lenses is ripe already at present, but is directed to the detection of free surface lens, at present in the world
Corresponding unified standard is not reached, the industry development to free surface lens produces high resistance.Now, commented with wave front aberration
The method of valency free surface lens increasingly attracts attention, but for fear of the instrument Shack-Hartmann wavefront biography of measuring wavefront aberrations
Sensor measurement size limitation, it is difficult to realize the measurement to full wafer eyeglass wave front aberration.
The content of the invention
In order to solve the above problems, the invention provides the free surface lens based on Shack-Hartmann wavefront sensor
Corrugated joining method.
The present invention is comprised the following steps:
Step one:The W of full wafer free surface lens is obtained using Shack-Hartmann wavefront sensor measurement1Region, obtains
W1First five term coefficient of region wavefront zernike polynomial, then move a certain distance measurement W2Region, obtains W2Region wavefront pool
Polynomial first five term coefficient of Buddhist nun gram;Overlap region in point, the zernike polynomial for measuring twice in theory first five
Term coefficient should be equal, but due to the presence of measurement error, measurement result can not possibly be essentially equal.
The conventional Ze Nike expansions of Wave-front phase are:
First five items expansion is:
With W1The phase distribution in regionOn the basis of, mobile distance is x0、y0, W2The phase distribution in region isHad using Shack Hartmann wave front sensor measurement:
(2) to x, derivation is obtained y formula respectively:
Step 2:Selection W1、W2Three point (x of overlapping region1,y1)、(x2,y2)、(x3,y3), W1Three points in region
Correspondence x, the wavefront slope in y-axis is respectively (c1,d1)、(c2,d2)、(c3,d3), W2Three points correspondence x in region, in y-axis
Wavefront slope difference (c '1,d1)、(c’2,d2)、(c’3,d3).By W1、W2The wave front aberration in region is represented with zernike polynomial
Out, have (3) formula is write as matrix form:
There can be unique solution (a for above formula (4)1、a2、a3、a4、a5), it is splicing parameter, the splicing parameter is substituted into (1)
Formula can be by W1、W2The wave front aberration in region shows.
Step 3:For W1、W2N point (x of overlapping region1,y1)…(xn,yn) have:
The form for being expressed as residual error is:
During equal precision measurement, the minimum matrix form of residual error quadratic sum is:
Wherein:
During equal precision measurement, the normal equation of matrix form is:
The solution of normal equation, the matrix expression of first five term coefficient of zernike polynomial are obtained according to (6) formula:
Then, W1Region, W2The wave front aberration in region is:
Repeat step one, step 2, you can realize the corrugated splicing to full wafer free surface lens, obtain full wafer freely bent
The expression formula of the zernike polynomial of face eyeglass Wave-front phase.
The beneficial effects of the present invention are:Free surface lens corrugated splicing based on Shack-Hartmann wavefront sensor
Method, compared to existing technology, the present invention solves the measurement size of limited existing Shack-Hartmann wavefront sensor, it is impossible to real
Now to problems such as the measurements of full wafer free surface lens wave front aberration, realize the method spliced using wavefront and obtain full wafer freedom
The function of curve lens wave front aberration, with measurement is quick, simple operation and other advantages.
Brief description of the drawings
The present invention is further described with reference to the accompanying drawings and examples.
Fig. 1 is adjacent sub-aperture W of the invention1、W2Splicing detects schematic diagram;
Specific embodiment
In order that technological means, creation characteristic, reached purpose and effect that the present invention is realized are easy to understand, tie below
Conjunction is specifically illustrating, and the present invention is expanded on further.It should be noted that in the case where not conflicting, embodiment in the application and
Feature in embodiment can be combined with each other.
As shown in figure 1, the free surface lens corrugated joining method based on Shack-Hartmann wavefront sensor, including with
Lower step:
Step one:Obtain measuring the W of full wafer free surface lens using Shack-Hartmann wavefront sensor measurement1Region,
Obtain W1First five term coefficient of region wavefront zernike polynomial, then move a certain distance measurement W2Region, obtains W2Region ripple
First five term coefficient of preceding zernike polynomial;Point in the region for overlapping, the zernike polynomial for measuring twice in theory
First five term coefficient should be equal, but due to the presence of measurement error, measurement result can not possibly be essentially equal.
The conventional Ze Nike expansions of Wave-front phase are:
First five items expansion is:
With W1The phase distribution in regionOn the basis of, mobile distance is x0、y0, W2The phase distribution in region isHad using Shack Hartmann wave front sensor measurement:
(2) to x, derivation is obtained y formula respectively:
Step 2:Selection W1、W2Three point (x of overlapping region1,y1)、(x2,y2)、(x3,y3), W1Three points in region
Correspondence x, the wavefront slope in y-axis is respectively (c1,d1)、(c2,d2)、(c3,d3), W2Three points correspondence x in region, in y-axis
Wavefront slope difference (c '1,d1)、(c’2,d2)、(c’3,d3).By W1、W2The wave front aberration in region is represented with zernike polynomial
Out, have (3) formula is write as matrix form:
There can be unique solution (a for above formula (4)1、a2、a3、a4、a5), it is splicing parameter, the splicing parameter is substituted into (1)
Formula can be by W1、W2The wave front aberration in region shows.
Step 3:For W1、W2N point (x of overlapping region1,y1)…(xn,yn) have:
The form for being expressed as residual error is:
During equal precision measurement, the minimum matrix form of residual error quadratic sum is:
Wherein:
During equal precision measurement, the normal equation of matrix form is:
The solution of normal equation, the matrix expression of first five term coefficient of zernike polynomial are obtained according to (6) formula:
Then, W1Region, W2The wave front aberration in region is:
Repeat step one, step 2, you can realize the corrugated splicing to full wafer free surface lens, obtain full wafer freely bent
The expression formula of the zernike polynomial of face eyeglass Wave-front phase, i.e. sensor survey the wave front aberration for once obtaining a fritter, pass through
Splicing obtains the wave front aberration of whole eyeglass.
Claims (1)
1. the free surface lens corrugated joining method of Shack-Hartmann wavefront sensor is based on, it is characterised in that the method bag
Include following steps:
Step one:The W of full wafer free surface lens is obtained using Shack-Hartmann wavefront sensor measurement1Region, obtains W1Area
First five term coefficient of domain wavefront zernike polynomial, then move a certain distance measurement W2Region, obtains W2Region wavefront Ze Nike
Polynomial first five term coefficient;Point in the region for overlapping, first five term system for the zernike polynomial for measuring twice in theory
Number should be equal, but due to the presence of measurement error, measurement result can not possibly be essentially equal;
The conventional Ze Nike expansions of Wave-front phase are:
First five items expansion is:
With W1The phase distribution in regionOn the basis of, mobile distance is x0、y0, W2The phase distribution in region isHad using Shack Hartmann wave front sensor measurement:
(2) to x, derivation is obtained y formula respectively:
Step 2:Selection W1、W2Three point (x of overlapping region1,y1)、(x2,y2)、(x2,y3), W1Three points correspondence in region
X, the wavefront slope in y-axis is respectively (c1,d1)、(c2,d2)、(c3,d3), W2Three points correspondence x in region, the ripple in y-axis
Front slope distinguishes (c '1,d1)、(c’2,d2)、(c’3,d3);By W1、W2The wave front aberration in region is represented with zernike polynomial
Come, have (3) formula is write as matrix form:
There is unique solution (a for above formula (4)1、a2、a3、a4、a5), it is splicing parameter, the splicing parameter is substituted into (1) formula can
W1、W2The wave front aberration in region shows;
Step 3:For W1、W2N point (x of overlapping region1,y1)…(xn,yn) have:
The form for being expressed as residual error is:
During equal precision measurement, the minimum matrix form of residual error quadratic sum is:
Wherein:
During equal precision measurement, the normal equation of matrix form is:
The solution of normal equation, the matrix expression of first five term coefficient of zernike polynomial are obtained according to (6) formula:
Then, W1Region, W2The wave front aberration in region is:
Repeat step one, step 2, you can realize the corrugated splicing to full wafer free surface lens.
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Cited By (4)
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CN107560564A (en) * | 2017-07-28 | 2018-01-09 | 中国计量大学 | A kind of free form surface detection method and system |
CN107966280A (en) * | 2017-11-21 | 2018-04-27 | 华东交通大学 | A kind of photodetector system applied to spliced telescope and its quick common phase adjusting method |
CN108827596A (en) * | 2018-04-03 | 2018-11-16 | 华东交通大学 | One kind being applied to the novel common phase detection method of sectional type spliced telescope and device |
CN111238664A (en) * | 2020-02-24 | 2020-06-05 | 中国科学院云南天文台 | Hartmann shack wavefront detection method based on region detection and reconstruction |
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Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107560564A (en) * | 2017-07-28 | 2018-01-09 | 中国计量大学 | A kind of free form surface detection method and system |
CN107560564B (en) * | 2017-07-28 | 2019-09-10 | 中国计量大学 | A kind of free form surface detection method and system |
CN107966280A (en) * | 2017-11-21 | 2018-04-27 | 华东交通大学 | A kind of photodetector system applied to spliced telescope and its quick common phase adjusting method |
CN107966280B (en) * | 2017-11-21 | 2021-07-06 | 华东交通大学 | Photoelectric detection system applied to spliced telescope and rapid common-phase adjustment method thereof |
CN108827596A (en) * | 2018-04-03 | 2018-11-16 | 华东交通大学 | One kind being applied to the novel common phase detection method of sectional type spliced telescope and device |
CN108827596B (en) * | 2018-04-03 | 2021-06-29 | 华东交通大学 | Common-phase detection method and device applied to segmented splicing telescope |
CN111238664A (en) * | 2020-02-24 | 2020-06-05 | 中国科学院云南天文台 | Hartmann shack wavefront detection method based on region detection and reconstruction |
CN111238664B (en) * | 2020-02-24 | 2021-03-30 | 中国科学院云南天文台 | Hartmann shack wavefront detection method based on region detection and reconstruction |
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