CN110081988A - A method of space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes - Google Patents
A method of space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes Download PDFInfo
- Publication number
- CN110081988A CN110081988A CN201910274361.8A CN201910274361A CN110081988A CN 110081988 A CN110081988 A CN 110081988A CN 201910274361 A CN201910274361 A CN 201910274361A CN 110081988 A CN110081988 A CN 110081988A
- Authority
- CN
- China
- Prior art keywords
- light
- phase
- lateral shear
- wavefront
- wave
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000000034 method Methods 0.000 title claims abstract description 33
- 230000010363 phase shift Effects 0.000 title claims abstract description 19
- 230000003287 optical effect Effects 0.000 claims abstract description 15
- 238000003384 imaging method Methods 0.000 claims description 6
- 230000001427 coherent effect Effects 0.000 claims description 4
- 239000012141 concentrate Substances 0.000 claims description 4
- 238000006073 displacement reaction Methods 0.000 claims description 3
- 238000010008 shearing Methods 0.000 claims description 3
- 238000005259 measurement Methods 0.000 abstract description 10
- 238000001514 detection method Methods 0.000 abstract description 2
- 230000000694 effects Effects 0.000 abstract description 2
- 238000001228 spectrum Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000000284 extract Substances 0.000 description 2
- 230000004075 alteration Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
Classifications
-
- 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
- G01J9/02—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength by interferometric methods
- G01J9/0215—Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength by interferometric methods by shearing interferometric methods
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
The present invention relates to a kind of methods that space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes, belong to field of optical detection.Space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes by this method, finally to realize unified, high-precision dynamic wavefront measurement.Especially by the relationship between control screen periods and image sensor pixel size, to control the phase-shift phase between carrier fringe adjacent pixel, and the suitable phase shift algorithm of final choice realizes the demodulation of wavefront slope.Fast Fourier Transform (FFT) method (Fast Fourier Transform is utilized compared to traditional four wave lateral shear interferometers, FFT wavefront slope) is demodulated, this method calculating process is simple, high-precision unified dynamic wavefront measurement may be implemented in the interrupted spectra being related to there is no FFT method and edge effect.
Description
Technical field
The invention belongs to the manufacture of advanced optics and detection fields, and in particular to a kind of that space carrier frequency phase shift algorithm is used for four
The method of wave lateral shear interferometer wavefront slope demodulation.
Background technique
Interferometer be using the wavelength of light as a kind of high-precision of measurement unit, highly sensitive metrology and measurement instrument, it
It is widely used in optical measurement.Interference fringe is the track of the identical point of optical path difference in interferometer interference field, according to interference
Shape, movement, density degree of striped etc. can demodulate to obtain the optical path difference information of tested light.
Four wave lateral shear interferometers are a kind of grating types by propositions such as French scientist Jerome Primo in 2000
Lateral shear interferometer.Light is tested through optical grating diffraction, 90% or more diffraction light energy concentrates on four beam first-order diffraction light.This four
Beam first-order diffraction light is along respective diffraction angular direction onwards transmission, and finally mutual dislocation and coherent superposition on the viewing screen, form
Interference fringe.By handling interference fringe, demodulation obtains fringe phase, can acquire the wavefront slope of tested light, most
Optical path difference information is obtained using restoration algorithm afterwards.
Currently from there are mainly three types of the methods of interference fringe demodulation phase, respectively the Schlieren method, FFT (Fast Fourier
Transform) method and phase-shifting method, the wherein precision highest of phase-shifting method, but its interference for needing to acquire several different phase-shift phases
Figure, it is more sensitive to extraneous ambient vibration;The Schlieren method and FFT method only need a width interference pattern, influenced by ambient vibration it is smaller,
It can be used for dynamically measuring, but processing accuracy is lower.In consideration of it, nineteen ninety Shough et al. proposes space carrier frequency phase shift
(Spatial-carrier phase shifting SCPS) method, specific method are the angles by controlling two interfering beams
The carrier phase amount for obtaining neighbor pixel is equal to the interference pattern of pi/2, and assumes phase phase of several consecutive points on tested surface
Together, then adjacent several pixels can substitute the pixel obtained in time domain by phase shifter phase shift in space, so
Phase can be calculated by phase shift formula afterwards.Although space carrier frequency phase shift method only handles single width interference pattern, its processing result
The processing accuracy that phase-shifting method can be reached approximately, in combination with FFT method dynamic measurement and the high-precision advantage of phase-shifting method.
The method of four traditional wave lateral shear interferometer demodulated interferential fringe phases is FFT method, but due to side in FFT method
The influence of the factors such as edge effect, interrupted spectra and spectral resolution limitation, causes its algorithm operation quantity larger and processing result precision
It is affected.
Space carrier frequency phase shifting method is used for four wave lateral shear interferometers by the present invention, passes through control screen periods and image
Relationship between sensor pixel size controls the phase-shift phase between carrier fringe neighbor pixel, is realized using phase shift algorithm
Interference fringe phase, that is, wavefront slope high-precision is restored, final to realize the measurement of optical path difference Dynamic High-accuracy.
Summary of the invention
The purpose of the present invention is space carrier frequency phase shift method is used for four wave lateral shear interferometer interference fringe phases, i.e. quilt
The Dynamic High-accuracy measurement of optical path difference is realized in the demodulation for surveying light wave front slope.This method passes through control screen periods and figure first
As the relationship between sensor pixel size, so that the carrier phase amount between adjacent pixel is pi/2, phase shift algorithm is then utilized
Solution obtains the wavefront slope of four direction.
The technical solution adopted by the present invention is that: it is a kind of that space carrier frequency phase shift algorithm is used for four wave lateral shear interferometer waves
The method of front slope demodulation, comprising:
Step 1: four wave lateral shear interferometer systems of building, comprising:
Two-dimentional complex amplitude grating, for generating four beam first-order diffraction light, the two dimension complex amplitude grating is by amplitude grating and phase
Position grating be formed by stacking, the amplitude grating period be p × p, light hole having a size ofPhase grating is by 0 phase and π phase
It is alternately arranged, the period is 2p × 2p;
Imaging sensor, for acquiring interference fringe, Pixel Dimensions
Tested light is incident on two-dimentional complex amplitude grating, and through optical grating diffraction, most diffraction light energies concentrate on four beams one
Grade diffraction light, this four beams diffraction light form interference fringe, utilize image in position of image sensor mutual dislocation and coherent superposition
The interference fringe of sensor acquisition, i.e., the resilient optical path difference information for obtaining tested light;Change screen periods or selection is suitable
Imaging sensor so that the carrier phase amount of interference fringe neighbor pixel be pi/2;
Step 2: the light intensity expression of four wave lateral shear interferometers are as follows:
Wherein I (x, y) is interference fringe light intensity, and a (x, y) is interference fringe background light intensity, and b (x, y) is modulation degree, s x
The shearing displacement in direction or the direction y, k are wave number, and p is the amplitude grating period;
When assuming that when the corresponding background light intensity of 10 adjacent position points, modulation degree and identical tested light phase, solution point
The formula of wavefront slope is as follows at (m, n):
Wherein, I0=I (m, n), I1=I (m-1, n), I2=I (m+1, n), I3=I (m, n-1), I4=I (m, n+1), I5
=I (m-1, n+1), I6=I (m+1, n-1), I7=I (m-1, n-1), I8=I (m+1, n+1), I9=I (m-2, n-2);
Wherein, W is tan before tested light wave-1For arctan function;
The wavefront slope of four direction is found out using formula (2)-(5), final restore obtains tested light optical path difference information.
The advantages of the present invention over the prior art are that:
(1) operation of the present invention is simple, and operand is low, can accelerate to restore speed, realize optical path difference transient measurement.
(2) marginal error of the present invention is small, and recovery accuracy is high, can almost realize unified measurement.
Detailed description of the invention
Fig. 1 is four wave lateral shear interferometer system schematics;
Fig. 2 is four wave lateral shear interferometer two dimension complex amplitude grating schematic diagrams;
Fig. 3 is the light intensity position that wavefront slope needs to use at solution point (m, n);
Fig. 4 is tested wavefront distribution schematic diagram;
Fig. 5 is the wavefront slope in the direction x extracted using the present invention;
Fig. 6 is the wavefront slope in the direction y extracted using the present invention;
Fig. 7 is the wavefront slope in the direction x+y extracted using the present invention;
Fig. 8 is the wavefront slope in the direction x-y extracted using the present invention;
Fig. 9 is that the wavefront restored using the wavefront slope that the present invention extracts is distributed.
Specific embodiment
With reference to the accompanying drawing and specific embodiment further illustrates the present invention.
A kind of method that space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes of the present invention,
If Fig. 1 show four wave lateral shear interferometer system schematics, tested light is incident on two-dimentional complex amplitude grating, spreads out through grating
It penetrates, most diffraction light energies concentrate on four beam first-order diffraction light, this four beams diffraction light is mutually wrong in position of image sensor
Position and coherent superposition form interference fringe.The interference fringe acquired using imaging sensor, i.e., the resilient light for obtaining tested light
Path difference information.
Two-dimentional complex amplitude grating (as shown in Figure 2), for generating four beam first-order diffraction light.The grating is by amplitude grating and phase
Position grating be formed by stacking, the amplitude grating period be p × p, light hole having a size ofPhase grating is by 0 phase and π phase
It is alternately arranged, the period is 2p × 2p;
Imaging sensor, for acquiring interference fringe, Pixel Dimensions
The light intensity expression of four wave lateral shear interferometers are as follows:
Wherein I (x, y) is interference fringe light intensity, and a (x, y) is interference fringe background light intensity, and b (x, y) is modulation degree, s x
The shearing displacement in direction or the direction y, k are wave number, and p is the amplitude grating period.
When assuming that the corresponding background light intensity of 10 adjacent position points shown in Fig. 3, modulation degree and tested light phase are identical
When, the formula of wavefront slope is as follows at solution point (m, n):
As shown in figure 3, I0=I (m, n), I1=I (m-1, n), I2=I (m+1, n), I3=I (m, n-1), I4=I (m, n+
1), I5=I (m-1, n+1), I6=I (m+1, n-1), I7=I (m-1, n-1), I8=I (m+1, n+1), I9=I (m-2, n-2).
Wherein W is tan before tested light wave-1For arctan function.
Shown in the light intensity expression of four wave lateral shear interferometer interference fringes such as claim 2 Chinese style (1), wherein striped is carried on the back
Scape light intensity a (x, y), the wavefront slope of modulation degree b (x, y) and four direction It is unknown.Therefore, in order to solve wavefront slope, six equations are at least needed.
For simplicity, it enables,
Then light intensity expression becomes:
After imaging sensor acquires, the light intensity expression of discretization are as follows:
Wherein m, n are the pixel coordinate in transverse and longitudinal direction, due toThereforeLight
Strongly expressed formula is rewritten are as follows:
In order to acquire the wavefront slope at point (m, n), the light intensity using as shown in Figure 3 ten consecutive points is needed, and assume
Their corresponding background light intensity, modulation degree and phase are identical, that is, assume:
Similarly, it is assumed that a (x, y), b (x, y),Respectively in this ten consecutive points
It is worth identical.
As shown in figure 3, this corresponding light intensity expression of ten points is respectively as follows:
Therefore,
According to formula (6), then shown in the solution formula of wavefront slope such as formula (2)~(5).
When wavefront to be measured is defocus aberration shown in (such as Fig. 4), with the direction x acquired of the present invention, the direction y, the direction x+y and
Respectively as shown in figures 5-8, the wavefront restored is as shown in Figure 9 for the wavefront slope in the direction x-y.As can be seen that the present invention proposes
Method can accurately extract the wavefront slopes of four wave lateral shear interferometers, and finally realize that the high-precision of wavefront is restored.
Claims (1)
1. a kind of method that space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes, feature exist
In, comprising:
Step 1: four wave lateral shear interferometer systems of building, comprising:
Two-dimentional complex amplitude grating, for generating four beam first-order diffraction light, the two dimension complex amplitude grating is by amplitude grating and phase light
Grid are formed by stacking, the amplitude grating period be p × p, light hole having a size ofPhase grating is by 0 phase and π phase alternation
It arranges, the period is 2p × 2p;
Imaging sensor, for acquiring interference fringe, Pixel Dimensions
Tested light is incident on two-dimentional complex amplitude grating, and through optical grating diffraction, most diffraction light energies concentrate on four beam level-ones and spread out
Light is penetrated, this four beams diffraction light forms interference fringe, utilize image sensing in position of image sensor mutual dislocation and coherent superposition
The interference fringe of device acquisition, i.e., the resilient optical path difference information for obtaining tested light;Change screen periods or the suitable figure of selection
As sensor, so that the carrier phase amount of interference fringe neighbor pixel is pi/2;
Step 2: the light intensity expression of four wave lateral shear interferometers are as follows:
Wherein I (x, y) is interference fringe light intensity, and a (x, y) is interference fringe background light intensity, and b (x, y) is modulation degree, and s is the direction x
Or the shearing displacement in the direction y, k are wave number, p is the amplitude grating period;
When assuming that when the corresponding background light intensity of 10 adjacent position points, modulation degree and identical tested light phase, solution point (m, n)
The formula for locating wavefront slope is as follows:
Wherein, I0=I (m, n), I1=I (m-1, n), I2=I (m+1, n), I3=I (m, n-1), I4=I (m, n+1), I5=I
(m-1, n+1), I6=I (m+1, n-1), I7=I (m-1, n-1), I8=I (m+1, n+1), I9=I (m-2, n-2);
Wherein, W is tan before tested light wave-1For arctan function;
The wavefront slope of four direction is found out using formula (2)-(5), final restore obtains tested light optical path difference information.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910274361.8A CN110081988B (en) | 2019-04-08 | 2019-04-08 | Method for applying spatial carrier frequency phase shift algorithm to wavefront slope demodulation of four-wave lateral shearing interferometer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910274361.8A CN110081988B (en) | 2019-04-08 | 2019-04-08 | Method for applying spatial carrier frequency phase shift algorithm to wavefront slope demodulation of four-wave lateral shearing interferometer |
Publications (2)
Publication Number | Publication Date |
---|---|
CN110081988A true CN110081988A (en) | 2019-08-02 |
CN110081988B CN110081988B (en) | 2021-09-21 |
Family
ID=67414384
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201910274361.8A Active CN110081988B (en) | 2019-04-08 | 2019-04-08 | Method for applying spatial carrier frequency phase shift algorithm to wavefront slope demodulation of four-wave lateral shearing interferometer |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN110081988B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111772574A (en) * | 2020-06-06 | 2020-10-16 | 宁波明星科技发展有限公司 | Method and device for eliminating defocusing during wavefront aberration measurement |
CN114137713A (en) * | 2021-11-17 | 2022-03-04 | 华中科技大学 | Real-time quantitative phase imaging method and system for unmarked thick sample |
Citations (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4692027A (en) * | 1985-07-03 | 1987-09-08 | Itek Corporation | Spatial processing for single or dual shear wavefront sensor |
US20090009751A1 (en) * | 2007-03-08 | 2009-01-08 | Yukio Taniguchi | Aberration measurement apparatus and aberration measurement method |
CN101451890A (en) * | 2008-12-18 | 2009-06-10 | 南京大学 | Three light wave transversal shearing interference apparatus and method for extracting differential phase |
US20110134438A1 (en) * | 2009-12-07 | 2011-06-09 | Canon Kabushiki Kaisha | Refractive index distribution measuring method and refractive index distribution measuring apparatus |
CN102252765A (en) * | 2011-06-24 | 2011-11-23 | 北京理工大学 | Wavefront aberration detection device and method for beam expansion and collimation system |
CN102681365A (en) * | 2012-05-18 | 2012-09-19 | 中国科学院光电技术研究所 | Projection objective wave aberration detection device and method |
CN102914374A (en) * | 2011-08-03 | 2013-02-06 | 佳能株式会社 | Wavefront measuring apparatus and wavefront measuring method |
CN102967378A (en) * | 2012-12-09 | 2013-03-13 | 中国科学院光电技术研究所 | Miniaturized radial shearing interferometer based on four-step phase-shifting principle |
CN103134439A (en) * | 2013-01-29 | 2013-06-05 | 天津大学 | Double-rotation optical wedge space phase shift method used for cutting speckle interference |
CN104155011A (en) * | 2014-07-22 | 2014-11-19 | 北京理工大学 | Phase extracting method for two-dimension interferogram |
CN204028565U (en) * | 2014-08-26 | 2014-12-17 | 中国科学院上海光学精密机械研究所 | A kind of projection objective wave aberration on-line checkingi interferometer |
CN104655291A (en) * | 2015-03-16 | 2015-05-27 | 中国科学院光电技术研究所 | Method for realizing programmable multi-wave lateral shearing interferometer |
CN107063477A (en) * | 2017-03-16 | 2017-08-18 | 中国科学院上海光学精密机械研究所 | Grating lateral shearing interference large-numerical aperture wave-front reconstruction method |
CN109163816A (en) * | 2018-08-28 | 2019-01-08 | 中国科学院光电技术研究所 | Radial shearing interferometer based on cosine wave band sheet |
-
2019
- 2019-04-08 CN CN201910274361.8A patent/CN110081988B/en active Active
Patent Citations (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4692027A (en) * | 1985-07-03 | 1987-09-08 | Itek Corporation | Spatial processing for single or dual shear wavefront sensor |
US20090009751A1 (en) * | 2007-03-08 | 2009-01-08 | Yukio Taniguchi | Aberration measurement apparatus and aberration measurement method |
CN101451890A (en) * | 2008-12-18 | 2009-06-10 | 南京大学 | Three light wave transversal shearing interference apparatus and method for extracting differential phase |
US20110134438A1 (en) * | 2009-12-07 | 2011-06-09 | Canon Kabushiki Kaisha | Refractive index distribution measuring method and refractive index distribution measuring apparatus |
CN102252765A (en) * | 2011-06-24 | 2011-11-23 | 北京理工大学 | Wavefront aberration detection device and method for beam expansion and collimation system |
CN102914374A (en) * | 2011-08-03 | 2013-02-06 | 佳能株式会社 | Wavefront measuring apparatus and wavefront measuring method |
CN102681365A (en) * | 2012-05-18 | 2012-09-19 | 中国科学院光电技术研究所 | Projection objective wave aberration detection device and method |
CN102967378A (en) * | 2012-12-09 | 2013-03-13 | 中国科学院光电技术研究所 | Miniaturized radial shearing interferometer based on four-step phase-shifting principle |
CN103134439A (en) * | 2013-01-29 | 2013-06-05 | 天津大学 | Double-rotation optical wedge space phase shift method used for cutting speckle interference |
CN104155011A (en) * | 2014-07-22 | 2014-11-19 | 北京理工大学 | Phase extracting method for two-dimension interferogram |
CN204028565U (en) * | 2014-08-26 | 2014-12-17 | 中国科学院上海光学精密机械研究所 | A kind of projection objective wave aberration on-line checkingi interferometer |
CN104655291A (en) * | 2015-03-16 | 2015-05-27 | 中国科学院光电技术研究所 | Method for realizing programmable multi-wave lateral shearing interferometer |
CN107063477A (en) * | 2017-03-16 | 2017-08-18 | 中国科学院上海光学精密机械研究所 | Grating lateral shearing interference large-numerical aperture wave-front reconstruction method |
CN109163816A (en) * | 2018-08-28 | 2019-01-08 | 中国科学院光电技术研究所 | Radial shearing interferometer based on cosine wave band sheet |
Non-Patent Citations (1)
Title |
---|
陈小君: "近场光强分布对四波横向剪切干涉仪波前复原的影响研究", 《中国博士学位论文全文数据库工程科技辑》 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111772574A (en) * | 2020-06-06 | 2020-10-16 | 宁波明星科技发展有限公司 | Method and device for eliminating defocusing during wavefront aberration measurement |
CN111772574B (en) * | 2020-06-06 | 2023-06-27 | 宁波明星科技发展有限公司 | Method and device for eliminating defocus during wavefront aberration measurement |
CN114137713A (en) * | 2021-11-17 | 2022-03-04 | 华中科技大学 | Real-time quantitative phase imaging method and system for unmarked thick sample |
Also Published As
Publication number | Publication date |
---|---|
CN110081988B (en) | 2021-09-21 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Leendertz | Interferometric displacement measurement on scattering surfaces utilizing speckle effect | |
Judge et al. | Holographic deformation measurements by Fourier transform technique with automatic phase unwrapping | |
CN101769722B (en) | Method for heterodyne temporal series speckle interferometry of object deformation | |
US20190011247A1 (en) | Method for Phase Resolved Heterodyne Shearographic Measurements | |
CN101915559B (en) | Method and system thereof for measuring three-dimensional surface shape of object by electronic speckle phase shift technology | |
CN103091676A (en) | Mining area surface subsidence synthetic aperture radar interferometry monitoring and calculating method | |
CN102221342A (en) | Method for measuring object deformation by time-domain multi-wavelength heterodyne speckle interference | |
CN104482877A (en) | Motion compensation method and system in three-dimensional imaging of dynamic object | |
CN110081988A (en) | A method of space carrier frequency phase shift algorithm is used for the demodulation of four wave lateral shear interferometer wavefront slopes | |
CN104034277A (en) | Measuring method for phase of dual-wavelength micro-nano structure | |
CN102914256A (en) | Synchronous phase shifting interference detection device based on orthogonal double grating and detection method | |
CN109059787A (en) | A kind of sheet thickness distribution measurement method and system based on lateral shearing interference | |
CN105698702B (en) | A kind of diplopore heterodyne ineterferometer based on acousto-optic low frequency differences phase shift | |
Flores et al. | Color deflectometry for phase retrieval using phase-shifting methods | |
CN102865810A (en) | Orthogonal double-grating based detecting device for synchronous phase shift common-light path interference and detecting method therefor | |
CN105300276A (en) | Dual-wavelength single-exposure interference measuring method and system | |
CN111947600B (en) | Robust three-dimensional phase unfolding method based on phase level cost filtering | |
CN103542870B (en) | Ac modulation type low coherence interference demodulating system | |
CN103267485A (en) | Point-diffraction three-dimensional absolute displacement measuring method | |
CN112212806A (en) | Three-dimensional phase unfolding method based on phase information guidance | |
CN106091974A (en) | A kind of object distortion measurement instrument, method and apparatus | |
CN106643474B (en) | A kind of orthonormalization multistep phase-shifting phase measurement method | |
El-Morsy | A novel algorithm based on sub-fringe integration method for direct two-dimensional unwrapping phase reconstruction from the intensity of one-shot two-beam interference fringes | |
CN201724658U (en) | System for measuring three dimensional surface shape of an object by electronic speckle phase shift technology | |
CN102853761A (en) | Space phase shifter |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |