CN106482664A - A kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe - Google Patents

A kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe Download PDF

Info

Publication number
CN106482664A
CN106482664A CN201510523660.2A CN201510523660A CN106482664A CN 106482664 A CN106482664 A CN 106482664A CN 201510523660 A CN201510523660 A CN 201510523660A CN 106482664 A CN106482664 A CN 106482664A
Authority
CN
China
Prior art keywords
wavelength
phase
carrier frequency
phase place
phase shift
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
Application number
CN201510523660.2A
Other languages
Chinese (zh)
Other versions
CN106482664B (en
Inventor
高志山
成金龙
王凯亮
王伟
王帅
袁群
窦建泰
朱丹
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nanjing University of Science and Technology
Original Assignee
Nanjing University of Science and Technology
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Nanjing University of Science and Technology filed Critical Nanjing University of Science and Technology
Priority to CN201510523660.2A priority Critical patent/CN106482664B/en
Publication of CN106482664A publication Critical patent/CN106482664A/en
Application granted granted Critical
Publication of CN106482664B publication Critical patent/CN106482664B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Length Measuring Devices By Optical Means (AREA)
  • Instruments For Measurement Of Length By Optical Means (AREA)

Abstract

The invention discloses a kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe, when detecting aspherical based on Moire fringe is theoretical using dual wavelength interference testing device, the round carrier frequency moiré topography after two kinds of wavelength-interferometric stripe stack can be obtained, it is proposed that a kind of method from circle carrier frequency moiré topography extracting directly synthetic wavelength phase place.By carrying out phase shift with the pi/2 of synthetic wavelength as phase shift stepping-in amount, to after circle carrier frequency Moire fringe phase-shift interference removal DC component square, and adopt secondary polar coordinate transform, obtain line carrier frequency moiré topography, re-construction theory is overlapped in conjunction with carrier frequency, the extraction of the synthetic wavelength component to low frequency being realized in spectrum domain, finally extracting synthetic wavelength phase place, when solving the problems, such as that Single wavelength is detected, striped is overstocked cannot recover phase place.

Description

A kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe
Technical field
The invention belongs to field of optical measuring technologies, particularly a kind of synthesis theoretical based on circle carrier frequency Moire fringe Wavelength phases extracting method.
Background technology
Phase shift interferes detection high have the advantages that high accuracy, contactless and automatic degree, thus in optical element face The aspects such as the test of shape, Performance of Optical System and optical material characteristic have a wide range of applications.Traditional phase shift Interfere detection using the LASER Light Source of single wavelength, its test scope is limited to its operation wavelength, thus in detection During the big graded face shape of aspherical grade its interference fringe can be overstocked and lead to not demodulation phase.
In order to solve the above problems, following methods are generally adopted:First, the resolution ratio for improving detector can make The more intensive interference fringe of resolution, so as to reach the purpose of extension measurement range, but high-resolution detection Device price general charged is expensive, meanwhile, the raising of detector resolution also results in the decline of test speed.Second, Big gradient sphere or aspherical can be measured using zero compensation e measurement technology, but due to tested optical surface and most Deviation between good fitting face is typically unknown, even if being tested using zero compensation, interference pattern is likely to It is difficult to analyze.3rd, survey can also be extended to a certain extent using the interferometer of longer wavelengths of infrared band Amount scope, but the interferometer of infrared band needs optical material and the Infrared Detectors using infrared band, processing Big, the high cost with resetting difficulty.4th, can using sub- Nyquist (Sub-Nyquist) Sample acquisition method To solve the problems, such as to detect that aspherical striped is overstocked using traditional PS I, but as SNI deviates zero-bit interference condition, Can there is larger hysterisis error and special alignment technique is needed, and require to visit using thinned array in SNI Device is surveyed, its design and processing want more conventional detector complicated.5th, using shear interference technology, by measurement Difference corrugated in two vertical direction is recovering original wave-front, it is also possible to realize the measurement of large deviation face shape, though So the measurement apparatus of this method are simple, but follow-up data handling procedure and its numerous and diverse, and precision is relatively low.The Six are detected using sub-aperture stitching, and optical element is divided into some sub-aperture, by mobile interferometer measuration system or Measured piece completes the interferometry to each sub-aperture, obtains a series of corrugated data, then these corrugated data are entered Row fitting splicing, obtains the surface form deviation of whole surface.But tiring out due to stitching error when sub-aperture stitching is detected The kinematic error of product and sub-aperture causes precision low, and detection process needs to carry out each sub-aperture in order Measurement, wastes time and energy, and measurement efficiency is very low.
From 1971 by James. White (J.C.Wyant) exists《Testing aspherics using two-wavelength holography》(APPLIED OPTICS,10(9):Propose in 2113-2118,1971) Since double-wavelength holographic interference measuring technology, on this basis, dual wavelength interference testing technology is developed. Dual wavelength Moire fringe theory refers to that the interference fringe lower to different wave length test is multiplied or linear superposition generation Moiré topography is processed, so as to extract synthetic wavelength phase information.Little open country temple (Onodera) in 1988 Et al.《Two-Wavelength Interferometry That Uses a Fourier-Transform Method》 (APPLIED OPTICS,37(34):7988~7994,1988) propose dry in the phase shift of wavelength tuning dual wavelength The spectrogram of dual wavelength Moire fringe on the basis of interferometer, is obtained using Fourier transformation, is processed and is obtained composite wave Long phase place, but which is confined to the process of line carrier coded fringes, and carrier frequency amount is not high.2003, Zhe Fu (Tetsuo) 《Phase calculation based on curve fitting with a two-wavelength interferometer》 (Optics Express,11(8):895~898,2003) on the basis of analysis dual wavelength Moire fringe light distribution On, it is proposed that time domain dual wavelength Moire fringe light distribution is fitted using curve point by point, its curve representation formula is respectively joined By a series of, number can assume that calculating, iteration are tried to achieve, finally solve and obtain synthetic wavelength phase distribution.Although The algorithm can directly process dual wavelength moire map and obtain synthetic wavelength phase place, but its complex and Process is loaded down with trivial details.2014, peeping for South China Normal University flat (Wangping Zhang) et al. existed 《Simultaneous phase-shifting dual-wavelength interferometry based on two-step demodulation algorithm》(Optics Letters,39(18):5375~5378,2014) in dual wavelength not You are analyzed in striped light distribution, it is proposed that a kind of Moire fringe in figure from online two-wavelength-interferometer is extracted The algorithm of synthetic wavelength phase place, the juche idea of algorithm are to realize the interference to different wave length by setting amount of phase shift The extraction of striped, so as to solve Single wavelength phase place respectively, finally solves and obtains synthetic wavelength phase place, but the algorithm The overstocked situation of Single wavelength striped is not considered.
Content of the invention
It is an object of the invention to provide a kind of synthetic wavelength phase extraction theoretical based on circle carrier frequency Moire fringe Method, while solve Single wavelength to detect that aspherical striped is overstocked and direct each point when processing circle carrier frequency Moire fringe Amount is difficult to detached problem.
The technical solution for realizing the object of the invention is:A kind of composite wave theoretical based on circle carrier frequency Moire fringe Long phase extraction method, method and step are as follows:
The first step:λ is respectively using operation wavelength1And λ2Dual wavelength interference testing device detect aspherical face Shape, wherein λ1≠λ2, two kinds of wavelength are while work, the axial location for adjusting test mirrors introduces round load by out of focus Frequently, the round carrier frequency moiré topography after two kinds of wavelength-interferometric stripe stack is obtained.
Second step:The output voltage of control Phase shifting adapter, realizes with synthetic wavelengthPi/2 Phase shift is carried out for phase shift stepping-in amount, CCD collects the oval load of double wave of one group of 4 frame phase shift stepping-in amount for pi/2 Frequency moire map, its light distribution is:
Wherein, IkFor the oval carrier frequency moire map light distribution of kth frame double wave, A is i.e. DC component,For wavelength X1Modulation degree,For wavelength X1Phase place to be measured, D for circle carrier frequency coefficient, S2For horizontal Pixel coordinate square and longitudinal direction pixel coordinate square sum (i.e. S2=x2+y2, x is horizontal pixel coordinate, y For longitudinal pixel coordinate), δ1,kFor kth frame interference pattern medium wavelength λ1Amount of phase shift,For wavelength X2Modulation Degree,For wavelength X2Phase place to be measured, δ2,kFor kth frame interference pattern medium wavelength λ2Amount of phase shift.
3rd step:The oval carrier frequency moire map of double wave to collecting removes direct current using the method for average and divides After amount, carry out square, the oval carrier frequency moire map light intensity I ' of the double wave after obtaining squarenIt is distributed as:
Wherein, A ' for square after DC component, B1For wavelength X1The coefficient of two harmonics, i.e.,With wavelength X1Downward systemRelevant, B2For wavelength X2The coefficient of two harmonics, i.e.,With wavelength X2Downward systemRelevant, B3For wavelength X1Downward systemWith wavelength X2Under Modulation degreeProduct,For synthetic wavelength phase place, δeq,kDry for kth frame Relate in figure wavelength XeqAmount of phase shift.
4th step:Determine the fringe center for justifying carrier frequency moire map in second step per frame, to above-mentioned More Striped phase-shift interference carries out secondary polar coordinate transform respectively, obtains the load of the dual wavelength line after corresponding Coordinate Conversion Frequency Moire fringe phase-shift interference, its coordinate transform formula is:
Wherein, (ρ, θ) is the point coordinates under polar coordinate system, and (x, y) is cartesian coordinate system corresponding to point (ρ, θ) Under point coordinates, (x0,y0) for the fringe center point coordinates under cartesian coordinate system.
5th step:According to overlapping re-construction theory, the dual wavelength line carrier frequency Moire fringe phase shift after Coordinate Conversion is done Relating to figure carries out interlocking to be spaced obtaining its space-time bar graph.
6th step:Fourier transformation is carried out to space-time bar graph, its spectrum distribution is obtained, to space-time bar graph frequency Select to be located at the forward direction of orientation in the 5th step in spectrum, and the phase spectrum at initial point d/4 carries out band logical filter Ripple, wherein d are overall length of the frequency spectrum in orientation, obtain phase component.
7th step:Inverse Fourier transform is carried out to phase component, obtains its briquetting extension phase place P ', by briquetting Extension phase place P ' according to arrangement mode in the 5th step, inversely extracted, return to the pressure of original phase size Bag phase place P, carries out unpacking acquisition unpacking phase place UP to whichq.
8th step:To unpacking phase place UP for obtainingqInverse transformation side according to secondary polar coordinate transform in the 4th step Formula, is cartesian coordinate system by polar coordinate transform, tries to achieve final phase distribution UP.
Compared with prior art, it is an advantage of the current invention that:(1) by processing two kinds of wavelength-interferometric stripe stack Round carrier frequency moiré topography afterwards, high frequency is obtained the composite wave strip that Single wavelength interference fringe information is converted to low frequency Line information, expands detection range;(2) circle carrier coded fringes are transformed to by line carrier frequency using secondary polar coordinate transform Striped, reduces intractability, improves precision;(3) combine carrier frequency and re-construction theory is overlapped, with synthetic wavelength pi/2 For phase shift stepping-in amount, it is achieved that its frequency spectrum is separated with each component, it is easy to which the synthetic wavelength phase place for extracting low frequency is divided Amount, and while the impact of Phase-shifting Errors can be suppressed.
Description of the drawings
Fig. 1 is a kind of synthetic wavelength phase extraction method flow chart theoretical based on circle carrier frequency Moire fringe.
Fig. 2 is to detect radius of curvature using 100mm bore dual wavelength fizeau interferometer in the embodiment of the present invention 41.4m the oval carrier frequency moire map of the collected double wave of the anti-sphere of height.
Fig. 3 be in the embodiment of the present invention the oval carrier frequency moire map of double wave through secondary polar coordinate transform Dual wavelength line carrier frequency moire map afterwards.
Fig. 4 is that dual wavelength line carrier frequency moire map is obtained after carrying out folded array in the embodiment of the present invention Space-time bar graph.
Fig. 5 is briquetting phase place P of original phase size under polar coordinate system in the embodiment of the present invention.
Fig. 6 be using based on the theoretical synthetic wavelength phase extraction of circle carrier frequency Moire fringe in the embodiment of the present invention Method is solved and obtains phase distribution to be measured.
Specific embodiment
Below in conjunction with the accompanying drawings the present invention is described in further detail.
In conjunction with Fig. 1, a kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe, step is such as Under:
The first step:It is λ using operation wavelength1And λ2Striking rope type (application number:CN201310589143) or Safe graceful type dual wavelength interference testing device (application number:CN201410342492) detection aspheric surface, two Wavelength is planted while working, the axial location for adjusting test mirrors introduces round carrier frequency by out of focus, obtains two kinds of wavelength and does Relate to the round carrier frequency moiré topography after stripe stack.
Second step:The output voltage of control Phase shifting adapter, realizes with synthetic wavelengthPi/2 Phase shift stepping-in amount carries out phase shift, collects the oval carrier frequency More of double wave of one group of 4 frame phase shift stepping-in amount for pi/2 Interference fringe, its light distribution is:
Wherein, IkFor the oval carrier frequency moire map light distribution of kth frame double wave, A is i.e. DC component, For wavelength X1Modulation degree,For wavelength X1Phase place to be measured, D for circle carrier frequency coefficient, S2For horizontal pixel Coordinate square and longitudinal direction pixel coordinate square sum (i.e. S2=x2+y2, x is horizontal pixel coordinate, and y is vertical To pixel coordinate), δ1,kFor kth frame interference pattern medium wavelength λ1Amount of phase shift,For wavelength X2Modulation degree,For wavelength X2Phase place to be measured, δ2,kFor kth frame interference pattern medium wavelength λ2Amount of phase shift.
3rd step:DC component is removed using the method for average to collecting double wave oval carrier frequency moire map Afterwards, carry out square, the oval carrier frequency moire map light distribution of the double wave after obtaining square is:
Wherein, A ' for square after DC component, B1For wavelength X1The coefficient of two harmonics, i.e., With wavelength X1Downward systemRelevant, B2For wavelength X2The coefficient of two harmonics, i.e.,With Wavelength X2Downward systemRelevant, B3For wavelength X1Downward systemWith wavelength X2Downward systemTake advantage of Product,For synthetic wavelength phase place, δeq,kFor kth frame interference pattern medium wavelength λeq Amount of phase shift.
4th step:Determine the fringe center for collecting round carrier frequency moire map, to Moire fringe phase shift Interference pattern carries out secondary polar coordinate transform respectively, obtains dual wavelength line carrier frequency Moire fringe phase-shift interference, its seat Marking transformation for mula is:
Wherein, (ρ, θ) is the point coordinates under polar coordinate system, and (x, y) is under cartesian coordinate system corresponding to point (ρ, θ) Point coordinates, (x0,y0) for the fringe center point coordinates under cartesian coordinate system.
5th step:The dual wavelength line carrier frequency Moire fringe phase shift after Coordinate Conversion is interfered according to overlapping re-construction theory Figure carries out staggered being spaced and obtains its space-time bar graph, the polar coordinates before the space-time bar graph after conversion and conversion Under system, the relation of dual wavelength line carrier frequency Moire fringe phase-shift interference is:
S'(Nx+n, y)=Sn(x,y);
6th step:Fourier transformation is carried out to space-time bar graph, its spectrum distribution is obtained, to space-time bar graph frequency (d is frequency spectrum in orientation at initial point 1/4d to select the forward direction positioned at orientation in step 5 in spectrum Overall length) phase spectrum carry out bandpass filtering, obtain phase component.
7th step:Inverse Fourier transform is carried out to phase component, obtains its briquetting extension phase place P ', by briquetting Extension phase place P ' according to arrangement mode in step 5, inversely extracted, return to the pressure of original phase size Bag phase place P, carries out unpacking acquisition unpacking phase place UP to whichq.
8th step:To obtain unpacking phase place UP according to secondary polar coordinate transform in step 4 inverse transformation mode, It is cartesian coordinate system by polar coordinate transform, tries to achieve final phase distribution UP.
Embodiment 1
The first step:Aspherical using the test of 100mm bore dual wavelength fizeau interferometer, interferometer work wavelength divides Wei not λ1=632.8nm and λ2=532nm, the axial location for adjusting test mirrors obtains two kinds of wavelength-interferometric stripeds Round carrier frequency moiré topography after superposition;
Second step:The output voltage of control Phase shifting adapter, realizes with synthetic wavelength λeq=3.339 μm of pi/2 Adopting phase shift stepping-in amount carries out phase shift, integrates the dual wavelength for obtaining one group of 4 frame phase shift stepping-in amount as pi/2 using CCD Circle carrier frequency moire map, the oval carrier frequency moire map of its double wave are specifically as shown in Figure 2;
3rd step:Divided using method of average removal direct current to collecting the oval carrier frequency moire map of double wave After amount, carry out square, the oval carrier frequency moire map light distribution of the double wave after obtaining square;
4th step:Determine the fringe center for collecting round carrier frequency moire map, to Moire fringe phase shift Interference pattern carries out secondary polar coordinate transform respectively, obtains dual wavelength line carrier frequency Moire fringe phase-shift interference, and which two Dual wavelength line carrier frequency moire map after secondary polar coordinate transform is specifically as shown in Figure 3
5th step:The dual wavelength line carrier frequency Moire fringe phase shift after Coordinate Conversion is interfered according to overlapping re-construction theory Figure carries out staggered being spaced and obtains its space-time bar graph, and the space-time bar graph after conversion is as shown in Figure 4;
6th step:Fourier transformation is carried out to space-time bar graph, its spectrum distribution is obtained, to space-time bar graph frequency (d is frequency spectrum in orientation at initial point 1/4d to select the forward direction positioned at orientation in step 5 in spectrum Overall length) phase spectrum carry out bandpass filtering, obtain phase component;
7th step:Inverse Fourier transform is carried out to phase component, obtains its briquetting extension phase place P ', by briquetting Extension phase place P ' according to arrangement mode in step 5, inversely extracted, return to the pressure of original phase size Bag phase place P unpacks phase place UP as shown in figure 5, carrying out unpacking to which obtainingq
8th step:To obtain unpacking phase place UP according to secondary polar coordinate transform in step 4 inverse transformation mode, It is cartesian coordinate system by polar coordinate transform, tries to achieve final phase distribution UP as shown in Figure 6.
Compared with the conventional method, based on the theoretical synthetic wavelength phase extraction method of circle carrier frequency Moire fringe by place Round carrier frequency moiré topography after two kinds of wavelength-interferometric stripe stack of reason, high frequency is obtained Single wavelength interference fringe information The synthetic wavelength stripe information of low frequency is converted to, expands detection range;And will circle using secondary polar coordinate transform Carrier coded fringes are transformed to line carrier coded fringes, reduce intractability, improve precision;Overlapping in combination with carrier frequency Re-construction theory, with synthetic wavelength pi/2 as phase shift stepping-in amount, it is achieved that its frequency spectrum is separated with each component, it is easy to The synthetic wavelength phase component of low frequency is extracted, and while the impact of Phase-shifting Errors can be suppressed.

Claims (1)

1. a kind of based on the synthetic wavelength phase extraction method for justifying carrier frequency Moire fringe theory, it is characterised in that Method and step is as follows:
The first step:λ is respectively using operation wavelength1And λ2Dual wavelength interference testing device detect aspherical face Shape, wherein λ1≠λ2, two kinds of wavelength are while work, the axial location for adjusting test mirrors introduces round load by out of focus Frequently, the round carrier frequency moiré topography after two kinds of wavelength-interferometric stripe stack is obtained;
Second step:The output voltage of control Phase shifting adapter, realizes with synthetic wavelengthPi/2 Phase shift is carried out for phase shift stepping-in amount, CCD collects the oval load of double wave of one group of 4 frame phase shift stepping-in amount for pi/2 Frequency moire map, its light distribution is:
Wherein, IkFor the oval carrier frequency moire map light distribution of kth frame double wave, A is i.e. DC component,For wavelength X1Modulation degree,For wavelength X1Phase place to be measured, D for circle carrier frequency coefficient, S2For horizontal Pixel coordinate square and longitudinal pixel coordinate square sum, S2=x2+y2, x is horizontal pixel coordinate, and y is Longitudinal pixel coordinate, δ1,kFor kth frame interference pattern medium wavelength λ1Amount of phase shift,For wavelength X2Modulation degree,For wavelength X2Phase place to be measured, δ2,kFor kth frame interference pattern medium wavelength λ2Amount of phase shift;
3rd step:The oval carrier frequency moire map of double wave to collecting removes direct current using the method for average and divides After amount, carry out square, the oval carrier frequency moire map light intensity I ' of the double wave after obtaining squarenIt is distributed as:
Wherein, A ' for square after DC component, B1For wavelength X1The coefficient of two harmonics,B2For wavelength X2The coefficient of two harmonics,B3For wavelength X1Under Modulation degreeWith wavelength X2Downward systemProduct, For synthetic wavelength Phase place, δeq,kFor kth frame interference pattern medium wavelength λeqAmount of phase shift;
4th step:Determine the fringe center for justifying carrier frequency moire map in second step per frame, to above-mentioned More Striped phase-shift interference carries out secondary polar coordinate transform respectively, obtains the load of the dual wavelength line after corresponding Coordinate Conversion Frequency Moire fringe phase-shift interference, its coordinate transform formula is:
{ x = x 0 + ρ cos θ y = y 0 + ρ sin θ - - - ( 3 )
Wherein, (ρ, θ) is the point coordinates under polar coordinate system, and (x, y) is cartesian coordinate system corresponding to point (ρ, θ) Under point coordinates, (x0,y0) for the fringe center point coordinates under cartesian coordinate system;
5th step:According to overlapping re-construction theory, the dual wavelength line carrier frequency Moire fringe phase shift after Coordinate Conversion is done Relating to figure carries out interlocking to be spaced obtaining its space-time bar graph;
6th step:Fourier transformation is carried out to space-time bar graph, its spectrum distribution is obtained, to space-time bar graph frequency Select to be located at the forward direction of orientation in the 5th step in spectrum, and the phase spectrum at initial point d/4 carries out band logical filter Ripple, wherein d are overall length of the frequency spectrum in orientation, obtain phase component;
7th step:Inverse Fourier transform is carried out to phase component, obtains its briquetting extension phase place P ', by briquetting Extension phase place P ' according to arrangement mode in the 5th step, inversely extracted, return to the pressure of original phase size Bag phase place P, carries out unpacking acquisition unpacking phase place UP to whichq
8th step:To unpacking phase place UP for obtainingqInverse transformation side according to secondary polar coordinate transform in the 4th step Formula, is cartesian coordinate system by polar coordinate transform, tries to achieve final phase distribution UP.
CN201510523660.2A 2015-08-24 2015-08-24 A kind of synthetic wavelength phase extraction method based on circle carrier frequency Moire fringe theory Expired - Fee Related CN106482664B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201510523660.2A CN106482664B (en) 2015-08-24 2015-08-24 A kind of synthetic wavelength phase extraction method based on circle carrier frequency Moire fringe theory

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510523660.2A CN106482664B (en) 2015-08-24 2015-08-24 A kind of synthetic wavelength phase extraction method based on circle carrier frequency Moire fringe theory

Publications (2)

Publication Number Publication Date
CN106482664A true CN106482664A (en) 2017-03-08
CN106482664B CN106482664B (en) 2019-02-05

Family

ID=58233766

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510523660.2A Expired - Fee Related CN106482664B (en) 2015-08-24 2015-08-24 A kind of synthetic wavelength phase extraction method based on circle carrier frequency Moire fringe theory

Country Status (1)

Country Link
CN (1) CN106482664B (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106931905A (en) * 2017-03-09 2017-07-07 北京理工大学 A kind of digital Moiré patterns phase extraction method based on nonlinear optimization
CN110375641A (en) * 2019-07-19 2019-10-25 黑龙江大学 Based on the circle carrier frequency digital holographic detection device and method for improving Michelson structure
CN114485473A (en) * 2022-02-21 2022-05-13 上海电机学院 Laser interference phase demodulation method based on component synthesis and gradient projection
CN114608472A (en) * 2022-02-22 2022-06-10 珠海迈时光电科技有限公司 Wide spectrum interference microscopic measuring method, device, electronic equipment and medium

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103557948A (en) * 2013-09-25 2014-02-05 南京理工大学 Optical system wavefront measurement device and method based on circular carrier frequency phase demodulation method
CN104236452A (en) * 2014-07-17 2014-12-24 华南师范大学 Single-monochrome-CCD phase shift dual-wavelength interferometry method based on specific phase shift amount
CN104655290A (en) * 2013-11-20 2015-05-27 南京理工大学 Fizeau dual-wavelength laser tuning phase-shifting interference testing device and testing method thereof
CN104713494A (en) * 2013-12-16 2015-06-17 南京理工大学 Testing device and method for dual-wavelength tuning interference marked by Fourier transforming phase shifting

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103557948A (en) * 2013-09-25 2014-02-05 南京理工大学 Optical system wavefront measurement device and method based on circular carrier frequency phase demodulation method
CN104655290A (en) * 2013-11-20 2015-05-27 南京理工大学 Fizeau dual-wavelength laser tuning phase-shifting interference testing device and testing method thereof
CN104713494A (en) * 2013-12-16 2015-06-17 南京理工大学 Testing device and method for dual-wavelength tuning interference marked by Fourier transforming phase shifting
CN104236452A (en) * 2014-07-17 2014-12-24 华南师范大学 Single-monochrome-CCD phase shift dual-wavelength interferometry method based on specific phase shift amount

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
JIN-PENG LI ET AL.: "Quadratic polar coordinate transform technique for the demodulation of circular carrier interferogram", 《OPTICS COMMUNICATIONS》 *
QIAN KEMAO: "Two-dimensional windowed Fourier transform for fringe pattern analysis: Principles, applications and implementations", 《OPTICS AND LASERS IN ENGINEERING》 *
SHOUYU WANG ET AL.: "Radial Hilbert transform phase retrieval algorithm for circular carrier interferogram", 《OPTICS COMMUNICATIONS》 *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106931905A (en) * 2017-03-09 2017-07-07 北京理工大学 A kind of digital Moiré patterns phase extraction method based on nonlinear optimization
CN106931905B (en) * 2017-03-09 2019-02-05 北京理工大学 A kind of digital Moiré patterns phase extraction method based on nonlinear optimization
CN110375641A (en) * 2019-07-19 2019-10-25 黑龙江大学 Based on the circle carrier frequency digital holographic detection device and method for improving Michelson structure
CN110375641B (en) * 2019-07-19 2021-04-09 黑龙江大学 Circular carrier frequency digital holographic detection device and method based on improved Michelson structure
CN114485473A (en) * 2022-02-21 2022-05-13 上海电机学院 Laser interference phase demodulation method based on component synthesis and gradient projection
CN114485473B (en) * 2022-02-21 2024-01-30 上海电机学院 Laser interference phase demodulation method based on component synthesis and gradient projection
CN114608472A (en) * 2022-02-22 2022-06-10 珠海迈时光电科技有限公司 Wide spectrum interference microscopic measuring method, device, electronic equipment and medium

Also Published As

Publication number Publication date
CN106482664B (en) 2019-02-05

Similar Documents

Publication Publication Date Title
CN106482664A (en) A kind of synthetic wavelength phase extraction method theoretical based on circle carrier frequency Moire fringe
CN101957182B (en) Large-caliber high-gradient optical mirror surface on-line measuring system
CN101832817B (en) Parallel complex frequency domain optical coherence tomography imaging method and system
CN102538986B (en) Three-window based common-path interference detecting method and device
CN104296677B (en) Common light path heterodyne ineterferometer based on low frequency differences acousto-optic frequency shifters phase shift
CN104655290A (en) Fizeau dual-wavelength laser tuning phase-shifting interference testing device and testing method thereof
CN103630086A (en) Dual-wavelength simultaneous phase-shift interferometry method based on monochromatic CCD (couple charged device)
CN102997863A (en) Direct detection system for surface-shape errors in full-aperture optical aspheric surfaces
CN100451535C (en) Phase-shift interference image information processing system and processing method thereof
CN104006948B (en) Based on the method that multimodal division cycle demodulates polarization maintaining optical fibre polarization coupled point position
CN105467806A (en) Single-pixel holographic camera
CN102749143B (en) Wavefront reconstruction method for improving measuring precision of Shack-Hartmann wavefront sensor
CN101866002A (en) Multi-baseline and multi-band InSAR phase unwrapping method based on Chinese remainder theorem
CN103399001B (en) A kind of crude oil identification method based on confocal micro Raman spectrum
CN105865370A (en) White-light scanning interferometry measurement method and system
CN104713494A (en) Testing device and method for dual-wavelength tuning interference marked by Fourier transforming phase shifting
CN104748671A (en) Nonlinear error correcting method and device for angular displacement type single-frequency laser interferometer
CN104165755A (en) Grating shear wave aberration detection interferometer and detection method thereof
CN105444693A (en) Surface form error measurement method for shallow aspheric surface
CN108279068B (en) Laser beam quality dynamic measuring device based on four-wave transverse shear interference
CN106767391B (en) The sensitivity enhancement device and method of four wavefront lateral shearing interference Wavefront sensors
CN103615993A (en) Microstructure testing system and method based on off-axis microscopic interferometry
CN102680117A (en) Common-path radial cutting liquid crystal phase shift interference wave-front sensor
CN108775861B (en) One kind being based on effective wavelength π/(2k) phase shift dual wavelength time domain phase demodulating method
CN105698702A (en) Diplopore heterodyne ineterferometer based on acousto-optic low-frequency difference phase shift

Legal Events

Date Code Title Description
C06 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
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20190205

Termination date: 20200824

CF01 Termination of patent right due to non-payment of annual fee