CN110360923A - A kind of rotatable phase shifting interferometer of tested surface and measurement method - Google Patents

A kind of rotatable phase shifting interferometer of tested surface and measurement method Download PDF

Info

Publication number
CN110360923A
CN110360923A CN201910491332.7A CN201910491332A CN110360923A CN 110360923 A CN110360923 A CN 110360923A CN 201910491332 A CN201910491332 A CN 201910491332A CN 110360923 A CN110360923 A CN 110360923A
Authority
CN
China
Prior art keywords
mirror
tested
phase
mirror surface
optical splitter
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
CN201910491332.7A
Other languages
Chinese (zh)
Other versions
CN110360923B (en
Inventor
辛青
李泾渭
侯昌伦
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.)
Bihu Jiaxiao Photoelectric Technology Chongqing Co ltd
Original Assignee
Hangzhou Dianzi University
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 Hangzhou Dianzi University filed Critical Hangzhou Dianzi University
Priority to CN201910491332.7A priority Critical patent/CN110360923B/en
Publication of CN110360923A publication Critical patent/CN110360923A/en
Application granted granted Critical
Publication of CN110360923B publication Critical patent/CN110360923B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • G01B11/2441Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures using interferometry
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B9/00Measuring instruments characterised by the use of optical techniques
    • G01B9/02Interferometers
    • G01B9/02083Interferometers characterised by particular signal processing and presentation
    • G01B9/02085Combining two or more images of different regions

Abstract

The invention discloses a kind of rotatable phase shifting interferometer of tested surface and measurement methods;Phase shifting interferometer includes laser emitter, collimating mirror, optical splitter, reference mirror, measured object, convex lens, mirror surface rotator and CCD camera, on the laser emitter, collimating mirror, optical splitter, measured object distribution and same axis, the reference mirror and imaging lens are distributed in the preceding survey of optical splitter and rear survey, the mirror surface rotator are located at measured object bottom;Phase shift is achieved the purpose that by the angle of side by rotating, without the use of traditional phase-shifter, object can so save space, make interferometer not in the limitation by length without movement in orbit.

Description

A kind of rotatable phase shifting interferometer of tested surface and measurement method
Technical field
The present invention relates to a kind of optical interference instruments, and in particular to a kind of rotatable phase shifting interferometer of tested surface and survey Amount method.
Background technique
Phase shift interference measuring technique is one of the important means of Optical Surface detection.In general, phase shifting method can divide For two classes: hardware phase shift and frequency conversion phase shift.Frequency conversion phase shift interference is that phase-modulation, light are realized by the change of light source frequency Source uses Wavelength tunable laser.Hardware phase shift is typically all that reference mirror is driven to make axial movement modulation by piezoelectric ceramics The phase difference of two coherent lights, to realize the modulation to phase.
Phase shift interference measuring technique is that a corrugated in two relevant corrugateds is made to make staged or consecutive variations, is formed Interference fringe.The light intensity that each point in interference field is obtained with video camera or CCD camera, in each measurement point, the variation of phase difference Make the light intensity value of interference field that corresponding variation (constituting light intensity equation group) occur, obtains the measurement point by solving light intensity equation group Phase value, so as to find out the phase information or wavefront figure on corrugated to be measured.
Summary of the invention
In view of the deficiencies of the prior art, the present invention proposes a kind of rotatable phase shifting interferometer of tested surface and measurement sides Method.
A kind of rotatable phase shifting interferometer of tested surface, including laser emitter, collimating mirror, optical splitter, reference mirror, Tested mirror surface, convex lens, mirror surface rotator and CCD camera, it is characterised in that: the laser emitter, collimating mirror, optical splitter, On measured lens EDS maps and same axis, the reference mirror and imaging lens are distributed in the preceding survey of optical splitter and survey afterwards, described Mirror surface rotator is located at tested mirror;The emergent ray of laser emitter is incident on collimating mirror, the collimated light of collimating mirror outgoing Line reaches tested mirror surface transmitted through optical splitter by optical splitter, a part of light, and another part light is reflected by optical splitter To reference mirror, this two-beam line all returns optical splitter by mirror-reflection;The reflected light of reference mirror transmitted through beam splitter, The light that test surfaces are reflected back is reflected through optical splitter, at this point, this two-beam forms interference, and is passed through convex lens and is converged light Gather CCD camera;Wherein the rotation of mirror surface rotator adjusts the angle between tested mirror surface and vertical plane;The tested mirror surface is Single side mirror surface.
Preferably, it is the single-mode laser that wavelength is 632.8nm that the laser emitter, which is to emit laser,.
Preferably, the mirror surface rotator rotation adjusts the angle, θ of tested mirror surface and vertical plane, the model of the angle theta Enclose is -90 ° to 90 °.
A kind of measurement method of the rotatable phase shifting interferometer of tested surface;This method is specific as follows:
Step 1: rotation m secondary mirror rotator obtains the interference light intensity I of m width phase shifthmAnd the phase-shift phase δ of tested mirror surfaceh
The wherein expression formula of the interference pattern light intensity without phase shift are as follows:
A is background light intensity in formula, and B is light intensity system,For the Wave-front phase of testee;
The phase-shift phase δ of tested mirror surfacehExpression formula are as follows:
δh=h*tan (θ),
H indicates tested height value of the mirror surface different location relative to bottommost in formula, therefore after rotating an angle θ, It is different when phase-shift phase is at different height, it needs individually to solve the Wave-front phase of each height;
Its dephased interference pattern light intensity expression are as follows:
In formula m indicate testee the m time rotation, be the m time rotate after different height light intensity, be the m times rotate after The a certain height of tested surface phase shift;
Step 2: the 4 width interference fringe pictures that will be obtained calculate it by the wave of side shape by the algorithm of least square Preceding phase
Dephased interference pattern light intensity expression is unfolded, is obtained:
Due to being to need the unknown quantity that acquires, above formula can be write as:
Ihm=a+b cos (δhm)+c sin(δhm),
A=A in formula,
The theoretical value of interference light intensityThe value I obtained with actual measurementhmBetween error be expressed as:
M indicates the light intensity for the interference fringe that different phase-shift phases obtains in above formula, according to the principle of least square:
X=A-1B,
In formula
X=[a b c]T,
After acquiring vector, by side phase distribution are as follows:
The present invention compared with the existing technology the utility model has the advantages that by the angle of side achieve the purpose that phase shift by rotating, and Without using traditional phase-shifter, object can so save space, grow interferometer not without movement in orbit The limitation of degree.
Detailed description of the invention
Fig. 1 is the phase shifting interferometer structural block diagram that embodiment provides;
Structural block diagram when Fig. 2 is the phase shifting interferometer phase shift of embodiment offer;
Fig. 3 is the detected element rotational structure block diagram that embodiment provides;
Fig. 4 is the face shape X-Y scheme for the simulation that embodiment provides;
Fig. 5 is the interference pattern measured by the face shape simulated that embodiment provides;
Fig. 6 is the face shape for the non-unpacking that embodiment provides;
Fig. 7 is the face shape for having solved package that embodiment provides.
In figure, laser emitter 1, collimating mirror 2, optical splitter 3, convex lens 4, reference mirror 5, tested mirror surface 6, CCD camera 7, mirror surface rotator 8
Specific embodiment
In order to more specifically describe the present invention, with reference to the accompanying drawing and specific embodiment is to technical solution of the present invention It is described in detail.
Embodiment
Fig. 1 is the phase shifting interferometer structural block diagram that embodiment provides.A kind of rotatable phase shifting interferometer of tested surface, packet Include laser emitter 1, collimating mirror 2, optical splitter 3, reference mirror 5, tested mirror surface 6, convex lens 4, mirror surface rotator 8 and CCD phase Machine 7, the laser emitter, collimating mirror, optical splitter, on measured lens EDS maps and same axis, the reference mirror and imaging Camera lens is distributed in the preceding survey and rear survey of optical splitter, and the mirror surface rotator is located at tested mirror;The emergent light of laser emitter Line is incident on collimating mirror, and by optical splitter, a part of light reaches tested the collimated ray of collimating mirror outgoing transmitted through optical splitter Mirror surface, another part light reflect it to reference mirror by optical splitter, this two-beam line all returns optical splitter by mirror-reflection;Ginseng Examine mirror-reflection return light transmitted through beam splitter, the light that test surfaces are reflected back is reflected through optical splitter, at this point, this two Beam light forms interference, and passes through convex lens and light is converged to CCD camera;Wherein the rotation of mirror surface rotator adjust tested mirror surface with Angle between vertical plane;The tested mirror surface is single side mirror surface.
When measuring, rotator will will drive tested surface and rotate, as shown in Fig. 2, to reach the mesh of phase shift , as shown in Figure 3, Figure 4, schematic diagram when rotating for testee, rotation is equivalent to the generation of testee different height Mobile, after testee rotates the angle θ, the position apart from bottom h height is equivalent to the distance for moving L backward, L=h* tan(θ).After rotator rotates an angle, it will obtain new interference fringe picture.After rotator rotates four times, it will 4 width interference fringe pictures are obtained, the wavefront phase information of tested surface will be obtained by carrying out least square using 4 width interference fringe pictures.
One face shape of this real case simulation, face shape formula are as follows:
X and y indicates face shape in the position of space pixel in formula, and unit is pixel.If rotating its rotation angle θ every time, then The distance of the tested surface of different height mobile h*tan (θ), is equivalent to L for its distance, then 4 phase shifts are L respectively1, L2, L3, L4, coefficient matrices A can be obtained according to phase-shift phase,
It, can be in the hope of formula I according to coefficient matrixhm=a+b cos (δhm)+c sin(δhm) in coefficient a, b and c.
Finally acquire face shape, face shape as shown in fig. 6, the face shape still obtained at this time be package face shape, need to pass through solution Algorithm is wrapped up, keeps its face shape smooth, unpacking face is shaped like Fig. 7.

Claims (4)

1. a kind of rotatable phase shifting interferometer of tested surface, including it is laser emitter, collimating mirror, optical splitter, reference mirror, tested Mirror surface, convex lens, mirror surface rotator and CCD camera, it is characterised in that: the laser emitter, optical splitter, is tested collimating mirror With on same axis, the reference mirror and imaging lens are distributed in the preceding survey of optical splitter and survey afterwards, the mirror surface for mirror surface distribution Rotator is located at tested mirror;The emergent ray of laser emitter is incident on collimating mirror, and the collimated ray of collimating mirror outgoing is logical Optical splitter is crossed, a part of light reaches tested mirror surface transmitted through optical splitter, and another part light reflects it to ginseng by optical splitter Mirror surface is examined, this two-beam line all returns optical splitter by mirror-reflection;The reflected light of reference mirror is tested transmitted through beam splitter The light that face is reflected back is reflected through optical splitter, at this point, this two-beam forms interference, and is passed through convex lens and is converged to light CCD camera;Wherein the rotation of mirror surface rotator adjusts the angle between tested mirror surface and vertical plane;The tested mirror surface is single side Mirror surface.
2. the rotatable phase shifting interferometer of a kind of tested surface according to claim 1, it is characterised in that: the Laser emission It is the single-mode laser that wavelength is 632.8nm that device, which is to emit laser,.
3. the rotatable phase shifting interferometer of a kind of tested surface according to claim 1, it is characterised in that: the mirror surface rotation Device rotation adjusts the angle, θ of tested mirror surface and vertical plane, and the range of the angle theta is -90 ° to 90 °.
4. a kind of measurement method of the rotatable phase shifting interferometer of tested surface;It is characterized in that, this method is specific as follows:
Step 1: rotation m secondary mirror rotator obtains the interference light intensity I of m width phase shifthmAnd the phase-shift phase δ of tested mirror surfaceh
The wherein expression formula of the interference pattern light intensity without phase shift are as follows:
A is background light intensity in formula, and B is light intensity system,For the Wave-front phase of testee;
The phase-shift phase δ of tested mirror surfacehExpression formula are as follows:
δh=h*tan (θ),
H indicates tested height value of the mirror surface different location relative to bottommost in formula, therefore after rotating an angle θ, phase shift It is different when amount is at different height, it needs individually to solve the Wave-front phase of each height;
Its dephased interference pattern light intensity expression are as follows:
M indicates testee the m times rotation in formula, is the m times postrotational quilt for the light intensity of different height after the m times rotation The phase shift of a certain height in survey face;
Step 2: the 4 width interference fringe pictures that will be obtained calculate its wavefront phase by side shape by the algorithm of least square Position
Dephased interference pattern light intensity expression is unfolded, is obtained:
Due to being to need the unknown quantity that acquires, above formula can be write as:
Ihm=a+bcos (δhm)+csin(δhm),
A=A in formula,
The theoretical value of interference light intensityThe value I obtained with actual measurementhmBetween error be expressed as:
M indicates the light intensity for the interference fringe that different phase-shift phases obtains in above formula, according to the principle of least square:
X=A-1B,
In formula
X=[a b c]T,
After acquiring vector, by side phase distribution are as follows:
CN201910491332.7A 2019-06-06 2019-06-06 Phase shift interferometer with rotatable measured surface and measuring method Active CN110360923B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910491332.7A CN110360923B (en) 2019-06-06 2019-06-06 Phase shift interferometer with rotatable measured surface and measuring method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910491332.7A CN110360923B (en) 2019-06-06 2019-06-06 Phase shift interferometer with rotatable measured surface and measuring method

Publications (2)

Publication Number Publication Date
CN110360923A true CN110360923A (en) 2019-10-22
CN110360923B CN110360923B (en) 2020-12-29

Family

ID=68215715

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910491332.7A Active CN110360923B (en) 2019-06-06 2019-06-06 Phase shift interferometer with rotatable measured surface and measuring method

Country Status (1)

Country Link
CN (1) CN110360923B (en)

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5398112A (en) * 1993-10-04 1995-03-14 Wyko Corporation Method for testing an optical window with a small wedge angle
CN101809755A (en) * 2007-09-24 2010-08-18 高通Mems科技公司 Interferometric photovoltaic cell
CN102109414A (en) * 2010-12-15 2011-06-29 深圳大学 Method and device for calibrating phase modulation of spatial light modulators by utilizing heterodyne interference
CN102589440A (en) * 2012-01-11 2012-07-18 西安交通大学 Continuous variable-angle digital holographic metrology method and device
CN103292738A (en) * 2013-06-26 2013-09-11 中国科学院光电技术研究所 Absolute detection method for surface shape error of spherical surface
CN103431845A (en) * 2013-08-28 2013-12-11 北京信息科技大学 Optical coherence tomography method and device based on radial-direction polarized beams
CN204479017U (en) * 2015-03-13 2015-07-15 浙江师范大学 Spiral phase shift interference instrument apparatus
CN106813594A (en) * 2017-01-03 2017-06-09 中国科学院上海光学精密机械研究所 Heavy caliber glancing incidence reflects focus lamp high-precision surface shape detection method
CN108627254A (en) * 2018-06-01 2018-10-09 南京理工大学 A kind of change inclination angle phase shift Mach-Zender interferometer measuring device and method

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5398112A (en) * 1993-10-04 1995-03-14 Wyko Corporation Method for testing an optical window with a small wedge angle
CN101809755A (en) * 2007-09-24 2010-08-18 高通Mems科技公司 Interferometric photovoltaic cell
CN102109414A (en) * 2010-12-15 2011-06-29 深圳大学 Method and device for calibrating phase modulation of spatial light modulators by utilizing heterodyne interference
CN102589440A (en) * 2012-01-11 2012-07-18 西安交通大学 Continuous variable-angle digital holographic metrology method and device
CN103292738A (en) * 2013-06-26 2013-09-11 中国科学院光电技术研究所 Absolute detection method for surface shape error of spherical surface
CN103431845A (en) * 2013-08-28 2013-12-11 北京信息科技大学 Optical coherence tomography method and device based on radial-direction polarized beams
CN204479017U (en) * 2015-03-13 2015-07-15 浙江师范大学 Spiral phase shift interference instrument apparatus
CN106813594A (en) * 2017-01-03 2017-06-09 中国科学院上海光学精密机械研究所 Heavy caliber glancing incidence reflects focus lamp high-precision surface shape detection method
CN108627254A (en) * 2018-06-01 2018-10-09 南京理工大学 A kind of change inclination angle phase shift Mach-Zender interferometer measuring device and method

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
I. MANUELDE LA TORRE: "Laser speckle based digital optical methods in structural mechanics: A review", 《OPTICS AND LASERS IN ENGINEERING》 *
申劭萌,马军,何煦: "便携式泰曼格林型干涉仪装调方法研究", 《应用光学》 *
马云,陈磊,朱文华,刘一鸣,李建欣: "用于相位缺陷检测的动态泰曼干涉仪", 《中国激光》 *

Also Published As

Publication number Publication date
CN110360923B (en) 2020-12-29

Similar Documents

Publication Publication Date Title
US20230392920A1 (en) Multiple channel locating
US8416669B2 (en) Generation method for complex amplitude in-line hologram and image recording device using said method
CN102589416B (en) Wavelength scanning interferometer and method for aspheric measurement
CN110017767A (en) Spatial Phase-shifting Method dynamic interferometer and its application based on LCD space light modulator
CN101033937A (en) Method and device of light splitting, image-forming and synchronous phase-shifting in optical interferometry.
CN104414621B (en) Optical measuring device and optical chromatography method
CN104713494B (en) The dual wavelength tuning interference testing device and method of Fourier transformation phase shift calibration
CN103292740A (en) Three-dimensional scanner measuring method and device
CN103344176A (en) Octave type short coherence transient phase-shifting interferometer and measurement method used for detecting spherical topographic characteristics
CN103245423B (en) Light path polarized point diffraction movable phase interfere Wavefront sensor altogether
CN103712554B (en) Based on the Dual-channel space-time mixing phase shift fizeau interferometer of crossed polarized light
CN110017794A (en) A kind of dynamic phasing deformation interferometric measuring means and method
JP6307517B2 (en) Vibration measuring method and interferometer
CN102954758B (en) Interference detecting device based on synchronous carrier phase shift and detecting method of interference detecting device
EP3899420A1 (en) Full-field heterodyne interferometer for inspecting an optical surface
CN110375640A (en) A kind of rotary phase shifting interferometer and measurement method measuring transparent substance
CN207676126U (en) Phase shift interference striped generates system
CN116379961B (en) Phase measurement system and method
CN110360923A (en) A kind of rotatable phase shifting interferometer of tested surface and measurement method
CN114459620A (en) Device and method for generating pi phase shift between double interference channels through single wave plate
CN107167071A (en) Synchronous phase shift interference measurement apparatus based on depolarization Amici prism
Gao et al. Wide-angle Michelson interferometer based on LCoS
CN102840823A (en) Common-path interference detecting device based on beam-split synchronism phase shifting and detecting method
CN116608792B (en) Wavefront interferometry system and method
Stašík et al. Advanced measurement procedure for interferometric microscope for three-dimensional imaging of complex surfaces using two-wavelength interferometry and reference arm attenuation

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
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20211215

Address after: 230000 B-1015, wo Yuan Garden, 81 Ganquan Road, Shushan District, Hefei, Anhui.

Patentee after: HEFEI MINGLONG ELECTRONIC TECHNOLOGY Co.,Ltd.

Address before: 310018 No. 2 street, Xiasha Higher Education Zone, Hangzhou, Zhejiang

Patentee before: HANGZHOU DIANZI University

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20220926

Address after: No.19 Yunkai Road, Beibei District, Chongqing 400700

Patentee after: Bihu Jiaxiao photoelectric technology (Chongqing) Co.,Ltd.

Address before: 230000 B-1015, wo Yuan Garden, 81 Ganquan Road, Shushan District, Hefei, Anhui.

Patentee before: HEFEI MINGLONG ELECTRONIC TECHNOLOGY Co.,Ltd.