CN107462149A - A kind of phase shift interference measuring system and its wave plate phase shift method - Google Patents

A kind of phase shift interference measuring system and its wave plate phase shift method Download PDF

Info

Publication number
CN107462149A
CN107462149A CN201710533969.9A CN201710533969A CN107462149A CN 107462149 A CN107462149 A CN 107462149A CN 201710533969 A CN201710533969 A CN 201710533969A CN 107462149 A CN107462149 A CN 107462149A
Authority
CN
China
Prior art keywords
mrow
wave plate
phase shift
mtd
light
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
CN201710533969.9A
Other languages
Chinese (zh)
Other versions
CN107462149B (en
Inventor
刘胜德
李娇声
吕晓旭
钟丽云
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.)
South China Normal University
Original Assignee
South China Normal 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 South China Normal University filed Critical South China Normal University
Priority to CN201710533969.9A priority Critical patent/CN107462149B/en
Publication of CN107462149A publication Critical patent/CN107462149A/en
Application granted granted Critical
Publication of CN107462149B publication Critical patent/CN107462149B/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
    • G01B9/00Measuring instruments characterised by the use of optical techniques
    • G01B9/02Interferometers
    • G01B9/02015Interferometers characterised by the beam path configuration
    • 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
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/30Measuring arrangements characterised by the use of optical techniques for measuring roughness or irregularity of surfaces

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Instruments For Measurement Of Length By Optical Means (AREA)
  • Microscoopes, Condenser (AREA)

Abstract

The present invention relates to optical interferometry and digital hologram field of measuring technique, a kind of phase shift interference measuring system and its wave plate phase shift method are provided, build phase shift interference measuring system, including light source, optical filter, first half wave plate, polarization beam splitter, first beam splitter, quarter-wave plate, second half wave plate, first polarizer and the first monochromatic black white image sensor, angle by the fixation quarter-wave plate is constant, adjust the anglec of rotation of the second half wave plate, realize any phase shift, it is not limited to be combined with the phase shift algorithm of particular step size, it is quick realization to be combined with the phase shift algorithm of present any phase-shift phase, high-precision phase shift interference measurement;And the drive device that accurately need not can be moved or rotate, system are succinct, easy to operate;Second half wave plate is equivalent to phase-shifter, it is not necessary to it is placed in optical interference circuit, therefore system will not be influenceed by mechanical movement, the stability of a system is more preferable.

Description

A kind of phase shift interference measuring system and its wave plate phase shift method
Technical field
The present invention relates to optical interferometry and digital hologram field of measuring technique, and in particular to a kind of phase shift interference measurement System and its wave plate phase shift method.
Background technology
Phase-shift interferometry is that one kind has the non-contact, whole audience, non-demolition, measurement is quick, measurement accuracy is high, can The optical phase measurement technology for the features such as being measured to irregular object, optical surface detection, three-dimensional have been widely used in it The fields such as topography measurement, imaging biological cells and digital hologram.In recent years, with computer technology and digital image processing techniques Continuous development, make interferometry this using the technology of light wave as measurement scale and measuring basis obtain more widely should With.
In the phase shift interference measurement of reality, the phase displacement error of phase-shifter and mechanical shock etc. can all directly affect phase Measurement accuracy.Therefore, the Stability and veracity of phase-shift phase plays vital effect in phase shift interference measurement.Traditional Time domain phase shifting method mainly includes:Piezoelectric ceramics (PZT) method, moving grating method, stretch light nanofarads, liquid crystal phase shift method, polarization Phase shift method, air phase shift method etc..But these methods all have the following disadvantages:(1) can accurately be moved due to needing Or the drive device of rotation, therefore systematic comparison is complicated;(2) phase-shifter is required for being placed in optical interference circuit, therefore system is held It is vulnerable to the influence of mechanical movement, the stability of a system is poor;(3) although traditional wave plate phase shift method can realize simple phase shift, But some special phase-shift values can only be obtained, any phase shift can not be realized, therefore can only be combined and make with some specific algorithms With precision and application are limited.
The content of the invention
The problem of existing for prior art, the present invention provide a kind of phase shift interference measuring system and its wave plate phase shift side Method, combination is simple, easy to operate and stably, effectively solves phase shift in single channel and multichannel phase shift interference measuring system Problem, realize simple, quick, high-precision, stable phase shift.
To achieve these goals, the present invention adopts the following technical scheme that:
A kind of phase shift interference measuring system, including light source, optical filter, the first half wave plate, polarization beam splitter, One beam splitter, quarter-wave plate, the second half wave plate, the first polarizer and the first monochromatic black white image sensor, institute The light that light source is sent is stated after the optical filter and the first half wave plate into the polarization beam splitter to be divided into Light beam and the second beam light, the optical path direction of the light beam are provided with the first plane mirror and the first microcobjective, The optical path direction of the second beam light is provided with the second plane mirror and the second microcobjective, and object under test is positioned over described It is anti-by first plane mirror and second plane mirror between two plane mirrors and second microcobjective The light penetrated enters first beam splitter after first microcobjective and second microcobjective respectively, and passes through institute Enter first polarizer after stating quarter-wave plate and the second half wave plate, by the described first monochromatic artwork master As sensor gathers.
Further, first polarizer and the first monochromatic black white image sensor are arranged at the light beam On optical path direction, the first monochromatic black white image sensor is used to gather from the light beam of the first polarizer outgoing Optical signal, the second polarizer and the second monochromatic black white image sensor are additionally provided with the optical path direction of the second beam light, it is described Second monochromatic black white image sensor is used for the optical signal for gathering the second beam light from second polarizer outgoing.
Further, the polarization direction setting at 45 ° of first polarizer and second polarizer.
A kind of wave plate phase shift method of phase shift interference measuring system, including:
Step 1:Build above-mentioned phase shift interference measuring system;
Step 2:The optical filter and the first half wave plate in regulating step one, to adjust contrast;
Step 3:The angle of the fixed quarter-wave plate is constant, adjusts the rotation of the second half wave plate Angle, to realize any phase shift.
Further, using the radiation direction that light source is sent as z-axis direction, then x-axis direction or y-axis direction are mutually hung down with z-axis direction Directly, the fast axle of quarter-wave plate described in step 1 and x-axis or y-axis are at 45 °.
Further, the anglec of rotation of the second half wave plate is adjusted in step 3 to realize the specific of any phase shift Method is:
The reference light and object light of interferometer are respectively a pair of orthogonal polarised light of polarization direction in the horizontal and vertical directions, Phase difference isTheir Jones vector E1And E2Respectively
Direction is shaken thoroughly in 45 ° of the first polarizer or the Jones matrix of the second polarizer, four point at 45 ° with x-axis of fast axle One of wave plate Jones matrix, and fast axle is respectively into the Jones matrix of θ half wave plate with x-axis:
Then reference light, object light are by the quarter-wave plate, the second half wave plate and first polarization The Jones vector of emergent light is expressed as after piece or second polarizer:
The light intensity I of the interference pattern finally formed on image device is:
Wherein symbol * represents conjugation, and e is natural constant, and i is imaginary unit, A1, A2It is shaking for reference light and object light respectively Width, from above formula (4) as can be seen that the light intensity that certain in interference field is put, is not only differed with positionIt is relevant, also with it is described The placed angle θ of second half wave plate is relevant, therefore, changes placed angle when rotating the second half wave plate When, interference fringe light and shade changes.
Further, phase-shift phase is 4 times of the second half wave plate anglec of rotation.
Beneficial effects of the present invention:
The phase shifting method of phase shift interference measuring system of the present invention can realize any phase shift, be not limited to and particular step size Phase shift algorithm combines, and can be combined with the phase shift algorithm of present any phase-shift phase and realize that quick, high-precision phase shift interference is surveyed Amount;And the drive device that accurately need not can be moved or rotate, system are succinct, easy to operate;Second half ripple Piece is equivalent to phase-shifter, it is not necessary to it is placed in optical interference circuit, therefore system will not be influenceed by mechanical movement, system is stable Property is more preferable.
Brief description of the drawings
Fig. 1 is a kind of structural representation for binary channels simultaneous phase shifting interference system that first embodiment of the invention provides;
Fig. 2 is a kind of structural representation for single channel phase shift interference system that second embodiment of the invention provides;
Fig. 3 is the width phase shifting interference gathered during second embodiment of the invention experiment measurement;
Fig. 4 is that phase-shift phase distribution corresponding to the 37 width phase shifting interferences gathered during second embodiment of the invention experiment measurement is bent Line;
It is 1-light source, 2-optical filter, the 3-the first half wave plate, 4-polarization beam splitter, 5-the first flat in figure Face speculum, the 6-the second plane mirror, 7-object under test, the 8-the second microcobjective, the 9-the first microcobjective, 10-the One beam splitter, 11-quarter-wave plate, the 12-the second half wave plate, the 13-the second beam splitter, the 14-the first polarizer, 15-the second polarizer, the 16-the first monochromatic black white image sensor, the 17-the second monochromatic black white image sensor, 101-light Source, 102-optical filter, the 103-the first half wave plate, 104-polarization beam splitter, the 105-the first plane mirror, 106-the second plane mirror, 107-object under test, the 108-the second microcobjective, the 109-the first microcobjective, 110-the One beam splitter, 111-quarter-wave plate, the 112-the second half wave plate, the 113-the first polarizer, the 114-the first list Color black white image sensor.
Embodiment
Below in conjunction with the accompanying drawing in the embodiment of the present invention, the technical scheme in the embodiment of the present invention is carried out clear, complete Site preparation describes, it is clear that described embodiment is only the part of the embodiment of the present invention, rather than whole embodiments.Base Embodiment in the present invention, those of ordinary skill in the art obtained under the premise of creative work is not made it is all its His embodiment, belongs to the scope of protection of the invention.
Such as Fig. 1, first embodiment of the invention provides binary channels simultaneous phase shifting interferometer measuration system, including light source 1, optical filter 2nd, the first half wave plate 3, polarization beam splitter 4, the first beam splitter 10, quarter-wave plate 11, the second half ripple The beam splitter 13 of piece 12 and second, the light that light source 1 is sent enter polarization spectro member after the half wave plate 3 of optical filter 2 and first Part 4, incident light are decomposed into P polarization light and S-polarization light by polarization beam splitter 4, and first is provided with the optical path direction of P polarization light The microcobjective 9 of plane mirror 5 and first, it is micro- that the second plane mirror 6 and second is provided with the optical path direction of S-polarization light Object lens 8, object under test 7 are placed between the second plane mirror 6 and the second microcobjective 8, and P polarization light is through the first plane reflection Mirror 5 reflects and enters the first beam splitter 10 after the first microcobjective 9, and S-polarization light reflects and passed through through the second plane mirror 6 Enter the first beam splitter 10 after crossing the microcobjective 8 of object under test 7 and second, then P polarization light and S-polarization light pass through a quarter Enter the second beam splitter 13 after the half wave plate 12 of wave plate 11 and second, it is inclined that first is provided with the optical path direction of P polarization light Shaken 14 and first monochromatic black white image sensor 16 of piece, and the second polarizer 15 and second is provided with the optical path direction of S-polarization light Monochromatic black white image sensor 17, the P that the first monochromatic black white image sensor 16 is used for collection from the outgoing of the first polarizer 14 are inclined Shake the optical signal of light, and the second monochromatic black white image sensor 17 is used for the light for gathering the S-polarization light from the outgoing of the second polarizer 15 Signal.
In the present embodiment, the light source 1 is the He-Ne lasers that a wavelength is 632.8nm, and the optical filter 2 is Neutral-density filter.
Binary channels simultaneous phase shifting interferometer measuration system of the present invention can be achieved to appoint by rotating the second half wave plate 12 Meaning phase shift.
In the present embodiment, using the radiation direction that light source 1 is sent as z-axis direction, x-axis direction or y-axis direction and z-axis direction Perpendicular, then the fast axle of quarter-wave plate 11 is at 45 ° with x or y.
First polarizer 14 is identical with the parameter of the second polarizer 15.In the present embodiment, the first polarizer 14 and second The polarization direction setting at 45 ° of polarizer 15.
First monochromatic black white image sensor 16 is identical with the specification of the second monochromatic black white image sensor 17.
Such as Fig. 2, second embodiment of the invention provides single channel phase shift interference measuring system, including light source 101, optical filter 102nd, the first half wave plate 103, polarization beam splitter 104, the first beam splitter 110, quarter-wave plate the 111, the 2nd 2 / mono- wave plate 112, the first polarizer 113 and the first monochromatic black white image sensor 114.The light that light source 101 is sent is through filtering Enter polarization beam splitter 104 after the half wave plate 103 of piece 102 and first, incident light is decomposed into by polarization beam splitter 104 P polarization light and S-polarization light, the first plane mirror 105 and the first microcobjective 109 are provided with the optical path direction of P polarization light, The second plane mirror 106 is provided with the optical path direction of S-polarization light and the second microcobjective 108, object under test 107 are placed on Between second plane mirror 106 and the second microcobjective 108, P polarization light reflects through the first plane mirror 105 and by the Enter the first beam splitter 110 after one microcobjective 109, S-polarization light reflects through the second plane mirror 106 and passes through object under test 107 and second enter the first beam splitter 110 after microcobjective 108, and then P polarization light and S-polarization light pass through quarter-wave plate 111 and second enter the first polarizer 113 after half wave plate 112, and are adopted by the first monochromatic black white image sensor 114 Collection, the first monochromatic black white image sensor 114 are used for the optical signal for gathering the P polarization light from the outgoing of the first polarizer 113.
In the present embodiment, the He-Ne lasers that the light source 101 is 632.8nm for a wavelength, the optical filter 2 For neutral-density filter.
Any phase can be achieved by rotating the second half wave plate 112 in single channel phase shift interference measuring system of the present invention Move.
In the present embodiment, using the radiation direction that light source 101 is sent as z-axis direction, x-axis direction or y-axis direction and z-axis side To perpendicular, then the fast axle of quarter-wave plate 111 is at 45 ° with x or y.
The present invention also provides a kind of wave plate phase shift method of phase shift interference measuring system, including:
Step 1:Build phase shift interference measuring system as shown in Figure 1 or 2;
Step 2:By the optical filter 2,102 in regulating step one and the first half wave plate 3,103, with regulation pair Degree of ratio;
Step 3:The angle of fixed quarter-wave plate 11,111 is constant, the second half wave plate 12,112 of regulation The anglec of rotation, to realize any phase shift.
Specifically, the fast axle of quarter-wave plate 11,111 should be at 45 ° with the x-axis in diagram or y-axis in step 1.
Specifically, the polarization direction of the first polarizer 14 and the second polarizer 15 is at 45 ° in first embodiment step 1 Set.
In the present invention, any phase is realized by adjusting the anglec of rotation of the second half wave plate 12,112 in step 3 The specific method of shifting is:
The reference light and object light of interferometer are respectively a pair of orthogonal polarised light of polarization direction in the horizontal and vertical directions, Phase difference isTheir Jones vector E1And E2Respectively
The saturating direction that shakes is at 45 ° in 45 ° of the first polarizer 14 or the Jones matrix of the second polarizer 15, fast axle and x-axis The Jones matrix of quarter-wave plate 11, and fast axle are distinguished with x-axis into the Jones matrix of θ the second half wave plate 12 For:
Then reference light, object light pass through quarter-wave plate 11, the second half wave plate 12 and the first polarizer 14 or the The Jones vector of emergent light is expressed as after two polarizers 15:
The light intensity I of the interference pattern finally formed on image device is:
Wherein symbol * represents conjugation, and e is natural constant, and i is imaginary unit, A1, A2It is shaking for reference light and object light respectively Width, from above formula (4) as can be seen that the light intensity that certain in interference field is put, is not only differed with positionIt is relevant, also with second The placed angle θ of half wave plate 12 is relevant, therefore, when rotating the second half wave plate 12 change placed angle, does Striped light and shade is related to change.Here the second half wave plate 12 is equivalent to time domain phase-shifter, and phase-shift phase is the two or two/ 4 times of the one wave plate anglec of rotation.
In order to further prove the practicality of the inventive method, the present invention is using second embodiment measurement as shown in Figure 2 Light path system carries out experiment measurement.Keep fast axle and the x directions of quarter-wave plate 111 at 45 °, be spaced 10 ° to rotate second Half wave plate 112, until rotate a circle 360 °, while interference pattern is gathered come corresponding using CCD, finally using it is improved most The method (AIA) that a young waiter in a wineshop or an inn multiplies iteration calculates the phase-shift phase of this 37 width interference pattern, wherein a width phase shifting interference such as Fig. 3 institutes gathered Show, phase-shift phase distribution curve is as shown in Figure 4 corresponding to 37 width.From the result in Fig. 4 can be seen that by rotation the two or two/ One wave plate 112 can realize any phase shift of system, and phase-shift phase is 4 times of the anglec of rotation of the second half wave plate 112.
The above embodiments are merely illustrative of the technical solutions of the present invention and it is unrestricted, although with reference to preferred embodiment to this hair It is bright to be described in detail, it will be appreciated by those skilled in the art that technical scheme can be modified or waited With replacing, without departing from the objective and scope of the technical program, it all should cover in scope of the presently claimed invention.

Claims (7)

  1. A kind of 1. phase shift interference measuring system, it is characterised in that including:Light source, optical filter, the first half wave plate, polarization Beam splitter, the first beam splitter, quarter-wave plate, the second half wave plate, the first polarizer and the first monochromatic artwork master As sensor, the light that the light source is sent enters the polarization spectro after the optical filter and the first half wave plate Element is divided into light beam and the second beam light, and the optical path direction of the light beam is provided with the first plane mirror and first Microcobjective, the optical path direction of the second beam light is provided with the second plane mirror and the second microcobjective, object under test are put It is placed between second plane mirror and second microcobjective, by first plane mirror and described second flat The light of face speculum reflection enters first beam splitting after first microcobjective and second microcobjective respectively Mirror, and enter first polarizer after the quarter-wave plate and the second half wave plate, by described One monochromatic black white image sensor collection.
  2. 2. phase shift interference measuring system according to claim 1, it is characterised in that:First polarizer and described first Monochromatic black white image sensor is arranged on the optical path direction of the light beam, and the first monochromatic black white image sensor is used Optical signal in collection from the light beam of the first polarizer outgoing, the is additionally provided with the optical path direction of the second beam light Two polarizers and the second monochromatic black white image sensor, the second monochromatic black white image sensor are used to gather from described second The optical signal of second beam light of polarizer outgoing.
  3. 3. phase shift interference measuring system according to claim 2, it is characterised in that:First polarizer and described second The polarization direction setting at 45 ° of polarizer.
  4. A kind of 4. wave plate phase shift method of phase shift interference measuring system, it is characterised in that including:
    Step 1:Build phase shift interference measuring system as claimed any one in claims 1 to 3;
    Step 2:The optical filter and the first half wave plate in regulating step one, to adjust contrast;
    Step 3:The angle of the fixed quarter-wave plate is constant, adjusts the anglec of rotation of the second half wave plate, To realize any phase shift.
  5. 5. the wave plate phase shift method of phase shift interference measuring system according to claim 4, it is characterised in that:Sent with light source Radiation direction be z-axis direction, then x-axis direction or y-axis direction and z-axis direction are perpendicular, quarter-wave described in step 1 The fast axle of piece and x-axis or y-axis are at 45 °.
  6. 6. the wave plate phase shift method of phase shift interference measuring system according to claim 4, it is characterised in that:Adjusted in step 3 Save the anglec of rotation of the second half wave plate using realize the specific method of any phase shift as:
    The reference light and object light of interferometer are respectively a pair of orthogonal polarised light of polarization direction in the horizontal and vertical directions, phase Difference isTheir Jones vector E1And E2Respectively
    Direction is shaken thoroughly in 45 ° of the first polarizer or the Jones matrix of the second polarizer, fast axle and x-axis a quarter at 45 ° The Jones matrix of wave plate, and fast axle is respectively into the Jones matrix of θ half wave plate with x-axis:
    <mrow> <mi>P</mi> <mrow> <mo>(</mo> <mi>&amp;pi;</mi> <mo>/</mo> <mn>4</mn> <mo>)</mo> </mrow> <mo>=</mo> <mfenced open = "[" close = "]"> <mtable> <mtr> <mtd> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </mtd> <mtd> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </mtd> <mtd> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </mtd> </mtr> </mtable> </mfenced> </mrow>
    <mrow> <mi>W</mi> <mrow> <mo>(</mo> <mi>&amp;pi;</mi> <mo>/</mo> <mn>2</mn> <mo>,</mo> <mi>&amp;pi;</mi> <mo>/</mo> <mn>4</mn> <mo>)</mo> </mrow> <mo>=</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mfenced open = "[" close = "]"> <mtable> <mtr> <mtd> <mrow> <mn>1</mn> <mo>+</mo> <mi>i</mi> </mrow> </mtd> <mtd> <mrow> <mn>1</mn> <mo>-</mo> <mi>i</mi> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mn>1</mn> <mo>-</mo> <mi>i</mi> </mrow> </mtd> <mtd> <mrow> <mn>1</mn> <mo>+</mo> <mi>i</mi> </mrow> </mtd> </mtr> </mtable> </mfenced> </mrow> 1
    <mrow> <mi>W</mi> <mrow> <mo>(</mo> <mi>&amp;pi;</mi> <mo>,</mo> <mi>&amp;theta;</mi> <mo>)</mo> </mrow> <mo>=</mo> <mfenced open = "[" close = "]"> <mtable> <mtr> <mtd> <mrow> <msup> <mi>cos</mi> <mn>2</mn> </msup> <mi>&amp;theta;</mi> <mo>+</mo> <msup> <mi>sin</mi> <mn>2</mn> </msup> <msup> <mi>&amp;theta;e</mi> <mrow> <mi>i</mi> <mi>&amp;pi;</mi> </mrow> </msup> </mrow> </mtd> <mtd> <mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mi>sin</mi> <mn>2</mn> <mi>&amp;theta;</mi> <mrow> <mo>(</mo> <mn>1</mn> <mo>-</mo> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>&amp;pi;</mi> </mrow> </msup> <mo>)</mo> </mrow> </mrow> </mtd> </mtr> <mtr> <mtd> <mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mi>sin</mi> <mn>2</mn> <mi>&amp;theta;</mi> <mrow> <mo>(</mo> <mn>1</mn> <mo>-</mo> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>&amp;pi;</mi> </mrow> </msup> <mo>)</mo> </mrow> </mrow> </mtd> <mtd> <mrow> <msup> <mi>sin</mi> <mn>2</mn> </msup> <mi>&amp;theta;</mi> <mo>+</mo> <msup> <mi>cos</mi> <mn>2</mn> </msup> <msup> <mi>&amp;theta;e</mi> <mrow> <mi>i</mi> <mi>&amp;pi;</mi> </mrow> </msup> </mrow> </mtd> </mtr> </mtable> </mfenced> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>2</mn> <mo>)</mo> </mrow> </mrow>
    Then reference light, object light by the quarter-wave plate, the second half wave plate and first polarizer or The Jones vector of emergent light is expressed as after second polarizer:
    The light intensity I of the interference pattern finally formed on image device is:
    Wherein symbol * represents conjugation, and e is natural constant, and i is imaginary unit, A1, A2It is reference light and the amplitude of object light respectively, from Above formula (4) not only differs as can be seen that the light intensity that certain in interference field is put with positionIt is relevant, also with described second The placed angle θ of half wave plate is relevant, therefore, when rotating the second half wave plate change placed angle, does Striped light and shade is related to change.
  7. 7. the wave plate phase shift method of phase shift interference measuring system according to claim 4, it is characterised in that:Phase-shift phase is institute State the second half wave plate anglec of rotation 4 times.
CN201710533969.9A 2017-07-03 2017-07-03 Phase-shift interferometry system and wave plate phase-shift method thereof Active CN107462149B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710533969.9A CN107462149B (en) 2017-07-03 2017-07-03 Phase-shift interferometry system and wave plate phase-shift method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710533969.9A CN107462149B (en) 2017-07-03 2017-07-03 Phase-shift interferometry system and wave plate phase-shift method thereof

Publications (2)

Publication Number Publication Date
CN107462149A true CN107462149A (en) 2017-12-12
CN107462149B CN107462149B (en) 2020-08-11

Family

ID=60544328

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710533969.9A Active CN107462149B (en) 2017-07-03 2017-07-03 Phase-shift interferometry system and wave plate phase-shift method thereof

Country Status (1)

Country Link
CN (1) CN107462149B (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109186764A (en) * 2018-09-11 2019-01-11 天津大学 A kind of acousto-optic modulation phase conjugation method for realizing scattering medium internal focus
CN109470173A (en) * 2018-12-29 2019-03-15 华南师范大学 A kind of binary channels simultaneous phase shifting interference microscopic system
CN110186388A (en) * 2019-05-13 2019-08-30 天津大学 Synchronization phase shift measurement system and method based on white light interference spectrum
CN112945083A (en) * 2021-01-29 2021-06-11 中国科学院长春光学精密机械与物理研究所 Parallel phase shift digital holographic microscopic imaging system with optical fiber interconnection
CN113405489A (en) * 2021-08-19 2021-09-17 南京施密特光学仪器有限公司 Method for inhibiting wave plate delay error interference in dynamic interferometer
CN113899305A (en) * 2021-09-30 2022-01-07 广东技术师范大学 Improved phase shift phase measurement method and system
CN114200723A (en) * 2021-10-29 2022-03-18 华南师范大学 Liquid crystal variable phase delay device without transverse deviation of light beam
CN114459619A (en) * 2022-01-27 2022-05-10 华南师范大学 Real-time online phase shift measurement device and method

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050259769A1 (en) * 2004-02-23 2005-11-24 Seagate Technology Llc Quadrature phase shift interferometer (QPSI) decoder and method of decoding
CN102914258A (en) * 2012-09-29 2013-02-06 哈尔滨工程大学 Synchronous phase shifting interference microscopy detection device and detection method based on orthogonal double-grating
CN102944169A (en) * 2012-11-26 2013-02-27 中国科学院长春光学精密机械与物理研究所 Simultaneous polarization phase-shifting interferometer
CN103712554A (en) * 2013-12-27 2014-04-09 华南师范大学 Dual-channel space-time mixing phase shifting Fizeau interferometer based on orthogonal polarized light
CN203929011U (en) * 2014-07-03 2014-11-05 佛山市南海区欧谱曼迪科技有限责任公司 Hyperchannel white light common path interference micro tomography system based on crossed polarized light
CN105300273A (en) * 2015-10-27 2016-02-03 中国科学院上海光学精密机械研究所 Dynamic point diffraction interferometer with adjustable fringe contrast

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050259769A1 (en) * 2004-02-23 2005-11-24 Seagate Technology Llc Quadrature phase shift interferometer (QPSI) decoder and method of decoding
CN102914258A (en) * 2012-09-29 2013-02-06 哈尔滨工程大学 Synchronous phase shifting interference microscopy detection device and detection method based on orthogonal double-grating
CN102944169A (en) * 2012-11-26 2013-02-27 中国科学院长春光学精密机械与物理研究所 Simultaneous polarization phase-shifting interferometer
CN103712554A (en) * 2013-12-27 2014-04-09 华南师范大学 Dual-channel space-time mixing phase shifting Fizeau interferometer based on orthogonal polarized light
CN203929011U (en) * 2014-07-03 2014-11-05 佛山市南海区欧谱曼迪科技有限责任公司 Hyperchannel white light common path interference micro tomography system based on crossed polarized light
CN105300273A (en) * 2015-10-27 2016-02-03 中国科学院上海光学精密机械研究所 Dynamic point diffraction interferometer with adjustable fringe contrast

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
易名: "《普通物理学教程光学》", 31 October 1999 *

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109186764A (en) * 2018-09-11 2019-01-11 天津大学 A kind of acousto-optic modulation phase conjugation method for realizing scattering medium internal focus
CN109470173A (en) * 2018-12-29 2019-03-15 华南师范大学 A kind of binary channels simultaneous phase shifting interference microscopic system
CN110186388A (en) * 2019-05-13 2019-08-30 天津大学 Synchronization phase shift measurement system and method based on white light interference spectrum
CN110186388B (en) * 2019-05-13 2021-04-06 天津大学 Synchronous phase shift measurement system and method based on white light interference spectrum
CN112945083A (en) * 2021-01-29 2021-06-11 中国科学院长春光学精密机械与物理研究所 Parallel phase shift digital holographic microscopic imaging system with optical fiber interconnection
CN113405489A (en) * 2021-08-19 2021-09-17 南京施密特光学仪器有限公司 Method for inhibiting wave plate delay error interference in dynamic interferometer
CN113405489B (en) * 2021-08-19 2021-11-02 南京施密特光学仪器有限公司 Method for inhibiting wave plate delay error interference in dynamic interferometer
CN113899305A (en) * 2021-09-30 2022-01-07 广东技术师范大学 Improved phase shift phase measurement method and system
CN113899305B (en) * 2021-09-30 2023-08-22 广东技术师范大学 Improved phase shift phase measurement method and system
CN114200723A (en) * 2021-10-29 2022-03-18 华南师范大学 Liquid crystal variable phase delay device without transverse deviation of light beam
CN114459619A (en) * 2022-01-27 2022-05-10 华南师范大学 Real-time online phase shift measurement device and method
CN114459619B (en) * 2022-01-27 2023-08-08 华南师范大学 Real-time online phase shift measurement device and method

Also Published As

Publication number Publication date
CN107462149B (en) 2020-08-11

Similar Documents

Publication Publication Date Title
CN107462149A (en) A kind of phase shift interference measuring system and its wave plate phase shift method
CN107014784B (en) A kind of measuring device and method of scattering medium vector transmission matrix
CN104713494B (en) The dual wavelength tuning interference testing device and method of Fourier transformation phase shift calibration
CN102749718B (en) Method and device for generating any vector light field based on trapezoidal Sagnac interferometer
CN103344176A (en) Octave type short coherence transient phase-shifting interferometer and measurement method used for detecting spherical topographic characteristics
CN204085698U (en) A kind of holographic measurement device of two-dimentional Jones matrix parameter
CN103968961A (en) Loop radial shearing N-step phase-shift interferometer based on polarization phase-shift principle
CN102914256A (en) Synchronous phase shifting interference detection device based on orthogonal double grating and detection method
CN102865810B (en) Orthogonal double-grating based detecting device for synchronous phase shift common-light path interference and detecting method therefor
CN103712554A (en) Dual-channel space-time mixing phase shifting Fizeau interferometer based on orthogonal polarized light
CN107121196B (en) A kind of Jones matrix parameter synchronous measuring apparatus and method inverting railway digital holography altogether based on visual field
CN103983366B (en) Oblique incidence reflection-type point diffractive plate and its interferometric method
CN101963495A (en) Device and method for measuring physical parameters of aeolotropic substance
CN107121205A (en) A kind of spot light dislocation type Mach-Zehnder interferometers measurement apparatus and method
CN207676126U (en) Phase shift interference striped generates system
CN109443554A (en) A kind of wavelength measuring apparatus and method based on graphene light logic gates
CN103471725B (en) Based on the Wave-front measurement device of modulated light source and positive and negative order of diffraction separate detection structure
KR101373709B1 (en) The measurement device and the method of the principle axis and retardation of the 3-dimensional film
CN102878922B (en) Device and method for detecting three-window common-path interference based on beam splitter prism
CN114323580A (en) Multidirectional synchronous phase shift transverse shearing interference device and measurement method
CN102840823B (en) Common-path interference detecting device based on beam-split synchronism phase shifting and detecting method
JPS6024401B2 (en) How to measure the physical constants of a measured object
TWI274142B (en) Apparatus and method for sequentially measuring multiple optical parameters of birefringence material
Kinyua et al. Interferometry analysis of cellophane birefringence
TW201031889A (en) Orthogonal-polarization Mirau interferometry and beam-splitting module and interferometric system using the same

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