CN103047928A - Random error mode evaluation method of phase shifting interferometer - Google Patents
Random error mode evaluation method of phase shifting interferometer Download PDFInfo
- Publication number
- CN103047928A CN103047928A CN2012105627369A CN201210562736A CN103047928A CN 103047928 A CN103047928 A CN 103047928A CN 2012105627369 A CN2012105627369 A CN 2012105627369A CN 201210562736 A CN201210562736 A CN 201210562736A CN 103047928 A CN103047928 A CN 103047928A
- Authority
- CN
- China
- Prior art keywords
- error
- phase
- random
- caused
- interferometer
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000011156 evaluation Methods 0.000 title abstract description 7
- 238000012360 testing method Methods 0.000 claims abstract description 33
- 238000000034 method Methods 0.000 claims abstract description 18
- 238000004458 analytical method Methods 0.000 claims abstract description 6
- 230000010363 phase shift Effects 0.000 claims description 9
- 238000005259 measurement Methods 0.000 claims description 7
- 238000000605 extraction Methods 0.000 claims description 3
- 238000012512 characterization method Methods 0.000 claims 1
- 238000012423 maintenance Methods 0.000 abstract description 4
- 230000003287 optical effect Effects 0.000 description 3
- 238000005305 interferometry Methods 0.000 description 2
- 238000004088 simulation Methods 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000009795 derivation Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
Images
Landscapes
- Instruments For Measurement Of Length By Optical Means (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention discloses a random error mode evaluation method of a phase shifting interferometer, and the method belongs to the field of the error evaluation of interferometers. The method comprises the following steps that a certain inclination quantity is led in during a testing process; the average value of a plurality of measuring results serves as a reference value; the random testing error of one testing result is obtained by subtracting the reference value from one testing result; and the error is analyzed according to the characteristics of different error sources, so as to obtain the main error sources in an interference measuring process by analysis. According to the random error mode evaluation method of the phase shifting interferometer, the categories of the random error sources in the phase shifting interferometer are quickly obtained by analyzing the modes of the random errors and comparing the difference among the random error modes caused by various error sources, so as to provide convenient and quick guidance for the maintenance and the use of the interferometer.
Description
Technical Field
The invention belongs to the field of interferometer error evaluation, and particularly relates to a method for evaluating a random error mode of a phase-shifting interferometer.
Background
The phase-shifting interferometer is a high-precision optical measuring device and is widely applied to scientific research and production. As a high-precision optical instrument, the phase-shifting interferometer utilizes optical and mechanical components with high precision to ensure the testing precision. After a long time of use, the measurement accuracy of the interferometer is affected by the increasing random error. Typically, multiple expensive, high precision instruments are required to analytically find the source of random errors. This greatly increases the maintenance and use costs of the interferometer.
Disclosure of Invention
In order to solve the problems in the prior art, the invention provides an evaluation method for the random error modes of the phase-shifting interferometer, which analyzes the modes of random errors, and quickly obtains the types of the random error sources in the phase-shifting interferometer by comparing the differences among the random error modes caused by various error sources, thereby providing simple and quick instructions for the maintenance and the use of the interferometer.
The technical scheme adopted by the invention for solving the technical problem is as follows:
a method for evaluating a random error mode of a phase-shifting interferometer is characterized by comprising the following steps:
the method comprises the following steps: measuring a good wavefront for multiple times by using a phase-shifting interferometer, introducing inclination in the measuring process, and taking the average value of multiple measuring results after the inclination is introduced as a reference phase; then randomly taking one of the test phases, subtracting the reference phase to obtain a test error of a random measurement result:
step two: by analyzing the random error source of the phase-shifting interferometer, the relation between different types of error sources and test errors is obtained, and the random error caused by inaccurate phase shifting, the position noise error caused by vibration, the random error caused by unstable light source power and the error characteristic caused by the drift of the central frequency of the light source are deduced and obtained;
step three: and comparing the test errors in the test result obtained in the first step according to the characteristics of random errors caused by different error sources obtained by analysis, and determining the main error source in the interferometer.
The invention has the beneficial effects that: the invention determines the characteristics of random errors caused by different error sources through mathematical analysis and simulation, can help related personnel to quickly identify and search the error sources in the instrument, greatly saves the cost of equipment maintenance and detection through a high-precision instrument, and is convenient and simple.
Drawings
FIG. 1 is a test wavefront of a phase-shifting interferometer random error mode evaluation method of the present invention.
The figure 2 test introduces a certain amount of tilt in the interference fringes.
FIG. 3 shows random errors caused by phase misalignment.
Figure 4 random errors caused by vibration.
FIG. 5 random errors due to unstable light source intensity.
FIG. 6 shows random errors due to instability of the center frequency of the light source.
Detailed Description
The present invention will be described in further detail with reference to the accompanying drawings and examples.
A method for evaluating a random error mode of a phase-shifting interferometer is characterized by comprising the following steps:
the method comprises the following steps: the method comprises the following steps of measuring a good wavefront for multiple times by using a phase-shifting interferometer, wherein the root mean square error of the wavefront is 1/10-1/20 wavelength, introducing a certain amount of inclination in the measuring process, two to three straight fringes are arranged in the interference fringes, taking the average value of multiple measuring results after the inclination is introduced as a reference phase, and taking the average value of the multiple measuring results after the inclination is introduced, wherein most random errors can be eliminated well by taking the average value of the multiple measuring results as a reference value, so that the random errors in the measuring process can be extracted conveniently; then randomly taking one of the test phases, subtracting the reference phase to obtain a test error of a random measurement result:
the phase-shifting interferometer generates interference fringes under different phase conditions in a phase-shifting mode to obtain different light intensity equations, and the required phase in interferometry is obtained by solving the series of equations. The interference fringe obtained by phase shifting of the phase shifting interferometer can be obtained by the following formula:
where V is the interference fringe contrast, φnIs the reference phase at time t,is the phase under test.
The measured phase is determined according to the generalized phase extraction algorithm of the phase-shifting interferometer mentioned in the publication Peter de Groot "Derivation of algorithms for phase-shifting interferometry using the concept of a data-sampling window". APPLIEDDOPTICS, 34, 4723-4730 (1995)Can be obtained from the following equation:
for the window function wnIn the case of a real function, Re is a real part, Im represents an imaginary part, and the following formula can be taken:
the extraction formula of the phase in such an interferometer is:
when the interferometer has an error source, the acquired image of the interference fringe isTo obtain
The errors of the test are:
where k is a constant for the same phase-shifting algorithm, k can be considered to be 1 on the premise that the specific form of the measurement error is concerned.
Step two: through deep analysis of a random error source of the phase-shifting interferometer, the relation between different types of errors and test errors is obtained, and random errors caused by inaccurate phase shifting, position noise errors caused by vibration, random errors caused by unstable light source power and error characteristics caused by central frequency drift of a light source are deduced and obtained;
the random error sources present in phase-shifting interferometers are: random Error Phase Shift Error caused by Phase Shift nonlinearity, Position noise Error caused by vibration, Unstable Intensity Unstable of light source power, and Frequency Shift of light source center Frequency. The interferometer testing error is directly expressed as the change of the light intensity of the interference fringe, so the relationship between the light intensity variation and the error source is as follows:
where x is the magnitude of the error source. The light intensity variation and the measurement error caused by the four random error sources can be discussed according to the above formula.
1. Phase shift error:
the test error calculated at this time is
Wherein, Δ PnIs the phase shift error. Such error andthe terms are proportional, which means that random errors caused by inaccurate phase shift appear as regular fringes in the test result, the number of the fringes is twice that of the interference fringes
2. Vibration-induced position noise error:
wherein,is the derivative of the wavefront. Error shape caused by vibration andandthe two terms are in direct proportion, and the direction and the magnitude of the vibration areIs closely related to the direction and magnitude of the wave, random errors caused by vibration appear as frequency doubling fringes (relative to interference fringes) in the test results, but the peaks of the same ripples do not coincide.
3. Unstable error of light source power:
wherein, DeltanIntensity is the light Intensity instability error. Error introduced by unstable power of light sourceAndcorrelation, and therefore random errors caused by unstable light source power appear as frequency-doubled fringes in test results, peaks in different periods are not consistent, and the peaks in different periods change like waves (positive selection curves).
4. Error caused by drift of the center frequency of the light source:
wherein, DeltanFreq is the error in the drift of the center frequency of the light source. Such error andin direct proportion to each other, at the same time isThe terms are modulated so that the source center frequency drift causes random errors that appear as peaks of different periods in the doubled fringes growing or decreasing in the same direction.
Step three: and comparing the test errors in the test result obtained in the first step according to the characteristics of random errors caused by different error sources obtained by analysis, and determining the main error source in the interferometer.
In order to more precisely describe the difference between random errors caused by different random error sources, simulation is performed by artificially introducing random errors into a measured wavefront as shown in fig. 1 and fig. 2. The difference between the different random errors can be obtained by means of fig. 3 to 6.
1. For phase shift errors, frequency doubled regular fringes are found in fig. 3 and are associated with the interference fringes shown in fig. 1 (error has 4 periods and interference fringes has 2 periods). It is obvious that this is the same as in the formula (17)And correspondingly.
2. For vibration errors, there are also frequency-doubled fringes in fig. 4, but the peaks of the same ripple do not coincide over the frequency-doubled fringes. This phenomenon is related to the term in equation (20)Andand (4) the same.
3. For the light source instability error, a stripe with frequency doubling is found in fig. 5, the peaks of different periods are not consistent, and the peaks of different periods are like waves (positive selection curve) —And (4) changing. This phenomenon is related to the term in the formula (23)Andit is related.
Claims (2)
1. A method for evaluating a random error mode of a phase-shifting interferometer is characterized by comprising the following steps:
the method comprises the following steps: measuring a good wavefront for multiple times by using a phase-shifting interferometer, introducing inclination in the measuring process, and taking the average value of multiple measuring results after the inclination is introduced as a reference phase; then randomly taking one of the test phases, subtracting the reference phase to obtain a test error of a random measurement result:
step two: by analyzing the random error source of the phase-shifting interferometer, the relation between different types of error sources and test errors is obtained, and the random error caused by inaccurate phase shifting, the position noise error caused by vibration, the random error caused by unstable light source power and the error characteristic caused by the drift of the central frequency of the light source are deduced and obtained;
step three: and comparing the test errors in the test result obtained in the first step according to the characteristics of random errors caused by different error sources obtained by analysis, and determining the main error source in the interferometer.
2. A phase shifting interferometer random error characterization according to claim 1, wherein the relationship between the error source and the test error in step two of the method is derived by:
interference fringe I obtained by phase shift of phase-shift interferometernExpressed as:
where V is the interference fringe contrast, φnFor the purpose of referencing the phase(s),is the phase under test.
Measured phaseCan be obtained from the following equation:
wherein the window function w used in the solving algorithmnIn the case of a real function, Re is a real part, Im represents an imaginary part, and the following formula can be taken:
the phase extraction formula (2) becomes:
when the interferometer has an error source, the acquired image of the interference fringe is,For the intensity variation of the interference fringes caused by the error source, the result is obtained:
where k is a constant for the same phase-shifting algorithm, k can be considered as 1 on the premise that the specific form of the measurement error is concerned,
according to the different influence characteristics of different random error sources on the interference fringes, the error of the test result caused by the different random error sources can be deduced by the formula as follows:
with respect to the random error caused by the phase shift,
wherein, Δ PnTo shift the phaseAnd (4) error. It can be seen that the error isThe terms are proportional;
the position noise error caused by the vibration is,
wherein,is the derivative of the wavefront. Random error caused by vibration andandthe two terms are in direct proportion, and the direction and the magnitude of the vibration areThe direction and the size of the Chinese characters are closely related;
random errors due to the instability of the power of the light source,
wherein, DeltanIntensity is the light Intensity instability error. Error introduced by unstable power of light sourceAndcorrelation;
errors caused by the drift of the center frequency of the light source,
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201210562736.9A CN103047928B (en) | 2012-12-21 | 2012-12-21 | A kind of method of testing to phase-shifting interferometer stochastic error mode |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201210562736.9A CN103047928B (en) | 2012-12-21 | 2012-12-21 | A kind of method of testing to phase-shifting interferometer stochastic error mode |
Publications (2)
Publication Number | Publication Date |
---|---|
CN103047928A true CN103047928A (en) | 2013-04-17 |
CN103047928B CN103047928B (en) | 2015-12-09 |
Family
ID=48060662
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201210562736.9A Expired - Fee Related CN103047928B (en) | 2012-12-21 | 2012-12-21 | A kind of method of testing to phase-shifting interferometer stochastic error mode |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN103047928B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104534978A (en) * | 2014-12-29 | 2015-04-22 | 中国科学院长春光学精密机械与物理研究所 | Phase-shifting interference detection vibration restraining method |
CN105509638A (en) * | 2015-12-01 | 2016-04-20 | 中国科学院长春光学精密机械与物理研究所 | Phase-shift interference information processing method based on error compensation |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102425988A (en) * | 2011-11-20 | 2012-04-25 | 中国科学院光电技术研究所 | Phase extraction method for phase-shifting interference fringe pattern |
-
2012
- 2012-12-21 CN CN201210562736.9A patent/CN103047928B/en not_active Expired - Fee Related
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102425988A (en) * | 2011-11-20 | 2012-04-25 | 中国科学院光电技术研究所 | Phase extraction method for phase-shifting interference fringe pattern |
Non-Patent Citations (2)
Title |
---|
左芬等: "一种同步移相干涉测量***的误差研究", 《光学技术》 * |
马冬梅: "一种移相干涉仪的测试方法", 《第十四届全国光学测试学术讨论会论文摘要集》 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104534978A (en) * | 2014-12-29 | 2015-04-22 | 中国科学院长春光学精密机械与物理研究所 | Phase-shifting interference detection vibration restraining method |
CN104534978B (en) * | 2014-12-29 | 2017-04-05 | 中国科学院长春光学精密机械与物理研究所 | Detection vibration suppressing method is interfered in a kind of phase shift |
CN105509638A (en) * | 2015-12-01 | 2016-04-20 | 中国科学院长春光学精密机械与物理研究所 | Phase-shift interference information processing method based on error compensation |
Also Published As
Publication number | Publication date |
---|---|
CN103047928B (en) | 2015-12-09 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN105180892B (en) | A kind of femtosecond laser frequency comb pulse chirp interfeerometry ranging method and range-measurement system | |
CN103890539B (en) | Film thickness measuring method | |
CN103175822B (en) | Eliminate the method for table difference of Raman spectrometer | |
JP5983779B2 (en) | Gas absorption spectroscopy apparatus and gas absorption spectroscopy method | |
EP2606311B1 (en) | Apparatus and method for measuring distance | |
Hindsley et al. | An investigation of photoelectric radial-velocity spectrometers as used in the analysis of Cepheid variables. | |
CN103954589B (en) | The precision measurement apparatus of a kind of optical material specific refractory power and method | |
US10746537B2 (en) | Radius-of-curvature measurement by spectrally-controlled interferometry | |
CN105571830B (en) | The method for measuring super-narrow line width laser device laser line width | |
JP6707670B2 (en) | Precision positioning system using tunable laser | |
CN106248623A (en) | Refractive index measurement method, measurement apparatus and Optical element manufacturing method | |
CN110048765A (en) | A method of the Φ-OTDR quantitative measurment based on Least Square fitting | |
US9228828B2 (en) | Thickness monitoring device, etching depth monitoring device and thickness monitoring method | |
CN106482633A (en) | A kind of multiple-beam interference phase extraction method based on π/4 phase shift | |
CN102620809B (en) | Optical measuring method for in-plane vibration of micro-electromechanical structure | |
CN103047928B (en) | A kind of method of testing to phase-shifting interferometer stochastic error mode | |
JP2013120063A5 (en) | ||
Zhang et al. | Ultrahigh-accuracy measurement of refractive index curves of optical materials using interferometry technology | |
US9001337B2 (en) | Etching monitor device | |
CN105339779A (en) | Method and apparatus for measuring refractive index and method for manufacturing optical element | |
CN103630336B (en) | The dynamic interferometry method of array is postponed based on random phase retardation | |
US8692999B1 (en) | Crosstalk cancellation for a simultaneous phase shifting interferometer | |
RU2491505C1 (en) | Method of determining surface roughness | |
CN103471528A (en) | Method for measuring interference fringe inclination angle | |
Wei et al. | Using dispersion-induced group delay to solve the integer ambiguity problem: a theoretical analysis |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
CF01 | Termination of patent right due to non-payment of annual fee | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20151209 Termination date: 20171221 |