CN103047928A - Random error mode evaluation method of phase shifting interferometer - Google Patents

Random error mode evaluation method of phase shifting interferometer Download PDF

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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
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error
phase
random
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interferometer
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CN103047928B (en
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马冬梅
邵晶
金春水
张海涛
于杰
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Changchun Institute of Optics Fine Mechanics and Physics of CAS
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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

Method for evaluating random error mode of phase-shifting interferometer
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:
Figure BDA0000262729581
where V is the interference fringe contrast, φnIs the reference phase at time t,
Figure BDA0000262729582
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)
Figure BDA0000262729583
Can be obtained from the following equation:
Figure BDA0000262729584
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:
s n = Im [ w n exp ( - i φ n ) ] = w n sin ( - φ n ) - - - ( 3 )
c n = Re [ w n exp ( - i φ n ) ] = w n cos ( φ n ) - - - ( 4 )
the extraction formula of the phase in such an interferometer is:
Figure BDA0000262729587
when the interferometer has an error source, the acquired image of the interference fringe is
Figure BDA0000262729588
To obtain
Figure BDA0000262729589
According to the formula arc tan ′ ( x ) = 1 1 + x 2
Figure BDA00002627295811
Figure BDA00002627295812
The errors of the test are:
Figure BDA00002627295813
due to the fact that
Figure BDA00002627295814
The above formula becomes:
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:
ΔI = dI ( x ) dx × Δx - - - ( 10 )
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:
Figure BDA00002627295817
Figure BDA00002627295818
the test error calculated at this time is
Figure BDA00002627295819
Wherein, Δ PnIs the phase shift error. Such error and
Figure BDA00002627295820
the 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:
Figure BDA00002627295822
Figure BDA00002627295823
wherein,
Figure BDA00002627295824
is the derivative of the wavefront. Error shape caused by vibration and
Figure BDA00002627295825
and
Figure BDA00002627295826
the two terms are in direct proportion, and the direction and the magnitude of the vibration are
Figure BDA00002627295827
Is 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:
Figure BDA00002627295829
Figure BDA00002627295830
wherein, DeltanIntensity is the light Intensity instability error. Error introduced by unstable power of light source
Figure BDA00002627295831
Andcorrelation, 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:
Figure BDA00002627295833
Figure BDA00002627295835
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 is
Figure BDA00002627295837
The 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)
Figure BDA00002627295838
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)
Figure BDA00002627295839
And
Figure BDA00002627295840
and (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)
Figure BDA00002627295841
And
Figure BDA00002627295842
it is related.
4. For the error caused by the unstable frequency of the light source, a stripe with frequency doubling is found in fig. 6, and the peak values of different periods in the stripe are continuously increased, which is similar to the term in equation (26)
Figure BDA00002627295843
It 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:
Figure FDA0000262729571
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:
Figure FDA0000262729574
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:
s n = Im [ w n exp ( - i φ n ) ] = w n sin ( - φ n ) - - - ( 3 )
c n = Re [ w n exp ( - i φ n ) ] = w n cos ( φ n ) - - - ( 4 )
the phase extraction formula (2) becomes:
Figure FDA0000262729577
when the interferometer has an error source, the acquired image of the interference fringe is
Figure FDA0000262729578
Figure FDA0000262729579
For the intensity variation of the interference fringes caused by the error source, the result is obtained:
according to the formula
Figure FDA00002627295711
Figure FDA00002627295712
The error of the test is:
due to the fact that
Figure FDA00002627295714
The above formula becomes:
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,
Figure FDA00002627295718
wherein,
Figure FDA00002627295719
is the derivative of the wavefront. Random error caused by vibration and
Figure FDA00002627295720
and
Figure FDA00002627295721
the two terms are in direct proportion, and the direction and the magnitude of the vibration are
Figure FDA00002627295722
The direction and the size of the Chinese characters are closely related;
random errors due to the instability of the power of the light source,
Figure FDA00002627295723
wherein, DeltanIntensity is the light Intensity instability error. Error introduced by unstable power of light source
Figure FDA00002627295724
And
Figure FDA00002627295725
correlation;
errors caused by the drift of the center frequency of the light source,
Figure FDA00002627295726
wherein, DeltanFreq is the error in the drift of the center frequency of the light source. Such error and
Figure FDA00002627295727
in direct proportion to each other, at the same time is
Figure FDA00002627295728
The terms are modulated.
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Cited By (2)

* Cited by examiner, † Cited by third party
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

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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

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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

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Cited By (3)

* Cited by examiner, † Cited by third party
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

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