CN105606338B - A kind of centre wavelength error compensating method based on white light interference test system - Google Patents
A kind of centre wavelength error compensating method based on white light interference test system Download PDFInfo
- Publication number
- CN105606338B CN105606338B CN201610034498.2A CN201610034498A CN105606338B CN 105606338 B CN105606338 B CN 105606338B CN 201610034498 A CN201610034498 A CN 201610034498A CN 105606338 B CN105606338 B CN 105606338B
- Authority
- CN
- China
- Prior art keywords
- light
- phase
- centre wavelength
- step pitch
- error
- 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.)
- Expired - Fee Related
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
The invention discloses a kind of centre wavelength error compensating method based on white light interference test system, belong to fiber end face measuring instrument technical field.Described calculation method changes the optical path difference between reference beam and test beams by phase-shifter first, while gathering some width interference patterns, then interference pattern is carried out to solve the height for obtaining fiber end face.Phase only pupil filter is carried out to the intensity maxima for extracting based on Carr é phase shift algorithms, computational accuracy is influenceed because the centre wavelength of light source has calibrated error, therefore piezoelectric ceramics step pitch is calibrated first by single groove standard sample, online demarcation is carried out to wavelength by the step pitch after check and correction.Can reduce by the error that light source characteristic and environmental perturbation are brought, improve computational accuracy.
Description
Technical field
The present invention relates to a kind of centre wavelength error compensating method based on white light interference test system, belong to fiber end face
Measuring instrument technical field.
Background technology
Fiber end face measuring instrument is the principle based on white light interference, and bar is interfered so as to realize fiber end face using phase shift
The change of line.Fiber end face tester can be with non-contacting measurement optical fiber surface pattern accurately and fast.As the biography of optical signal
Defeated medium, fiber end face form directly affects optical signal transmission performance in a fiber, therefore fiber end face measurement to end face shape
The measurement of state is most important in Fibre Optical Sensor and transmission.Because fiber end face measuring instrument disclosure satisfy that optical fiber in production, application
During on-line testing demand, therefore, it is possible to be widely used in high power laser, military opto-electronic device, fiber-optic current sensor
The high-grade, precision and advanced sciemtifec and technical sphere such as device.
Fiber end face measuring instrument during interferometry, changed by phase-shifter reference beam and test beams it
Between optical path difference, while gathering some width interference patterns, then interference pattern is carried out to solve the height for obtaining fiber end face.Using
When Light bulb phase-shift interfering method is demodulated relevant peak, influence to calculate essence because the centre wavelength of light source has calibrated error
Degree, therefore a kind of online real-Time Compensation light source center wavelength error is designed, high precision, fireballing white light interference algorithm is particularly weighed
Will.
The content of the invention
The invention aims to solve the above problems, a kind of centre wavelength based on white light interference test system is proposed
Error compensating method, can be used for reducing centre wavelength calibrated error in fiber end face measuring system, and anti-interference, speed is fast, right
The linearity error of phase-shifter is insensitive.
Plant the centre wavelength error compensating method based on white light interference test system, including following steps:
The first step, demarcates piezoelectric ceramic motor step pitch;
Second step, with the centre wavelength of the online real-time calibration white light source of the step pitch demarcated;
3rd step, relative altitude is resolved based on Carr é phase shift algorithms using the wavelength for extracting;
The advantage of the invention is that:
The present invention can demarcate step pitch when fiber end face height value is resolved by single groove sample block, and real-time calibration is calculated
Light source center wavelength, anti-interference with reducing due to the centre wavelength calibrated error that environmental perturbation brings, speed is fast, to phase shift
The advantages of linearity error of device is insensitive.
Brief description of the drawings
Fig. 1 is fiber end face measuring system schematic diagram;
Fig. 2 is the graph of a relation of white light interference light intensity and optical path difference;
Fig. 3 is single groove sample block pictorial diagram;
Fig. 4 is that actual measurement height is the standard sample interference pattern of 663nm;
Fig. 5 is flow chart of the method for the present invention.
Specific embodiment
The present invention is described in detail with reference to the accompanying drawings and examples.
As shown in Fig. 1 the principle schematic of fiber end face measuring system, light source is by condenser, and aperture diaphragm is accurate
Straight beam expanding lens reaches Amici prism, and a portion light can reach tested optical fiber end face, and another part reaches reference mirror, after reflection
Microcobjective is reached simultaneously, finally reaches CCD imagings.When interfering, formed after the interference fringe superposition that each wavelength light is produced
White-light fringe, as shown in Figure 2.When piezoelectric ceramics (PZT) phase-shifter drives index plane to move, interference fringe can become
Change.
Fiber end face measuring system measures three-dimensional appearance, is the light intensity value according to the interference fringe image for being gathered, and obtains
The relative altitude value of body surface, it is critical only that the maximum relevant peak of the position i.e. light intensity value for accurately finding zero optical path difference
Position.White light interference light intensity has relation as shown in Figure 2 with optical path difference, and when optical path difference is 0, light intensity reaches maximum.
When step pitch is demarcated using single groove sample block, it is extracted respectively to the point outside the point and groove in same a line groove
The corresponding number of image frames of light strong extremum, the actual step pitch of piezoelectric ceramic motor can be drawn by groove height.
By the relation between wavelength and phase, centre wavelength is calculated with the step pitch demarcated in real time online.
Based on above-mentioned fiber end face measuring system, and optical path difference and light intensity relation, it is of the invention a kind of based on white
The centre wavelength error compensating method of interference of light test system, flow is as shown in figure 5, including following steps:
The first step, demarcates piezoelectric ceramic motor step pitch;
First, the step pitch of piezoelectric ceramic motor, single groove standard sample such as Fig. 3 institutes are demarcated by single groove standard sample
Show, the interference fringe that Fig. 4 is arrived for actual acquisition, Fig. 4 more intuitively illustrates the interference at interference fringe at groove and non-groove
Striped has the changing of the relative positions, therefore can demarcate piezoelectric ceramic motor by the movement of interference fringe when known groove depth H
Step pitch.The method that the present invention is used to extract its light strong extremum pair respectively to the point outside the point and groove in same a line groove
The number of image frames answered, respectively N1, N2, groove depth is H, then actual step pitch d can be by formulaTry to achieve;
Second step, with the centre wavelength of the online real-time calibration white light source of the step pitch demarcated;
When being scanned to measured object, the picture frame number P that zero order fringe is included can be extracted, be counted in real time by following formula
Calculate centre wavelength
3rd step, relative altitude is resolved based on Carr é phase shift algorithms using the wavelength for extracting;
The intensity level of the light synthesized by two-beam vibration:
In formula:IaRepresent the light intensity value of the light reflected by optical fiber surface, IbRepresent the light intensity value of the light reflected by reference mirror, I
The intensity level of the light of synthesis is represented,Represent light source by the light and light source after the reflection that spectroscope reaches measured object by light splitting
Mirror reaches the position difference with reference to light after reflection, so
Wherein, ImaxIt is intensity maxima, IminIt is light intensity minimum, γ is intetference-fit strengthening.
Make I0=Ia+Ib, then can obtain:
When optical path difference is zero, i.e.,When being zero, luminous intensity is peak value.Because sampling precision etc. is asked in actually measurement
Also there is the φ phase extraction errors of with zero optical path difference in topic, the maximum extracted, it is therefore desirable to solve φ and it is entered
Row amendment;In measurement process, it is accurately linear mobile that PZT drives reference mirror to carry out.Piezoelectric ceramics step pitch is set to d, then two-phase
Phase place change between adjacent imageDue to the presence of piezoelectric ceramics linearity error ε, phase place change is designated as:
Wherein,It is phase change value
Phase only pupil filter is carried out to the intensity maxima for extracting based on Carr é phase shift algorithms, its general principle is as follows:
Wherein:IbgIt is background light intensity value, I-3、I-1、I1、I3Respectively relative to before the zero order fringe light intensity value for being positioned 3
Frame, preceding 1 frame, rear 1 frame, the corresponding light intensity value of rear 3 frame.
Solve
From above formula, the extraction of phase is unrelated with the linearity error ε of piezoelectric ceramics.
By the resolving to phase, using the centre wavelength of online real-time calibrationThe relative altitude of measured object can be tried to achieve:
Wherein, h is relative altitude, and N is the corresponding picture frame number of intensity maxima.
Claims (1)
1. a kind of centre wavelength error compensating method based on white light interference test system, including following steps:
The first step, demarcates piezoelectric ceramic motor step pitch;
First, the step pitch of piezoelectric ceramic motor is demarcated by single groove standard sample, the step pitch of piezoelectric ceramic motor is:
Wherein, N1、N2It is that its corresponding picture frame of light strong extremum is extracted respectively to the point outside the point and groove in same a line groove
Number, H is groove depth;
Second step, with the centre wavelength of the online real-time calibration white light source of the step pitch demarcated;
When being scanned to measured object, the picture frame number P that zero order fringe is included is extracted, centre wavelength is calculated in real time
3rd step, relative altitude is resolved based on Carr é phase shift algorithms using the wavelength for extracting;
Obtain the intensity level of the light of two-beam vibration synthesis:
In formula:IaRepresent the light intensity value of the light reflected by optical fiber surface, IbThe light intensity value of the light reflected by reference mirror is represented, I is represented
The intensity level of the light of synthesis,Represent and reached with reference to warp with by spectroscope by the light after the reflection that spectroscope reaches measured object
The position difference of the light after reflection, if:
Wherein, ImaxIt is intensity maxima, IminIt is light intensity minimum, γ is intetference-fit strengthening;
Make I0=Ia+Ib, obtain:
When optical path difference is zero, i.e.,When being zero, luminous intensity is peak value;
To phase extraction error φ, it is modified, piezoelectric ceramics step pitch is d, the phase place change between two adjacent images isThen phase place change is:
Wherein,It is phase change value, ε represents piezoelectric ceramics linearity error;
Phase only pupil filter is carried out to the intensity maxima for extracting based on Carr é phase shift algorithms, its general principle is as follows:
Wherein:IbgIt is background light intensity value, I-3、I-1、I1、I3Respectively relative to 3 frames before the zero order fringe light intensity value for being positioned, preceding
1 frame, rear 1 frame, the corresponding light intensity value of rear 3 frame;
Solve
By the resolving to phase, the relative altitude of measured object is obtained:
Wherein, h is relative altitude, and N is the corresponding picture frame number of intensity maxima.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610034498.2A CN105606338B (en) | 2016-01-19 | 2016-01-19 | A kind of centre wavelength error compensating method based on white light interference test system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610034498.2A CN105606338B (en) | 2016-01-19 | 2016-01-19 | A kind of centre wavelength error compensating method based on white light interference test system |
Publications (2)
Publication Number | Publication Date |
---|---|
CN105606338A CN105606338A (en) | 2016-05-25 |
CN105606338B true CN105606338B (en) | 2017-06-16 |
Family
ID=55986451
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201610034498.2A Expired - Fee Related CN105606338B (en) | 2016-01-19 | 2016-01-19 | A kind of centre wavelength error compensating method based on white light interference test system |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN105606338B (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109358334B (en) * | 2018-11-09 | 2023-03-14 | 复旦大学 | Nano displacement table precision positioning method based on partially coherent light |
CN112902846B (en) * | 2021-03-22 | 2022-04-19 | 天津大学 | Position coarse acquisition method applied to wavelength modulation anti-vibration interference system |
CN115046469B (en) * | 2022-05-20 | 2023-05-02 | 浙江大学 | Interference fringe envelope extraction method for optical fiber white light interference |
CN116929571A (en) * | 2023-05-06 | 2023-10-24 | 深圳市中图仪器股份有限公司 | Method for measuring center wavelength of white light source |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH1047927A (en) * | 1996-07-31 | 1998-02-20 | Fuji Photo Optical Co Ltd | Method and device for optically measuring air gap |
US7505208B1 (en) * | 2006-02-06 | 2009-03-17 | Raytheon Company | Air-gap optical structure with a nonreflective air-gap spacer |
CN201732177U (en) * | 2009-12-21 | 2011-02-02 | 福建福晶科技股份有限公司 | Novel polarizing and beam-splitting prism |
CN103353390B (en) * | 2013-06-26 | 2015-12-23 | 中国石油大学(华东) | A kind of measuring method of air-gap type ahrens prism gummed error |
-
2016
- 2016-01-19 CN CN201610034498.2A patent/CN105606338B/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
---|---|
CN105606338A (en) | 2016-05-25 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN105571517B (en) | A kind of modified suitable for fiber end inspection is concerned with peak demodulation method | |
CN105606338B (en) | A kind of centre wavelength error compensating method based on white light interference test system | |
CN101581576B (en) | Method for measuring straightness accuracy and position thereof based on double frequency interference principle | |
CN102944169B (en) | A kind of synchronous polarization phase-shifting interferometer | |
CN104330039B (en) | A kind of large-numerical aperture optical fiber point-diffraction interference device and method for three-dimensional coordinates measurement | |
CN105044035B (en) | Refractive index and thickness method for synchronously measuring and system based on spectral domain interferometer | |
CN103454249B (en) | Based on optical glass homogeneity detection method and the device of white light interference | |
CN103471533B (en) | Surface appearance anti-vibration interferometry system | |
CN114061783B (en) | Mach-Zehnder interference-based high-frequency heat release rate pulsating field measuring device and method | |
CN108426530B (en) | Device and method for simultaneously measuring thickness and refractive index of thin film | |
CN105333815B (en) | A kind of super online interferometer measuration system of lateral resolution surface three dimension based on the scanning of spectrum colour loose wire | |
CN102865810B (en) | Orthogonal double-grating based detecting device for synchronous phase shift common-light path interference and detecting method therefor | |
CN113175894A (en) | Object surface three-dimensional shape white light interferometry device and method | |
CN104034272B (en) | A kind of wide spectral light interferometric method measures the system of film thickness | |
CN102353520B (en) | Delay amount measuring method applied for fiber delay line measuring system and realization apparatus thereof | |
WO2018072446A1 (en) | Asymmetric optical interference measurement method and apparatus | |
CN104792269B (en) | A kind of calculation method of the fiber end face height value insensitive to linear phase-shift error | |
CN103196834B (en) | With the interference of light gas detecting system of air-pressure balancing device | |
CN105674875A (en) | Full visual field low frequency heterodyne point diffraction interferometer | |
JP5704150B2 (en) | White interference device and position and displacement measuring method of white interference device | |
CN106091974A (en) | A kind of object distortion measurement instrument, method and apparatus | |
CN110631509B (en) | Object surface curvature detection system and method based on grating Talbot image | |
CN2679644Y (en) | D.C. light inntensity active shock resisting and shifting interferometer | |
CN105928454B (en) | A kind of double optical fiber point-diffraction full filed low frequency heterodyne ineterferometers | |
CN108317962B (en) | Method for measuring thickness and refractive index of common-path self-calibration film for eliminating transmitted light |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20170616 Termination date: 20220119 |
|
CF01 | Termination of patent right due to non-payment of annual fee |