CN100538260C - Micro-displacement high-precision real-time interferometer - Google Patents

Micro-displacement high-precision real-time interferometer Download PDF

Info

Publication number
CN100538260C
CN100538260C CNB2007100372659A CN200710037265A CN100538260C CN 100538260 C CN100538260 C CN 100538260C CN B2007100372659 A CNB2007100372659 A CN B2007100372659A CN 200710037265 A CN200710037265 A CN 200710037265A CN 100538260 C CN100538260 C CN 100538260C
Authority
CN
China
Prior art keywords
circuit
micro
real
high accuracy
chip microcomputer
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
Application number
CNB2007100372659A
Other languages
Chinese (zh)
Other versions
CN101033939A (en
Inventor
何国田
王向朝
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.)
Shanghai Institute of Optics and Fine Mechanics of CAS
Original Assignee
Shanghai Institute of Optics and Fine Mechanics of CAS
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 Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CNB2007100372659A priority Critical patent/CN100538260C/en
Publication of CN101033939A publication Critical patent/CN101033939A/en
Application granted granted Critical
Publication of CN100538260C publication Critical patent/CN100538260C/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Instruments For Measurement Of Length By Optical Means (AREA)

Abstract

A micro-displacement high-precision real-time interferometer comprises a Tyman Green interferometer composed of a semiconductor laser, a collimation beam expander, a beam splitter, a reference flat plate, an object to be measured and a detection element, and is characterized in that: the output end of the detection element is sequentially connected with a real-time signal processing circuit normalization circuit and a single chip microcomputer in series, the single chip microcomputer is provided with phase continuous processing software, the output end of the single chip microcomputer is connected with the input end of an oscilloscope, a direct-current power supply and a signal source are connected with the semiconductor laser through a modulator, and the signal source is further connected with the real-time signal processing circuit. The invention has the advantages of improved displacement measurement precision, expanded measurement range, no need of correction during use, simple operation and high reliability.

Description

Micro-displacement high accuracy real-time interferometry instrument
Technical field
The present invention relates to the displacement interferometer measuring technique, particularly a kind of semiconductor laser micro-displacement high accuracy real-time interferometry instrument that adopts sinusoidal phase modulation.
Background technology
In the optical precision interferometry, the sinusoidal phase modulation interfere measurement technique has higher measuring accuracy, and the displacement measurement precision can reach nanometer scale.Semiconductor laser (being designated hereinafter simply as LD) has characteristics such as volume is little, power-saving, price is low, wavelength-modulated is easy, in the interferometer that adopts light heterodyne technology, realize sinusoidal phase modulation by the injection current of direct modulation LD, not only can improve measuring accuracy, can also make the structure of interferometer more simple.Interferometer (the technology [1] formerly: Takamasa Suzuki that is used for measuring vibrations that proposes such as the Suzuki Xiaochang people such as (Takamasa Suzuki) of Japanese Niigata University, Takao Okada, Osami Sasaki, Takeo Maruyama, " Real-time vibration measurement using a feedback type of laser diodeinterferometer with an optical fiber ", Opt.Eng., 1997,36 (9), 2496-2502), it is simple in structure, and modulation accurately can be treated Measuring Object any position vibration and measure; Do not need reference surface, have the phase compensation function, feedback circuit has been eliminated the extraneous vibration interference; Can obtain vibration displacement in real time.On this basis, people such as the Song Song of Shanghai Optics and Precision Mechanics institute, Chinese Academy of Sciences have proposed another kind of semiconductor laser microvibration real-time interferometer (technology [2]: Song Song formerly, Wang Xiangchao, Wang Xuefeng, cutting edge of a knife or a sword cutting edge of a knife or a sword, Lu Hongbin, " semiconductor laser microvibration real-time interferometer ", optics journal, 2001,21 (5), 578-580; Technology [3] Song Song formerly, Wang Xiangchao, Wang Xuefeng, the cutting edge of a knife or a sword cutting edge of a knife or a sword, Chen Gaoting, " microvibration of adopting locking phase to detect is measured in real time ", and Chinese laser, 2001,28 (8), 753-756).The interference signal of this interferometer converts electric signal to by detecting element, carries out the displacement that data processing obtains vibrating by signal processing circuit.
Technology [2,3] formerly, the wavelength and the intensity of semiconductor laser are respectively:
λ(t)=λ 01Δi(t), (1)
g(t)=β 2[i 0+Δi(t)], (2)
i 0Be the DC component of drive current, Δ i (t) is the AC compounent of drive current, β 1Be wavelength-modulated coefficient, β 2Be intensity modulation coefficient, λ 0Be DC component i 0Corresponding centre wavelength.Modulating current is
Δi(t)=acos(ω 0t+θ) (3)
In the formula: a is the modulating current amplitude.
The detected interference signal of detecting element is
S(t)=S 0(t)+S 1(t)cos[z?cos(ω 0t+θ)+α 0r(t)], (4)
S 0(t) and S 1(t) changed z=4 π β in time by intensity modulation 1β 2AD 0/ λ 0 2Be the sinusoidal phase modulation degree of depth.α in the formula (t) is α 0With α r(t) and.Obtaining detectable signal P (t) after interference signal is handled through signal processing circuit is:
P(t)=KaJ 1(z)sin?α(t), (5)
In the formula: K is the enlargement factor of signal processing circuit, J 1(z) be the 1st rank Bessel's function.
From the above, interference signal obtains phase place α (t) after signal processing circuit is handled, thereby can obtain micro-displacement r (t).Because the light intensity of semiconductor laser is modulated, make S 0(t), S 1(t) change in time, cause measuring error.Simultaneously, the displacement in (5) formula is with initial light path difference 2D 0, circuit enlargement factor K, depth of modulation z be relevant with the Bessel's function value, they are influential to measuring accuracy, will proofread and correct before the test.Formerly technology [1] does not solve the modulated problem of light intensity yet, and intensity modulation causes that the flip-flop of interference signal and AC amplitude composition change in time, have bigger influence to measuring accuracy.
Summary of the invention
The technical problem to be solved in the present invention is to overcome the defective of above-mentioned prior art, and a kind of micro-displacement high accuracy real-time interferometry instrument is provided, and to solve the light intensity variation and interferometer parameter that the directly modulated laser wavelength causes, comprises initial light path difference 2D 0, circuit enlargement factor K, depth of modulation z and Bessel's function value make microdisplacement measurement not need correction, easy to operate to the influence of measuring accuracy, and reliable test result.
Technical solution of the present invention is as follows:
A kind of micro-displacement high accuracy real-time interferometry instrument, comprise by semiconductor laser, the collimator and extender mirror, beam splitter, reference plate, safe graceful Green's interferometer that object to be measured and detecting element are formed, be characterized in: the output termination real time signal processing circuit input end of described detecting element, this real time signal processing circuit output end connects the normalization circuit input end, this normalization circuit output terminal connects the single-chip microcomputer input end, this single-chip microcomputer has the continuous phase process software, the output terminal of this single-chip microcomputer links to each other with oscillographic input end, direct supply is connected with described semiconductor laser by modulator with signal source, and described signal source also is connected with described real time signal processing circuit.
Described beam splitter is that incident light is divided into the element of two-beam by 1: 1 light intensity, and the parallel flat of being analysed the light film by Amici prism or one side plating constitutes.
Described reference plate is an optical flat, and its one side near beam splitter is coated with highly reflecting films.
Described detecting element is photodiode or photoelectric cell or photomultiplier.
Described real time signal processing circuit is by two amplifiers, a multiplier), wave filter constitutes.
Described normalization circuit is made of power operation circuit, filtering circuit, extracting operation circuit and division arithmetic circuit polyphone.
The function that described single-chip microcomputer calculates and oscillograph shows is finished by a computing machine.
Advantage of the present invention:
1), eliminated the influence of light intensity.In the prior art, during the wavelength of directly modulated laser, the output intensity of semiconductor laser changes in time, and measured displacement is obtained according to this light intensity, so measuring error has been introduced in the variation of output intensity.The present invention utilizes normalization circuit to eliminate the influence of light intensity to measuring accuracy.
2), technology [2] formerly, can't accurately measure initial light path difference 2D 0, therefore can not accurately obtain the Bessel's function value.Need during use to proofread and correct, this correctly uses this instrument to bring difficulty for the user.The present invention has eliminated initial light path difference 2D 0Influence, make the operation of interferometer more simple.
3), technology [2] formerly, the circuit enlargement factor can't accurately be measured, and the circuit enlargement factor will change with variation of ambient temperature.The present invention has eliminated the influence of circuit enlargement factor to measuring accuracy.
4), the anti-external interference ability of method of the present invention is strong.
5), measurement range of the present invention exceeds half wavelength, enlarged measurement range.
Description of drawings
Fig. 1 is micro-displacement high accuracy real time interferometer example structure figure of the present invention.
Fig. 2 is the signal flow graph of real time signal processing circuit of the present invention and normalization circuit.
Embodiment
The invention will be further described below in conjunction with embodiment and accompanying drawing, but should not limit protection scope of the present invention with this.
See also Fig. 1 earlier, Fig. 1 is a micro-displacement high accuracy real time interferometer embodiment structural representation of the present invention.As seen from the figure, micro-displacement high accuracy real time interferometer of the present invention has on the semiconductor laser 1 emission light beam working direction of direct supply 11 and is placed with lens 2 successively with optical axis, beam splitter 3, object 5 to be measured; Place reference plate 4 on the folded light beam f1 working direction of this beam splitter 3.Light beam f1 is placed with detecting element 6 on reference plate 4 beam reflected f2 working direction, constitute safe graceful Green's interferometer, what contact successively with detecting element 6 is real time signal processing circuit 7, normalization circuit 8, single-chip microcomputer 9, shows measurement results by oscillograph 10 at last.Direct supply 11, signal source 12 are connected with modulator 13.Signal source 12 also is connected with real time signal processing circuit 7.Semiconductor laser 1 is connected with modulator 13.
In the present embodiment, described semiconductor laser 1 is that centre wavelength is the semiconductor laser of 785nm.Described beam splitter 3 is by the Amici prism that is divided into two-beam at 1: 1 with light intensity.Described reference plate 4 is gold-plated level crossings.Described detecting element 6 is photodiodes.
Described real time signal processing circuit 7 is by first amplifying circuit 701, second amplifying circuit 702, mlultiplying circuit 703, and filtering circuit 704 constitutes.First amplifying circuit 701 is made of chip LM232, and second amplifying circuit 702 is made of chip LM232.Mlultiplying circuit 703 is made of chip AD532, and filtered electrical router chip LF356 and follower BC108 constitute.
Described normalization circuit 8 is made of power circuit 801, filtering circuit 802, evolution circuit 803, division circuit 804.Power circuit 801 is made of the identical chip AD532 of two-way input.Filtering circuit 802 is pi type filters.Evolution circuit 803 is made of chip LM232.Division circuit 804 is made of chip AD538.
Described single-chip microcomputer 9 is that a model is the single-chip microcomputer of ADuc812.Described oscillograph 10 is one to have the digital oscilloscope of memory function.Described signal source 12 is signal generators.Described modulator 13 is laser current modulators.
The course of work of micro-displacement high accuracy real time interferometer of the present invention is: semiconductor laser 1 is driven by direct supply 11, the sinusoidal signal modulation that the wavelength of semiconductor laser 1 is exported by signal generator 12.The light beam that semiconductor laser 1 sends shines on the Amici prism 3 behind collimator and extender mirror 2 collimator and extenders, and a branch of light is divided into two-beam, and folded light beam f1 shines on the reference plate 4, and another transmitted light beam t1 shines on the object 5 to be measured.The interference signal that reference planes mirror 4 and object to be measured 5 beam reflected f2 and t2 produce converts electric signal to by detecting element 6, and this interference signal is
S(t)=S 0(t)+S 1(t)cos[z?cos(ω 0t+θ)+α 0+α(t)], (6)
α 0=4πD 00, (7)
α(t)=4πr(t)/λ 0, (8)
2D 0Be two optical path differences of interfering between the arm of the graceful interferometer of described Thailand, the micro-displacement of r (t) expression object 5 to be measured.In Fig. 2, above-said current signal S (t) and modulation signal α cos (ω cT+ θ) (gain is respectively K to amplify the back through first amplifier 701, second amplifier 702 in the signal processing circuit 7 respectively 1, K 2), (coefficient is K to carry out multiplying by computing and filtering circuit 703 c) (gain is K with low-pass filtering L) after obtain detectable signal P (t)
P s(t)=K 1K 2K cK LS 1AJ 1(z)sin?α(t)=K ssin?α(t), (9)
K wherein s=K 1K 2K cK LS 0AJ 1(z); A is the amplitude of the sinusoidal phase modulation voltage signal of signal generator 12 outputs.
Detectable signal P (t) through the power circuit 801 of normalization circuit 8 as power is
P 1 ( t ) = K s 2 sin 2 α ( t ) . - - - ( 10 )
If the frequency of α (t) is ω, selecting cutoff frequency for use is that the low-pass filtering 802 of 1.5 ω gets as filtering operation,
P 2 ( t ) = K s 2 , - - - ( 11 )
With 803 couples of P of evolution circuit 2(t) get as extracting operation
P 3(t)=K s, (12)
To (9) formula and (12) formula division arithmetic, obtain measured signal P (t) by division circuit 804
P(t)=sinα(t)。(13)
Its signal Processing block diagram is as shown in Figure 2.
With measured signal P (t) input single-chip microcomputer 9, this single-chip microcomputer 9 has continuous phase to be handled (referring to technology [4] Wang Xuefeng formerly, Wang Xiangchao etc., be used for the semiconductor laser interference instrument that the nano-precision large range displacement is measured, Chinese laser, 2001,28 (5)) software of computing method establishment, handle to calculate phase place α (t) through continuous phase, calculate measured displacement again and be
r(t)=mπ/4+λ 0α(t)/(4π)。(14)
Wherein m is an integer.The measuring accuracy of phase place can reach 0.001rad, and the resolution of measurement is 0.1nm, and has enlarged range of displacement measurement.
By (13) formula as can be seen, the light intensity of measuring-signal P (t) and semiconductor laser 1 output changes irrelevant, and light intensity changed the influence to measurement result when wavelength-modulated had fundamentally been eliminated in the displacement that obtains from (14) formula.Measuring-signal P (t) and measurement parameter are as the two initial light path difference 2D that interfere between the arm 0, circuit enlargement factor K 1, K 2, K c, K L, depth of modulation z and Bessel's function value be irrelevant.
This shows that the present invention has improved the displacement measurement precision, its measurement range surpasses one more than the wavelength, does not need during use to proofread and correct, and is easy and simple to handle, the reliability height.

Claims (7)

1, a kind of micro-displacement high accuracy real-time interferometry instrument, comprise safe graceful Green's interferometer of forming by semiconductor laser (1), collimator and extender mirror (2), beam splitter (3), reference plate (4), object to be measured (5) and detecting element (6), it is characterized in that:
Output termination real time signal processing circuit (7) input end of described detecting element (6), this real time signal processing circuit (7) output termination normalization circuit (8) input end, this normalization circuit (8) output terminal connects single-chip microcomputer (9) input end, this single-chip microcomputer (9) has the continuous phase process software, the output terminal of this single-chip microcomputer (9) links to each other with the input end of oscillograph (10), direct supply (11) is connected with described semiconductor laser (1) by modulator (13) with signal source (12), and described signal source (12) also is connected with described real time signal processing circuit (7).
2, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described beam splitter (3) is that incident light is divided into the element of two-beam by 1: 1 light intensity, and the parallel flat of being analysed the light film by Amici prism or one side plating constitutes.
3, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described reference plate (4) is an optical flat, and its one side near beam splitter is coated with highly reflecting films.
4, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described detecting element (6) is photodiode or photoelectric cell or photomultiplier.
5, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described real time signal processing circuit (7) is made of two amplifiers (701,702), a multiplier (703) and a wave filter (704).
6, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described normalization circuit (8) is made of power operation circuit (801), filtering circuit (802), extracting operation circuit (803) and division arithmetic circuit (804) polyphone.
7, micro-displacement high accuracy real-time interferometry instrument according to claim 1 is characterized in that described single-chip microcomputer (9) calculates and the function of oscillograph (10) demonstration is finished by a computing machine.
CNB2007100372659A 2007-02-07 2007-02-07 Micro-displacement high-precision real-time interferometer Expired - Fee Related CN100538260C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB2007100372659A CN100538260C (en) 2007-02-07 2007-02-07 Micro-displacement high-precision real-time interferometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB2007100372659A CN100538260C (en) 2007-02-07 2007-02-07 Micro-displacement high-precision real-time interferometer

Publications (2)

Publication Number Publication Date
CN101033939A CN101033939A (en) 2007-09-12
CN100538260C true CN100538260C (en) 2009-09-09

Family

ID=38730599

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB2007100372659A Expired - Fee Related CN100538260C (en) 2007-02-07 2007-02-07 Micro-displacement high-precision real-time interferometer

Country Status (1)

Country Link
CN (1) CN100538260C (en)

Families Citing this family (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101625233B (en) * 2009-08-05 2010-12-29 富美科技有限公司 Installation detecting system of cleaning scraper blade
CN101907443B (en) * 2010-06-23 2012-03-07 清华大学 Displacement measuring device for movable mutual inductor of energy balance
CN104048588B (en) * 2014-06-25 2017-07-14 中国科学院长春光学精密机械与物理研究所 Capacity plate antenna calibration device for displacement sensor
CN104597316A (en) * 2015-01-08 2015-05-06 聚光科技(杭州)股份有限公司 Weak current detecting device and method
CN108680107A (en) * 2018-05-16 2018-10-19 中北大学 A kind of high-precision prism displacement measuring device and method based on digital servo-control
CN109631767B (en) * 2018-12-12 2020-11-24 上海卫星装备研究所 Distance measuring method
CN109470152A (en) * 2018-12-18 2019-03-15 华中科技大学 A kind of cantilever beam microdisplacement measurement method and system
CN110017793B (en) * 2019-04-10 2020-09-18 南京理工大学 Double-channel anti-vibration interference measurement device and method
CN110987373B (en) * 2019-12-04 2021-08-10 北京自动化控制设备研究所 Method and device for measuring phase modulation depth of interference type optical fiber sensor

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5532479A (en) * 1993-11-11 1996-07-02 Goldstar Co., Ltd. Temperature, pressure, vibration or humidity sensor based on reflected light from a bimetallic, plastic or dehumidifying material
CN1166734A (en) * 1996-03-27 1997-12-03 三星电子株式会社 Normalization circuit for preventing divergence of normalizing voltage in coupler used for diversity operation
US6128083A (en) * 1998-04-08 2000-10-03 Sony Precision Technology Inc. Displacement measuring apparatus
CN1280293A (en) * 2000-08-03 2001-01-17 中国科学院上海光学精密机械研究所 Method for measuring nanometer precision of object displacement
CN1281970A (en) * 1999-07-23 2001-01-31 中国科学院上海光学精密机械研究所 Micro-displacement interferometer using semiconductor laser
CN1431478A (en) * 2003-02-14 2003-07-23 中国科学院上海光学精密机械研究所 Micro-displacement real-time interferometer
CN1563890A (en) * 2004-03-30 2005-01-12 中国科学院上海光学精密机械研究所 Double-sine phase modulation real-time interference range finder
JP2005283520A (en) * 2004-03-31 2005-10-13 Iai:Kk Displacement measuring device
CN201016705Y (en) * 2007-02-07 2008-02-06 中国科学院上海光学精密机械研究所 Micro-displacement high-precision real-time interference measuring device

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5532479A (en) * 1993-11-11 1996-07-02 Goldstar Co., Ltd. Temperature, pressure, vibration or humidity sensor based on reflected light from a bimetallic, plastic or dehumidifying material
CN1166734A (en) * 1996-03-27 1997-12-03 三星电子株式会社 Normalization circuit for preventing divergence of normalizing voltage in coupler used for diversity operation
US6128083A (en) * 1998-04-08 2000-10-03 Sony Precision Technology Inc. Displacement measuring apparatus
CN1281970A (en) * 1999-07-23 2001-01-31 中国科学院上海光学精密机械研究所 Micro-displacement interferometer using semiconductor laser
CN1280293A (en) * 2000-08-03 2001-01-17 中国科学院上海光学精密机械研究所 Method for measuring nanometer precision of object displacement
CN1431478A (en) * 2003-02-14 2003-07-23 中国科学院上海光学精密机械研究所 Micro-displacement real-time interferometer
CN1563890A (en) * 2004-03-30 2005-01-12 中国科学院上海光学精密机械研究所 Double-sine phase modulation real-time interference range finder
JP2005283520A (en) * 2004-03-31 2005-10-13 Iai:Kk Displacement measuring device
CN201016705Y (en) * 2007-02-07 2008-02-06 中国科学院上海光学精密机械研究所 Micro-displacement high-precision real-time interference measuring device

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Real-time vibration measurement using a feedback type of laser diode interferometer with an optical fiber. Takamasa Suzuki,Takao Okada,Osami Sasaki,etc.Optical Engineering,Vol.36 No.9. 1997 *
半导体激光微小振动实时干涉测量仪. 宋松,王向朝,王学锋,钱锋,卢洪斌.光学学报,第21卷第5期. 2001 *

Also Published As

Publication number Publication date
CN101033939A (en) 2007-09-12

Similar Documents

Publication Publication Date Title
CN100538260C (en) Micro-displacement high-precision real-time interferometer
US10641600B2 (en) Real-time normalization apparatus and method of phase generated carrier demodulation in sinusoidal phase modulation interferometer
CN110411335B (en) Differential sine phase modulation laser interference nano displacement measuring device and method
CN102564564A (en) Non-contact micro-vibration measuring system based on non-equilibrium Michelson fiber-optic interferometer
CN103075969B (en) Differential laser interference nano-displacement measurement method and differential laser interference nano-displacement measurement apparatus
CN109059754B (en) Laser self-mixing interference measuring device and measuring method
CN102353341B (en) Phase-modulating synchronous-integral phase-shifting interference-measuring method and device
CN103528511A (en) Sinusoidal phase modulation type laser self-mixing interferometer and measuring method thereof
CN201016705Y (en) Micro-displacement high-precision real-time interference measuring device
CN101290215B (en) Micro-displacement sensor based on PGC demodulated interferential scanning
CN102168944A (en) Double-frequency laser interferometer for absolute distance measurement and measuring method thereof
CN100464153C (en) Real-time interference measurement device and method for nanometer precision of object surface appearance
CN108775954A (en) A kind of adjustable dual wavelength LD of resolution ratio is from mixing vibration measuring instrument and its measurement method
CN104330147A (en) Micro-cantilever thermal shock signal measuring apparatus
CN110879040B (en) Displacement measurement method of Michelson heterodyne interferometer based on double acousto-optic modulator
CN104535535B (en) A kind of apparatus for measuring refractive index and method based on self-mixed interference
CN100547344C (en) Sine phase modulation interferometer for real-time measurement of surface topography
CN110118532B (en) Dual-wavelength nonlinear displacement demodulation method and system of fiber Fabry-Perot displacement sensor
CN102288387B (en) Method for measuring modulation depth of semiconductor laser sine phase modulation interferometer
CN201003946Y (en) Real-time interference measuring device for object surface appearance nanometer precision
CN201548201U (en) Vibration-resistant dynamic interferometer
CN102252622A (en) Device and method for measuring glass thickness by adopting sinusoidal modulation multi-beam laser heterodyning of Doppler galvanometer
CN112304225B (en) Symmetrical semiconductor laser self-mixing grating interference three-dimensional displacement measurement system and measurement method thereof
CN108627084B (en) Laser instrument wavelength calibration system based on static michelson interferometer
CN101706253B (en) Filtering phase discriminator type dynamic interferometry system

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
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20090909

Termination date: 20120207