CN106338334B - A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device - Google Patents

A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device Download PDF

Info

Publication number
CN106338334B
CN106338334B CN201610850354.4A CN201610850354A CN106338334B CN 106338334 B CN106338334 B CN 106338334B CN 201610850354 A CN201610850354 A CN 201610850354A CN 106338334 B CN106338334 B CN 106338334B
Authority
CN
China
Prior art keywords
light
phase
polarization converter
polarization
polarizing beam
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.)
Active
Application number
CN201610850354.4A
Other languages
Chinese (zh)
Other versions
CN106338334A (en
Inventor
张志伟
郑宾
张文静
郭华玲
刘利平
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.)
North University of China
Original Assignee
North University of China
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 North University of China filed Critical North University of China
Priority to CN201610850354.4A priority Critical patent/CN106338334B/en
Publication of CN106338334A publication Critical patent/CN106338334A/en
Application granted granted Critical
Publication of CN106338334B publication Critical patent/CN106338334B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
  • Instruments For Measurement Of Length By Optical Means (AREA)

Abstract

A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device, is mainly characterized by efficiently utilizing luminous energy, is suitable for Weak absorption, can get vibration and the frequency spectrum of micro-vibration, the phase generated using the amplitude that Suo Lieer-Babinet phase compensator obtains micro-vibration;It is compared using reference path with optical path, greatly reduces the common-mode noise generated by environmental factor variation, improve measurement accuracy;The phase-conjugation light with phase compensation characteristic generated using photorefractive crystal eliminates " the speckle noise " of the generation of testee surface, and the surface of testee is expanded to relatively rough surface by being similar to mirror surface;Orthogonal two beams crossed polarized light is obtained using alliteration optical modulator, eliminates the influence of acousto-optic modulator intensity modulation, it is easy to accomplish the high-precision measurement of amplitude;The beat frequency of alliteration optical modulator is middle frequency difference, realizes low frequency signal in the processing of radio-frequency region, eliminates the interference of low-frequency noise.

Description

A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device
Technical field
It is a kind of based on laser, alliteration optical modulator and photorefractive crystal characteristic the invention belongs to physical optical arts And a kind of dual-acousto-optic phase modulation proposed is conjugated optical heterodyne detection device.
Background technique
Optical heterodyne detection technology has very high sensitivity compared with incoherent technique, and measurement accuracy wants high 7-8 A order of magnitude, therefore had a wide range of applications in signal detection;But the interference signal of high s/n ratio in order to obtain, it is right The smoothness requirements on testee surface be it is relatively high, in general closer to shiny surface more be conducive to improve signal-to-noise ratio.It is right In coarse testee surface, a large amount of " speckle noise " is carried in reflected light, this brings larger to high-acruracy survey Difficulty.
The sub-nm resolution phase conjugation interference of Chinese invention patent, a kind of object vibration amplitude of ZL00115304.8 is surveyed Device is measured, including in the direction of advance of source emissioning light beam, being successively equipped with the first lens, the second lens, beam splitter, polarization point Beam device, polarisation transformer to testee.By the light beam with dapple noise of testee first reflection through polarization beam splitting After device reflection, photorefractive crystal is converged to by the 4th lens.The phase-conjugation light that photorefractive crystal generates is anti-by polarization beam apparatus It is mapped to testee, the phase-conjugation light of testee reflection is no longer with dapple noise.This is that one kind is not only suitable for surface Smooth testee, and be also applied for shaggy testee, measure the resolution ratio of vibration amplitude less than 5 × 10-10Rice.
This vibration measuring method is disadvantageous in that without reference path, cannot utilize radio-frequency technique processing phase (amplitude) Signal.Accordingly, it is difficult to eliminate the interference of common-mode noise caused by environmental factor and low-frequency noise (also referred to as 1/f noise).
Summary of the invention
It is existing based on optical interferometry object vibration method and to be solved the purpose of the present invention is overcoming the shortcomings of Technical problem provides a kind of phase conjugation heterodyne spy using green (light) laser, alliteration optical modulator and photorefractive crystal composition Survey new equipment.
To achieve the purpose of the present invention, the technical solution of the present invention is as follows:
A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device, it is characterised in that: orthogonal including generating two beams Cross-polarization electro-optical device, phase reference device, micro-vibration amplitude (phase) measuring device and data acquisition and procession display dress It sets;The micro-vibration phase amplitude measurement device, by a beam expander 14, two polarizing beam splitters, i.e. the first polarization spectro Device 15, the second polarizing beam splitter 24, three polarization converters, i.e. the first polarization converter 16, the second polarization converter 22 and Three polarization converters 25, two biconvex lens, i.e. the first biconvex lens 19 and the second biconvex lens 27, the second analyzer 18, one A half-wave plate 23, the injection device 17 that is all-trans, the second photodetector 20 and a photorefractive crystal 28 form;Wherein:
● the orthogonal cross-polarization electro-optical device of two beam of generation includes a laser 1, a polarised light point Light device 2, two total reflection right-angle prisms, i.e., the first total reflection right-angle prism 3 and the second total reflection right-angle prism 6, two drivings Frequency is respectively f1And f2Acousto-optic modulator, i.e. first sound-optic modulator (4) and second sound-optic modulator 5 and polarization close Light device 7;
● the phase reference device includes an optical splitter 8, the first analyzer 9, third biconvex lens 10 and first Photodetector 11;
● the data acquisition and processing (DAP) device includes two bandpass filters, i.e. the first bandpass filter 12 and the Two band-pass filter 21,16 oscillograph cards 13 of a binary channels and a set of computer system 29;
● the laser beam issued by laser 1 is divided into two bunch polarised lights through third polarised light splitter 2: a branch of is p light (i.e. light vector direction of vibration be parallel to the plane of incidence polarised light), another beam are that (i.e. light vector direction of vibration is perpendicular to incidence for s light The polarised light in face).It is f that p light, which enters driving frequency by the first total reflection right-angle prism 3,1First sound-optic modulator 4, s light is logical Frequency of overdriving is f2Second sound-optic modulator 5 after, generate two 0 grade of diffraction lights and two+1 grade of diffraction lights, driving respectively Frequency is f2Second sound-optic modulator 5+1 grade of diffraction light by second total reflection right-angle prism 6 and driving frequency be f1? + 1 grade of diffraction light of one acousto-optic modulator 4 enters polarization splicer 7, and synthesis light beam is by the transmitted light beam of optical splitter 8 by the After one analyzer 9, interfered on the photosurface of the first photodetector 11 by third biconvex lens 10, and be converted to Beat frequency is the electric signal of middle frequency difference, phase reference signal of the electric signal of the middle frequency difference as system, through the first bandpass filtering Device 12 filters, and becomes digital signal into 16 oscillograph cards 13 of binary channels;
Light beam is synthesized by the reflected beams of optical splitter 8 by after beam expander 14, into the first polarizing beam splitter 15, Middle s light is reflected and is totally reflected later by the injection device 17 that is all-trans that the first polarization converter 16 reaches regulating reflection degree, should Reflected light becomes p light again by the first polarization converter 16, and penetrates the first polarizing beam splitter 15 and the second analyzer 18 Later, it is focused on by the first biconvex lens 19 on the photosurface of second photodetector 20;Through the p of the first polarizing beam splitter 15 Light penetrates the second polarizing beam splitter 24 by being still p light after the second polarization converter 22 and half-wave plate 23, later by the Three polarization converters 25 reach 26 surface of testee and are totally reflected, which carries " speckle noise " again by third Polarization converter 25 becomes s light and is reflected by the second polarizing beam splitter 24, by converging to Preset grating after the second biconvex lens 27 On crystal 28, the phase-conjugation light generated by photorefractive crystal 28, by the second polarization spectro after being collimated by the second biconvex lens 27 The another secondary reflection of device 24, and reach 26 surface of testee through third polarization converter 25 and be totally reflected, reflected phase Position conjugate beam becomes p light after third polarization converter 25, and partially by the second polarizing beam splitter 24, half-wave plate 23 and second Become s light after vibration converter 22, is reflected by the first polarizing beam splitter 15 and by the second analyzer 18 by the first biconvex lens 19 focus on the photosurface of the second photodetector 20, occur with the p light on the photosurface of arrival photodetector 20 before Interference, and be converted to the electric signal that beat frequency is middle frequency difference, measuring signal of the electric signal of the middle frequency difference as system, through second Bandpass filter (21) filtering, becomes digital signal into 16 oscillograph cards 13 of binary channels;
The digital signal passes through processing of the computer system 29 to reference signal and measuring signal data, obtains micro-vibration Amplitude, the spectrum value of signal.
The present invention compared with prior art, has substantive distinguishing features outstanding and significant effect are as follows:
The present invention can efficiently utilize luminous energy, be suitable for Weak absorption, can get the amplitude and spectrum information of micro-vibration, The phase generated using the amplitude that Suo Lieer-Babinet phase compensator obtains micro-vibration;Utilize reference path and measurement light Road compares, and significantly reduces the common-mode noise generated by environmental factor variation, improves measurement accuracy.
The phase-conjugation light with phase compensation characteristic that the present invention utilizes photorefractive crystal to generate, eliminates testee " the speckle noise " generated, the surface of testee is expanded to relatively rough surface by being similar to mirror surface;Utilize dual-acousto-optic tune Device processed obtains orthogonal two beams crossed polarized light, eliminates the influence of acousto-optic modulator intensity modulation, it is easy to accomplish amplitude High-precision measurement;The beat frequency of alliteration optical modulator is middle frequency difference, realizes low frequency signal in radio-frequency region processing, eliminates The interference of low-frequency noise (1/f noise).
Present invention is mainly used for the micro-vibrations of measurement object, be both suitable for the smooth object in surface, it is thick to be also suitable for surface Rough object.
Detailed description of the invention
Fig. 1 is a kind of schematic illustration of dual-acousto-optic phase modulation conjugation heterodyne detection device;
Fig. 2 is the waveform diagram of the reference path that beat frequency is 30MHz and optical path;
Fig. 3 is the demodulation result that the vibration frequency of testee aluminium sheet is the micro-vibration of 6kHz.
In Fig. 1: laser 1, the first polarizing beam splitter 15, the second polarizing beam splitter 24 and third polarizing beam splitter 2, first Right angle total reflection prism 3 and the second right angle total reflection prism 6, first sound-optic modulator 4 and second sound-optic modulator 5, polarization close Light device 7, optical splitter 8, the first analyzer 9 and the second analyzer 18, the first biconvex lens 19, the second biconvex lens 27 and third are double Convex lens 10, the first photodetector 11 and the second photodetector 20, the first bandpass filter 12 and the second bandpass filter 21,16 oscillograph cards 13 of binary channels, beam expander 14, the first polarization converter 16, the second polarization converter 22, third optical rotation Parallel operation 25, be all-trans injection device 17, half-wave plate 23, testee 26, photorefractive crystal 28, computer system 29.
Specific embodiment
Below in conjunction with Detailed description of the invention specific implementation method of the present invention.
Shown in Fig. 1, a kind of dual-acousto-optic phase modulation of the present invention is conjugated heterodyne detection device, including generates two beams and be mutually perpendicular to Cross-polarization electro-optical device, phase reference device, micro-vibration amplitude (phase) measuring device and data acquisition and procession show Device, it is characterised in that: described micro-vibration amplitude (phase) measuring device is a kind of to eliminate testee surface reflection In include " speckle noise " device, the dress that " the speckle noise " that includes in testee surface reflection can be eliminated It sets, by a beam expander 14, two polarizing beam splitters, i.e. the first polarizing beam splitter 15 and the second polarizing beam splitter 24, three partially Shake converter, i.e. the first polarization converter 16, the second polarization converter 22 and third polarization converter 25, two biconvex lens, That is the first biconvex lens 19 and the second biconvex lens 27, the second analyzer 18, a half-wave plate 23, the injection device 17 that is all-trans, Second photodetector 20 and a photorefractive crystal 28 form;Wherein:
● the orthogonal cross-polarization electro-optical device of two beam of generation includes a laser 1, a polarised light point Light device 2, two total reflection right-angle prisms, i.e., the first total reflection right-angle prism 3 and the second total reflection right-angle prism 6, two drivings Frequency is respectively f1And f2Acousto-optic modulator, i.e. first sound-optic modulator (4) and second sound-optic modulator 5 and polarization close Light device 7;
● the phase reference device includes an optical splitter 8, the first analyzer 9, third biconvex lens 10 and first Photodetector 11;
● the data acquisition and processing (DAP) device includes two bandpass filters, i.e. the first bandpass filter 12 and the Two band-pass filter 21,16 oscillograph cards 13 of a binary channels and a set of computer system 29;
● the laser beam issued by laser 1 is divided into two bunch polarised lights through third polarizing beam splitter 2: a branch of is p light, separately A branch of is s light.It is f that p light, which enters driving frequency by the first total reflection right-angle prism 3,1First sound-optic modulator 4, s light passes through Driving frequency is f2Second sound-optic modulator 5 after, generate two 0 grade of diffraction lights and two+1 grade of diffraction lights, driving frequency respectively Rate is f2Second sound-optic modulator 5+1 grade of diffraction light by second total reflection right-angle prism 6 and driving frequency be f1First + 1 grade of diffraction light of acousto-optic modulator 4 enters polarization splicer 7, and synthesis light beam passes through first by the transmitted light beam of optical splitter 8 After analyzer 9, interfered on the photosurface of the first photodetector 11 by third biconvex lens 10, and be converted to bat Frequency is the electric signal of middle frequency difference, phase reference signal of the electric signal of the middle frequency difference as system, through the first bandpass filter 12 filtering, become digital signal into 16 oscillograph cards 13 of binary channels;
Light beam is synthesized by the reflected beams of optical splitter 8 by after beam expander 14, into polarization beam apparatus 15, wherein s Light is reflected and is totally reflected later by the injection device 17 that is all-trans that the first polarization converter 16 reaches regulating reflection degree, the reflection Light becomes p light again by the first polarization converter 16, and after the first polarizing beam splitter 15 of transmission and the second analyzer 18, It is focused on by the first biconvex lens 19 on the photosurface of second photodetector 20;It is logical through the p light of the first polarizing beam splitter 15 Crossing after the second polarization converter 22 and half-wave plate 23 is still p light, and penetrates the second polarizing beam splitter 24, inclined by third later Vibration converter 25 reaches 26 surface of testee and is totally reflected, which carries " speckle noise " again by polarization Device 25 becomes s light and is reflected by factory's polarizing beam splitter 24, by being converged on photorefractive crystal 28 after the second biconvex lens 27, The phase-conjugation light generated by photorefractive crystal 28, after being collimated by the second biconvex lens 27 again by the second polarizing beam splitter 24 Reflection, and reach 26 surface of testee through third polarization converter 25 and be totally reflected, reflected phase-conjugation light warp Become p light after crossing third polarization converter 25, and passes through the second polarizing beam splitter 24, half-wave plate 23 and the second polarization converter 22 Become s light later, reflected by the first polarizing beam splitter 15 and focuses on the by the first biconvex lens 19 by the second analyzer 18 On the photosurface of two photodetectors 20, with reach the second photodetector 20 before photosurface on p light interfere, and The electric signal that beat frequency is middle frequency difference is converted to, measuring signal of the electric signal of the middle frequency difference as system is filtered through the second band logical Wave device 21 filters, and becomes digital signal into 16 oscillograph cards 13 of binary channels.By computer system 29 to reference signal and The processing of measuring signal data obtains amplitude, the spectrum value of micro-vibration signal.
It is interfered on the photosurface of first photodetector 11, the first bandpass filter 12 filters out direct current therein After item, optical frequency item, the electric signal of output be can be written as
In formula, Δ ω=ω21Δ θ=θ21, ω2With ω1Respectively second sound-optic modulator 5 With the frequency displacement of+1 grade of diffraction light of first sound-optic modulator 4,WithRespectively in reference path, second sound-optic modulator 5 The phase of 11 photosurface of the first photodetector, θ are reached with+1 grade of diffraction light of first sound-optic modulator 42With θ1Respectively second The initial phase of acousto-optic modulator 5 and first sound-optic modulator 4.
It is interfered on the photosurface of second photodetector 20, the second bandpass filter 21 filters out direct current therein After item, optical frequency item, the electric signal of output be can be written as
In formula, WithRespectively in optical path, second sound-optic modulator 5 and the first acousto-optic + 1 grade of diffraction light of modulator 4 reaches the phase of 20 photosurface of the second photodetector, remaining same formula of parameter meaning (1).
When the driving frequency of second sound-optic modulator 5 is 110.12MHz, the driving frequency of first sound-optic modulator 4 is When 80MHz, frequency difference between the two is 30.12MHz, and the waveform of laser heterodyne interferometry signal is as shown in Fig. 2, wherein the channel CH1 is Reference signal, the channel CH2 are measuring signals.
If in optical path, the equivalent optical path of s light and p light then comes when testee surface has micro-vibration to be displaced s (t) The phase shift of (4 π/λ) s (t) will be generated from the signal light of testee surface reflection, wherein λ is optical wavelength, at this moment the second photoelectricity The expression formula of 20 photoelectric current of detector is
Im∝cos[Δωt+(4π/λ)s(t)+Δθ] (3)
In formula, Δ ω and the same formula of Δ θ meaning (1).The photoelectric current provided in formula (1) and (3) is converted to quilt after voltage (selected photodetector is photoelectric converter, current-to-voltage converting circuit and voltage amplifier circuit in the present invention for amplification Integrate), and be respectively the first bandpass filter 12 and the second bandpass filter 21 of beat frequency, filtering by centre frequency Voltage afterwards, which is sent to 16 oscillograph cards 13 of binary channels, which carries out analog-to-digital conversion, becomes digital signal, which is deposited Storage is used for data processing and display in computer system 29.
In specific implementation, the splitting ratio of optical splitter 8 is 70:30 (reflective light intensity: transmitted light intensity), the first analyzer 9 and the The extinction ratio of two analyzers 18 is greater than 10000:1, and the first polarization converter 16 uses quarter wave plate, the choosing of the second polarization converter 22 With Faraday polarization apparatus, third polarization converter 25, which is selected, uses quarter wave plate, and beam expander 14 uses 5 times of beam expanders, and Preset grating is brilliant Body 28 selects barium titanate crystal, and the injection device 17 that is all-trans is total reflection right-angle prism either prism of corner cube;The intensity of s light and p light It can change by adjusting the Linear Control voltage of first sound-optic modulator 4 and second sound-optic modulator 5;In computer system 29 Control and calculation procedure equipped with data sampling and processing and display, these programs include micro-vibration waveform drawing and amplitude, phase The functions such as position and frequency spectrum calculating.
It is the waveform diagram of reference path and optical path that beat frequency is 30.12MHz, wherein measuring signal is opposite shown in Fig. 2 The phase of reference signal is π/4, and electric signal of the channel CH1 from the first photodetector 11 is reference signal, and the channel CH2 is come It is measuring signal from the electric signal of the second photodetector 20.By adjusting the injection device 17 that is all-trans in specific implementation, so that measurement Signal is 0 (or integral multiple of 2 π) with respect to the phase of reference signal, that is, makes the waveform of reference path and optical path Strictly coincide together.Reference signal and measuring signal are sampled respectively, then pass through data processing, and the phase of the two can be obtained Potential difference.
It is the demodulation result that the vibration frequency that testee 26 is aluminium sheet is the micro-vibration of 6kHz shown in Fig. 3.Wherein Fig. 3 It (a) is the vibrational waveform figure of demodulation, Fig. 3 (b) is the result of spectrum analysis of vibrational waveform.In specific implementation, quilt shown in FIG. 1 One end (rigid connection) that object 26 (aluminium sheet) is fixed on Piezoelectric Ceramic bar is surveyed, then drive power supply for piezoelectric ceramics is set Driving voltage and driving frequency make testee make micro-vibration by certain frequency and amplitude, to reference signal and measuring signal It samples respectively, data processing is carried out to sampled value, vibrational waveform and rumble spectrum can be obtained.For example, Piezoelectric Ceramic is electric Pressure is 1.8 volts, and when driving frequency is 6kHz, demodulation result shown in Fig. 3 can be obtained, from Piezoelectric Ceramic voltage and displacement The table of comparisons, it is known that its vibration amplitude is about 170 nanometers.
Using Suo Lieer-Babinet phase compensator, having surveyed testee 26 is shaggy aluminium sheet micro-vibration The phase that amplitude generates, and amplitude is scaled by formula (3), its amplitude discrimination is obtained by phase resolution.For example, laser Output wavelength is 633nm, the injection device 17 that is all-trans is the girdle prisms such as right angle, and photodetector 11 and 20 is silicon substrate across resistance amplification photoelectricity Detector, the resolution ratio of the present apparatus is up to 2.76 × 10-12Rice.

Claims (5)

1. a kind of dual-acousto-optic phase modulation is conjugated heterodyne detection device, it is characterised in that: orthogonal just including generating two beams Hand over polarized light device, phase reference device, micro-vibration phase amplitude measurement device and data acquisition and procession display device; The micro-vibration phase amplitude measurement device, by a beam expander (14), two polarizing beam splitters, i.e. the first polarizing beam splitter (15), the second polarizing beam splitter (24), three polarization converters, i.e. the first polarization converter (16), the second polarization converter (22) and third polarization converter (25), two biconvex lens, i.e. the first biconvex lens (19) and the second biconvex lens (27), Two analyzers (18), a half-wave plate (23), an injection device that is all-trans (17), the second photodetector (20) and a Preset grating Crystal (28) composition;Wherein:
● the orthogonal cross-polarization electro-optical device of two beam of generation includes a laser (1), a third polarised light Optical splitter (2), two total reflection right-angle prisms, i.e., the first total reflection right-angle prism (3) and the second total reflection right-angle prism (6), Two driving frequencies are respectively f1And f2Acousto-optic modulator, i.e., first sound-optic modulator (4) and second sound-optic modulator (5) and One polarization splicer (7);
● the phase reference device includes an optical splitter (8), the first analyzer (9), third biconvex lens (10) and the One photodetector (11);
● the data acquisition and processing (DAP) device includes two bandpass filters, i.e. the first bandpass filter (12) and second Bandpass filter (21), 16 oscillograph cards (13) of a binary channels and a set of computer system (29);
● be divided into two bunch polarised lights through third polarised light splitter (2) by the laser beam that laser (1) issues: a branch of is p light, Another beam is s light, and it is f that p light, which enters driving frequency by the first total reflection right-angle prism (3),1First sound-optic modulator (4), s Light is f by driving frequency2Second sound-optic modulator (5) after, generate two 0 grade of diffraction lights and two+1 grade of diffraction respectively Light, driving frequency f2Second sound-optic modulator (5)+1 grade of diffraction light by second total reflection right-angle prism (6) and drive Frequency is f1First sound-optic modulator (4)+1 grade of diffraction light enter polarization splicer (7), synthesis light beam pass through optical splitter (8) transmitted light beam passes through after the first analyzer (9), by third biconvex lens (10) in the first photodetector (11) It is interfered on photosurface, and is converted to the electric signal that beat frequency is middle frequency difference, phase of the electric signal of the middle frequency difference as system Position reference signal, filters through the first bandpass filter (12), becomes digital signal into 16 oscillograph cards (13) of binary channels;
Light beam is synthesized by the reflected beams of optical splitter (8) by after beam expander (14), into the first polarizing beam splitter (15), Wherein s light is reflected and is all-trans later by the injection device that is all-trans (17) that the first polarization converter (16) reach regulating reflection degree It penetrates, which becomes p light again by the first polarization converter (16), and penetrates the first polarizing beam splitter (15) and second After analyzer (18), focused on the photosurface of the second photodetector (20) by the first biconvex lens (19);Through first The p light of polarizing beam splitter (15) penetrates second partially by being still p light after the second polarization converter (22) and half-wave plate (23) It shakes optical splitter (24), reaches testee (26) surface by third polarization converter (25) later and be totally reflected, the reflected light It carries " speckle noise " and becomes s light again by polarization converter (25) and reflected by the second polarizing beam splitter (24), by the It is converged on photorefractive crystal (28) after two biconvex lens (27), the phase-conjugation light generated by photorefractive crystal (28), quilt By the second polarizing beam splitter (24) another secondary reflection after second biconvex lens (27) collimation, and penetrate third polarization converter (25) It reaches testee (26) surface to be totally reflected, reflected phase-conjugation light becomes after third polarization converter (25) P light, and by becoming s light after the second polarizing beam splitter (24), half-wave plate (23) and the second polarization converter (22), by first Polarizing beam splitter (15) reflects and focuses on the second photodetector by the first biconvex lens (19) by the second analyzer (18) (20) it on photosurface, is interfered with the p light on the photosurface of arrival photodetector (20) before, and be converted to beat frequency and be The electric signal of middle frequency difference, measuring signal of the electric signal of the middle frequency difference as system are filtered through the second bandpass filter (21), Become digital signal into 16 oscillograph cards (13) of binary channels;
The digital signal passes through the processing of computer system (29) to reference signal and measuring signal data, obtains micro-vibration letter Number amplitude, spectrum value.
2. a kind of dual-acousto-optic phase modulation according to claim 1 is conjugated heterodyne detection device, it is characterised in that: described to swash Light device (1) is gas laser semiconductor laser or solid state laser.
3. a kind of dual-acousto-optic phase modulation according to claim 1 is conjugated heterodyne detection device, it is characterised in that: described the Two polarization converters (22) are Faraday rotators.
4. a kind of dual-acousto-optic phase modulation according to claim 1 is conjugated heterodyne detection device, it is characterised in that: described the One polarization converter (16), the second polarization converter (25) are Faraday rotator or quarter-wave plate.
5. a kind of dual-acousto-optic phase modulation according to claim 1 is conjugated heterodyne detection device, it is characterised in that: described The crystallographic axis of half-wave plate (23) with by the p optical vibration direction angle of the first polarizing beam splitter (15) be 22.5 degree, acting on is The p light for crossing the first polarizing beam splitter (15), after the second polarization converter (22) and half-wave plate (23), partially relative to first Vibration optical splitter (15) is still p light.
CN201610850354.4A 2016-09-26 2016-09-26 A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device Active CN106338334B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610850354.4A CN106338334B (en) 2016-09-26 2016-09-26 A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610850354.4A CN106338334B (en) 2016-09-26 2016-09-26 A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device

Publications (2)

Publication Number Publication Date
CN106338334A CN106338334A (en) 2017-01-18
CN106338334B true CN106338334B (en) 2019-01-15

Family

ID=57840335

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610850354.4A Active CN106338334B (en) 2016-09-26 2016-09-26 A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device

Country Status (1)

Country Link
CN (1) CN106338334B (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107463007B (en) * 2017-09-27 2020-06-12 北京航空航天大学 Dual-channel phase jitter suppression device and method for Raman laser system
CN110849593B (en) * 2019-11-22 2021-06-01 中国科学院长春光学精密机械与物理研究所 Measuring equipment for measuring wave aberration of optical system based on heterodyne interference of acousto-optic modulator

Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04263225A (en) * 1991-02-18 1992-09-18 Kowa Co Method and instrument for optical measurement
US5546187A (en) * 1995-03-15 1996-08-13 Hughes Aircraft Company Self-referencing laser-based ultrasonic wave receiver
CN1264830A (en) * 2000-03-30 2000-08-30 中国科学院上海光学精密机械研究所 Sub-nanometer resolution phase conjugate interference measuring device for object vibration amplitude
CN2419594Y (en) * 2000-03-30 2001-02-14 中国科学院上海光学精密机械研究所 Optical Measuring Instrument for Object Vibration Amplitude
CN2577238Y (en) * 2002-10-24 2003-10-01 中国科学院上海光学精密机械研究所 Measuring device for interference of flat-plate surface appearance
CN201622111U (en) * 2010-03-15 2010-11-03 中国计量科学研究院 Low-noise heterodyne laser interferometer for measuring vibration
JP2011033759A (en) * 2009-07-31 2011-02-17 Sony Corp Three-dimensional image imaging apparatus, three-dimensional image imaging method, three-dimensional image information acquisition system, three-dimensional image information acquisition method
CN102168953A (en) * 2011-01-12 2011-08-31 南京大学 Full-distributed optical fiber strain and vibration sensor based on coherent heterodyne detection
CN103324003A (en) * 2013-06-07 2013-09-25 中国科学院西安光学精密机械研究所 Method and device for nonlinear optical amplification and signal-to-noise ratio enhancement of weak light signal
CN104990619A (en) * 2015-06-12 2015-10-21 哈尔滨工业大学 Polarization- and aliasing-resistance Michelson heterodyne laser vibration measurer based on double acousto-optic modulation and non-polarizing light splitting
CN105634588A (en) * 2015-12-30 2016-06-01 电子科技大学 Coherent optical time domain reflectometer based on phase conjugation double wavelets

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04263225A (en) * 1991-02-18 1992-09-18 Kowa Co Method and instrument for optical measurement
US5546187A (en) * 1995-03-15 1996-08-13 Hughes Aircraft Company Self-referencing laser-based ultrasonic wave receiver
CN1264830A (en) * 2000-03-30 2000-08-30 中国科学院上海光学精密机械研究所 Sub-nanometer resolution phase conjugate interference measuring device for object vibration amplitude
CN2419594Y (en) * 2000-03-30 2001-02-14 中国科学院上海光学精密机械研究所 Optical Measuring Instrument for Object Vibration Amplitude
CN2577238Y (en) * 2002-10-24 2003-10-01 中国科学院上海光学精密机械研究所 Measuring device for interference of flat-plate surface appearance
JP2011033759A (en) * 2009-07-31 2011-02-17 Sony Corp Three-dimensional image imaging apparatus, three-dimensional image imaging method, three-dimensional image information acquisition system, three-dimensional image information acquisition method
CN201622111U (en) * 2010-03-15 2010-11-03 中国计量科学研究院 Low-noise heterodyne laser interferometer for measuring vibration
CN102168953A (en) * 2011-01-12 2011-08-31 南京大学 Full-distributed optical fiber strain and vibration sensor based on coherent heterodyne detection
CN103324003A (en) * 2013-06-07 2013-09-25 中国科学院西安光学精密机械研究所 Method and device for nonlinear optical amplification and signal-to-noise ratio enhancement of weak light signal
CN104990619A (en) * 2015-06-12 2015-10-21 哈尔滨工业大学 Polarization- and aliasing-resistance Michelson heterodyne laser vibration measurer based on double acousto-optic modulation and non-polarizing light splitting
CN105634588A (en) * 2015-12-30 2016-06-01 电子科技大学 Coherent optical time domain reflectometer based on phase conjugation double wavelets

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
脉冲相位共轭光研究的进展;钱锋 等;《光电子·激光》;20010525;第12卷(第5期);第536-539页

Also Published As

Publication number Publication date
CN106338334A (en) 2017-01-18

Similar Documents

Publication Publication Date Title
US5491552A (en) Optical interferometer employing mutually coherent light source and an array detector for imaging in strongly scattered media
US3728030A (en) Polarization interferometer
Ing et al. Broadband optical detection of ultrasound by two‐wave mixing in a photorefractive crystal
WO2021017098A1 (en) Differential laser interferometric nanometer displacement measurement apparatus and method employing sinusoidal phase modulation
US10895477B2 (en) Sine-cosine optical frequency encoder devices based on optical polarization properties
CN108692663A (en) Phase modulation-type cross-polarization Laser feedback grating interferometer and its measurement method
US4176951A (en) Rotating birefringent ellipsometer and its application to photoelasticimetry
US6819428B2 (en) Instruments of optical pulse characterization
US7864332B2 (en) Differential-phase interferometric system
CN107064001A (en) Monochromatic light spectrometer polarization domain optical coherence tomography system based on photoswitch
CN206497027U (en) Monochromatic light spectrometer polarization domain optical coherence tomography system based on photoswitch
CN1187600C (en) Apparatus and method for measuring equivalent refraction power of optical film and physical thickness
CN106338334B (en) A kind of dual-acousto-optic phase modulation conjugation heterodyne detection device
JPH05264609A (en) Method and system for measuring high frequency electric signal through electrooptic effect
KR101081370B1 (en) High resolution optical interferometer with parallel multiple pass configuration and apparatus for measuring distance using the same
WO2017163233A1 (en) Frequency modulated multiple wavelength parallel phase shift interferometry
JPH0695114B2 (en) Voltage detector
US20240142370A1 (en) Circularly polarized light illuminator, analysis device, and microscope
Polavarapu et al. Development, justification, and applications of a mid-infrared polarization-division interferometer
US3520615A (en) Optical phase measuring apparatus
Xie et al. Real-time measurement of retardation and fast axis azimuth for wave plates
CN2419594Y (en) Optical Measuring Instrument for Object Vibration Amplitude
CN109387455B (en) Method and system for measuring wide-area plasma density in real time
JPH0663869B2 (en) Optical sampling waveform measuring device
JPS63128211A (en) Spacing measuring method

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
GR01 Patent grant