CN104035087B - High-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement device and method - Google Patents

High-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement device and method Download PDF

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CN104035087B
CN104035087B CN201410263610.0A CN201410263610A CN104035087B CN 104035087 B CN104035087 B CN 104035087B CN 201410263610 A CN201410263610 A CN 201410263610A CN 104035087 B CN104035087 B CN 104035087B
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input
outfan
laser
frequency
connects
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CN104035087A (en
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谭久彬
杨宏兴
胡鹏程
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Harbin Institute of Technology
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Harbin Institute of Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S11/00Systems for determining distance or velocity not using reflection or reradiation
    • G01S11/12Systems for determining distance or velocity not using reflection or reradiation using electromagnetic waves other than radio waves

Abstract

The invention provides a high-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement device and method and belongs to a phase laser distance measurement technology. The high-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement device comprises a measuring ruler generation unit, a laser frequency shifting unit, a beam expanding collimation lens group and a light path and a circuit measurement unit. The high-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement method comprises step 1, opening a frequency standard laser and a semiconductor laser; step 2, serving one beam as a reference laser beam and serving the other beam as a measurement laser beam; step 3, serving a formula as an accurate measurement ruler; step 4, serving a formula as a rough measurement ruler; step 5, moving a measurement prism to a target side to obtain the phase difference Phi 1 of the rough measurement ruler and the phase difference Phi 2 of the accurate measurement ruler and obtaining a measured distance value through a formula. According to the high-accuracy synchronous multi-measurement-ruler based semiconductor laser distance measurement device and method, the problem that the multi-measurement-ruler synchronicity and traceability of devices and methods cannot be integrated in the phase laser distance measurement technology is solved, the accuracy of distance measurement is high, the measurement efficiency is high, and the stability and the real-time performance are high.

Description

Based on the semiconductor laser range apparatus and method surveying chi high-precise synchronization more
Technical field
The invention belongs to phase place laser measuring technique, relate generally to a kind of phase laser distance apparatus and method.
Background technology
Large-scale metrology development large-scale precision machine-building, great science and technology engineering, aerospace industry, shipping industry and Receive much concern in the large-scale optical, mechanical and electronic integration equipment processing and manufacturing of microelectronics equipment industry etc., wherein several meters to hundreds of meter of scopes big Dimensional measurement is large parts processing and the overall important foundation assembled in aerospace vehicle and jumbo ship, its measurement side Method directly affects workpiece quality and assembly precision with the quality of equipment performance, and then affects the running quality of complete equipment, performance And the life-span.Chi phase ranging methods of surveying carry out refining accuracy survey using one group of survey chi wavelength from big to small to tested distance more Amount, solves conflicting between measurement range and certainty of measurement, can reach submillimeter in hundreds of meters overlength operating distance To micron-sized static measurement precision.
Survey in chi phase laser distance technology, although the mode how survey chi measures step by step has taken into account measurement range and survey more The demand of accuracy of measurement, but the restriction due to light source technology, bigness scale chi and accurate measurement chi can not produce line phase measurement of going forward side by side simultaneously, Cause that time of measuring is long, the problem of measurement result poor real, on the other hand due to surveying chi phase laser distance skills more Measured on the basis of surveying chi wavelength size in art, survey the stability of chi wavelength and accuracy directly affects the essence of laser ranging How degree, therefore obtain the bigness scale chi that high stability can trace to the source and accurate measurement chi wavelength, and to be allowed to simultaneously participate in measurement be current Improve the subject matters surveying chi phase laser distance precision and real-time more.
Under distance or even over distance measurement background, the output of light source is one of important aspect, passes through The analysis of existing LASER Light Source is understood, light source the more commonly used at present is gas laser, semiconductor laser, Solid State Laser Device and dye laser.Wherein gas laser structure is simple, good beam quality, but its output is limited simultaneously, and document was [once Bright, fourth Venus, Yuan Xiaodong. improve frequency stabilization he-ne laser output power research. Acta Optica .1996.1] mention conventional He-ne laser instrument peak power output also only within 5 milliwatts it is impossible to meet the needs of long range measurements.And quasiconductor swashs Light device is a kind of high efficiency, broadband, is easy to the laser instrument modulated, its peak power output is far longer than gas laser, and Structure is simple, meets demand for development and the trend of over distance range finding.
In absolute distance measurement, another key point is to survey stability and the tractability of chi, and it is relevant with light source technology, By the analysis of the light source technology to phase laser distance method laser, the modulation means of phase method have electric current both at home and abroad at present Directly modulation, light modulation and intermode beats frequency modulation etc..
Direct current modulation method utilizes semiconductor laser, the feature that light intensity changes with curent change, comes to quasiconductor The output intensity of laser instrument is modulated, and has the advantages that simply easily to modulate.Document [siyuan liu, jiubin tan and binke hou. multicycle synchronous digital phase measurement used to further improve phase-shift laser range finding.meas. sci. technol.2007,18:1756– 1762] with patent [multiple frequency synchronous modulation large range high precision fast laser ranging apparatus and method, publication number: Cn1825138] all elaborate a kind of current modulating method based on semiconductor laser, it adopts the compound of multiple frequency synchronous synthesis Signal synchronizes modulation it is achieved that obtaining each modulation frequency pin in multifrequency modulation range finding in synchronization to laser output power Measurement result to tested distance, but in order to obtain linear modulation, make operating point be in the straight line portion of output characteristic curve, Suitable bias current makes its output signal undistorted must to add one while adding modulated signal electric current, the introducing of direct current biasing Increase power consumption, temperature raises when working long hours, and can affect the stability of Output optical power, lead to modulation waveform to deform, And the increase with modulating frequency, modulation depth can reduce, and lead to modulation waveform to deform it is impossible to carry out high frequency modulated, limit The size of accurate measurement chi wavelength and degree of stability;On the other hand, in the actual application of large-scale metrology, laser passes in distance Easily cause the loss of laser power during defeated, cause to modulation waveform impact, and then affect survey chi accuracy and Degree of stability, it is surveyed the frequency stability of chi and is generally less than 10-7.
It is mainly acousto-optic modulation method and electro-optic modulation method using light modulating method, its modulation bandwidth is subject to laser beam spot sizes Etc. multifactorial impact, also bring along waveform distortions, just even more serious, therefore its institute particularly when high frequency (Gigahertz) Form big survey chi, certainty of measurement is difficult to improve due to limiting by maximum modulation frequency.
Method by the use of the formed beat signal of laser instrument different mode output as surveying chi, referred to as intermode modulation.This The modulation bandwidth of method is related to the chamber length of laser instrument, and he-ne laser frequency stabilization technology is ripe, and its frequency stability is high, by The degree of stability of the survey chi that it is obtained is high, patent [high accuracy multiple frequency synchronous phase laser distance apparatus and method, publication number: cn 102419166] and patent [the multiple frequency synchronous phase laser distance apparatus and method based on dual-acousto-optic shift, publication number: cn 102305591a] all make use of the intermode of he-ne laser instrument to modulate and combine acousto-optic frequency translation technology, obtain high-precision accurate measurement Chi and bigness scale chi, but the produced chi of surveying of the method does not possess tractability, and during its measurement, absolute measuring chi length needs another detection System is given, and increased the complexity of measurement;On the other hand, the method that this utilization heterodyne method obtains accurate measurement chi phase place, at it The frequency of reason signal is higher, can be to follow-up phase measurement difficulty with certainty of measurement affects it is assumed that phase-measurement accuracy For 0.05o, range measurement accuracy will reach 1um-10um, then signal frequency is at least 2ghz-20ghz, at signal The bandwidth of reason circuit.
Patent [superheterodyne device and method of reseptance and reception device semiconductor integrated circuit, open Number: cn102484492a] all describe a kind of superhet interference signal treatment technology, [Zhang Cunman etc. surpasses Tsing-Hua University Zhang Cunman Difference interference absolute distance measurement Review Study, optical technology 1998, (1): 7-9.] and Japanese shuko yokoyama professor [shuko yokoyamaet al. real-time and high-resolution absolute-distance measurement using a two-wavelength superheterodyne interferometer. meas. sci. Technol.1999,10:1233-1239] all describe superhet absolute distance measurement method, this method reduce signal Processing frequency it is easier to reach higher certainty of measurement.But this technology is on the one hand, can only obtain a survey chi, and do not possess Tractability measures it is impossible to carry out chis of surveying more, let alone the synchronicity surveying chi more;Another aspect superhet obtains surveying chi wavelength Less, typically in micron dimension, it is only used for the measurement of the micro- shape in surface.
In order to improve the stability of laser instrument output frequency, occur in that with the output laser of iodine saturated absorption frequency stabilization laser instrument Frequency is entered to he-ne laser instrument and semiconductor laser as the frequency-stabilizing method of frequency stabilization benchmark, the saturated absorption spectra using iodine Row rrequency-offset-lock controls.China has been also carried out studying, such as patent zl200910072518.5 and patent Zl200910072519.x etc. all describes a kind of rrequency-offset-lock device of utilization iodine saturated absorption he-ne frequency stabilized carbon dioxide laser, makes Laser output frequency after rrequency-offset-lock has very high frequency stability, has the advantages that output frequency can be traced to the source, but laser Output frequency reach 1014Hz, between 400-700nm, measurement range is in nm rank it is impossible to be used for long distance for corresponding survey chi From laser ranging, need a kind of survey chi of laser ranging on a large scale high frequency stability laser frequency being converted to and can tracing to the source badly, and Synchronize them the technology of generation.
In sum, lack in phase laser distance technology at present one kind can take into account high-power, many survey chi synchronicitys with The long distance and high precision laser ranging system of tractability and method.
Content of the invention
The invention aims to solve the existing technology in phase laser distance in lack one kind can take into account high-power, many Survey the laser ranging system of chi synchronicity and tractability and the problem of method, provide a kind of based on surveying chi high-precise synchronization more Semiconductor laser range apparatus and method, reach increase range finding motility, simplify ranging step, improve measurement efficiency and precision and Degree of stability, the purpose of real-time.
The object of the present invention is achieved like this:
A kind of based on the semiconductor laser range device surveying chi high-precise synchronization more, by surveying chi signal generating unit, laser shift frequency Unit, beam-expanding collimation microscope group and optical path and circuit unit composition, the laser that survey chi signal generating unit sends exports laser and moves The input of frequency unit, a road laser of laser shift frequency unit output exports optical path and circuit by beam-expanding collimation microscope group One input of unit, another road laser of laser shift frequency unit output is directly inputted to the another of optical path and circuit unit One input;
The structure of described survey chi signal generating unit is: the laser beam of frequency reference laser instrument transmitting reaches the input of beam splitter End, first outfan of beam splitter connects No. seven spectroscopical inputs, and No. seven spectroscopical outfans connect No. three The input of photodetector, second outfan of beam splitter connects a spectroscopical input, a spectroscope Outfan connect the input of a photodetector, the 3rd outfan of beam splitter connect No. two spectroscopical one defeated Enter end, No. two spectroscopical outfans connect the input of No. two photodetectors, photodetector, No. two photodetections The outfan of device and No. three photodetectors all connects the input of single-chip microcomputer, and connecting cavity is long respectively for three outfans of single-chip microcomputer The input of adjustment executor, the outfan that chamber length adjusts executor connects a semiconductor laser, No. two quasiconductors respectively Laser instrument and the input of No. three semiconductor lasers, an outfan connection four of a semiconductor laser is spectroscopical One input, one outfan of No. four spectroscopes connects a spectroscopical input, No. four another output spectroscopical End connects the input of a polaroid, and an outfan of No. two semiconductor lasers connects No. five spectroscopical inputs End, one outfan of No. five spectroscopes connects No. two spectroscopical inputs, and No. five another outfan spectroscopical connect two The input of number polaroid, the outfan of No. two polaroids connects No. six spectroscopical inputs, No. three semiconductor lasers One outfan of device connects No. three spectroscopical inputs, and No. three spectroscopical outfans connect No. seven spectroscopes Input, No. three spectroscopical another outfan connect the input of No. three polaroids, and the outfan of No. three polaroids leads to Cross No. ten reflecting mirrors and connect No. six another input spectroscopical;
The structure of described laser shift frequency unit is: an outfan surveying chi signal generating unit connects the input of No. six reflecting mirrors End, the outfan of No. six reflecting mirrors connects No. eight spectroscopical inputs, and No. eight spectroscopical outfans connect No. nine points One input of light microscopic, another outfan surveying chi signal generating unit connects the input of a polarization spectroscope, and No. one partially Spectroscopical outfan that shakes connects the input of a half-wave plate, and the outfan of a half-wave plate connects No. two polarization spectros The input of mirror, an outfan of No. two polarization spectroscopes connects an input of No. three polarization spectroscopes, No. two polarizations Another outfan spectroscopical connects the input of a reflecting mirror, and the outfan of a reflecting mirror connects a laser shift frequency One input of device, the outfan of a dds signal source connects another input of a laser frequency shifter, a laser The outfan of frequency shifter connects the input of No. two reflecting mirrors, and the outfan of No. two reflecting mirrors connects the another of No. three polarization spectroscopes One input, the outfan of No. three polarization spectroscopes connects No. eight another input spectroscopical, and No. eight spectroscopical defeated Go out end and connect No. nine spectroscopical inputs, another outfan of a polarization spectroscope connects the defeated of No. three reflecting mirrors Enter end, the outfan of No. three reflecting mirrors connects the input of No. four polarization spectroscopes, No. four polarization spectros through No. two half-wave plates One outfan of mirror connects an input of No. five polarization spectroscopes, and another outfan of No. four polarization spectroscopes connects The input of No. four reflecting mirrors, the outfan of No. four reflecting mirrors connects an input of No. two laser frequency shifters, No. two dds letters The outfan in number source connects another input of No. two laser frequency shifters, the outfan of No. two laser frequency shifters connect No. five anti- Penetrate the input of mirror, the outfan of No. five reflecting mirrors connects another input of No. five polarization spectroscopes, No. five polarization spectros The outfan of mirror connects No. nine another input spectroscopical;
The structure of described optical path and circuit unit is: an outfan of laser shift frequency unit connects No. seven reflecting mirrors Input, the outfan of No. seven reflecting mirrors connects No. ten spectroscopical inputs, and No. ten spectroscopical outfans pass through No. four polaroids are connected with the input of No. four photodetectors, and the outfan of No. four photodetectors connects a low-pass filtering The input of device, an input of an outfan number frequency mixer of connection of a low pass filter, the one of No. three dds signal sources Individual outfan connects another input of a frequency mixer, and one of an outfan number phase discriminator of connection of a frequency mixer defeated Enter end, No. ten another outfan spectroscopical are connected with the input of No. five photodetectors by No. five polaroids, No. five The outfan of photodetector connects the input of No. two low pass filters, and the outfan of No. two low pass filters connects No. two mirror One input of phase device, the outfan of beam-expanding collimation microscope group connects an input of No. six polarization spectroscopes, No. six polarizations A spectroscopical outfan is connected with the input of No. eight reflecting mirrors by a quarter-wave plate, No. eight reflecting mirrors defeated Go out end connected with an input of No. six polarization spectroscopes by a quarter-wave plate, No. six polarization spectroscopes another Individual outfan is connected with the input of No. nine reflecting mirrors by No. two quarter-wave plates, and the outfan of No. nine reflecting mirrors passes through two Number quarter-wave plate is connected with another input of No. six polarization spectroscopes, another outfan of No. six polarization spectroscopes Connect the spectroscopical input of ride on Bus No. 11, the spectroscopical outfan of ride on Bus No. 11 passes through No. six polaroids and No. six photoelectricity The input connection of detector, the outfan of No. six photodetectors connects the input of No. three low pass filters, No. three low passes The outfan of wave filter connects an input of No. three frequency mixers, and another outfan of No. three dds signal sources connects No. three Another input of frequency mixer, the outfan of No. three frequency mixers connects another input of a phase discriminator, and ride on Bus No. 11 is divided Another outfan of light microscopic is connected with the input of No. seven photodetectors by No. seven polaroids, No. seven photodetectors Outfan connects the input of No. four low pass filters, and the outfan of No. four low pass filters connects another of No. two phase discriminators Input.
A kind of based on the semiconductor laser range method surveying chi high-precise synchronization more, it specifically comprises the following steps that
Step one, open frequency benchmark laser, semiconductor laser, No. two semiconductor lasers and three and half are led Body laser, after passing through preheating and frequency stabilization, by feedback control, by a semiconductor laser, No. two semiconductor lasers Within the scope of device and No. three semiconductor laser output frequencies are locked in the certain frequency of frequency reference laser instrument, lead from one and half Body laser sends after polaroid only surplus frequencyv 1Laser, send through polaroid from No. two semiconductor lasers Only remaining frequency afterwards isv 2Laser, and by spectroscope with send from No. three semiconductor lasers remaining after polaroid Frequency isv 3Laser converge;
Step 2, the laser of the three kinds of frequencies being formed by step one enter laser shift frequency unit, and wherein a branch of double frequency swashs Light separates frequency with a polarization spectroscopev 2Withv 3Two bundle laser, are polarized with No. two after half-wave plate more respectively Spectroscope and No. four polarization spectroscopes separate two bundle double-frequency lasers, and wherein one tunnel, through laser frequency shifter, is driven by dds signal source Laser frequency shifter, frequency is respectivelyf 1Withf 2, finally the laser of various frequencies collect, wherein have five kinds of frequencies, respectivelyv 1v 2v 3v 2+f 1Withv 3+f 2, this bundle laser light incident be divided into two-beam to Amici prism, a branch of as reference Laser beam, another Shu Zuowei Laser Measurement bundle shines measurement target;
Step 3, reference laser beam are divided into two bundle laser through Amici prism, wherein beam of laser through polarization direction withv 1Phase After No. four same polaroids, frequency isv 1v 2Withv 3The polarization laser of horizontal direction enter into No. four photodetectors Changed, it exports the signal of telecommunication, frequency isv 1 -v 2 ,In this, as bigness scale chi, another beam of laser through polarization direction withv 1 No. five photodetectors are incided, the signal of telecommunication of No. five photodetector outputs is through low pass filtered after No. five polaroids becoming 45 degree Ripple device has filtered high frequency electrical signal, retains low-frequency electrical signal, and its frequency isf 1-f 2, in this, as accurate measurement chi;
When step 4, measurement start, No. eight reflecting mirrors of the plane of reference maintain static, and mobile No. nine reflecting mirrors, to destination end, are surveyed , from for l, after measuring beam reflects through No. nine reflecting mirrors, the light beam reflecting with the plane of reference is at No. six polarization spectroscopes for span Converge, enter measuring circuit, Laser Measurement bundle is divided into two bundle laser beams through Amici prism, and wherein one laser beam is through polarization direction Withv 1After No. six polaroids of identical, frequency isv 1v 2Withv 3The polarization laser of horizontal direction enter into No. six photoelectricity Detector is changed, and it exports the signal of telecommunication, and its frequency isv 1-v 2, in this, as bigness scale chi, survey chi a length of, separately Beam of laser through polarization direction withv 1No. seven photodetectors, No. five photodetections are incided after No. seven polaroids becoming 45 degree The signal of telecommunication of device output has filtered high frequency electrical signal through low pass filter, retains low-frequency electrical signal, and its frequency isf 1-f 2, In this, as accurate measurement chi, survey chi a length of
Step 5, respectively obtain frequency by a phase discriminator and No. two phase discriminators and bev 1-v 2Withf 1-f 2Two-way The phase contrast of the signal of telecommunicationφ 1Withφ 2, according to formulaTry to achieve the distance measure of bigness scale chil c , and will It substitutes into the phase integer value that formula tries to achieve accurate measurement chi;Whereinfloor(x) function returnxValue Integer part, try to achieve tested distance value finally according to formula:, in formula: c is the light velocity, n is environment Air refraction.
The feature of the present invention and beneficial effect are:
First, the present invention proposes a kind of trace to the source
Survey chi production methods and device, this apparatus and method utilizes frequency reference type frequency reference laser instrument to three and half Conductor laser carries out frequency stabilization and feedback control, makes output laser frequency and can directly trace back with the laser ranging survey chi wavelength being formed Source is to frequency/wavelength benchmark, and can adjust lock point according to actual needs, and then is adjusted to surveying chi wavelength, increases The motility of range finding, overcomes in existing range unit and surveys the shortcoming that chi is not directly traced to the source, simplify general range unit Survey, when absolute measuring is long, the step that chi wavelength needs another detecting system need to provide, improve measurement efficiency and precision, this is this One of innovative point of the other existing apparatus in area pellucida.
Second, the present invention proposes a kind of many surveys chi Phase synchronization acquisition methods being combined based on heterodyne and dress with superhet Put.This apparatus and method carries out shift frequency using laser frequency shifter to the laser of component frequency, produces the laser of multi-frequency, and with Shi Liyong heterodyne approach and superhet approach obtain bigness scale chi and accurate measurement chi respectively, so be allowed to simultaneously participate in measurement it is achieved that The coarse-fine synchro measure surveying chi phase place, shortens time of measuring, improves the real-time of measurement result.By heterodyne and superhet The laser interferometry combining obtains test phase signal, eliminates common mode disturbances, improves the degree of stability surveying chi, drops simultaneously The low frequency of phase measuring circuit receipt signal, reduces the difficulty of circuit design, and this is the wound that the present invention distinguishes existing apparatus The two of new point.
3rd, there is light source using the semiconductor laser light resource based on rrequency-offset-lock as surveying chi in the present invention, make quasiconductor Laser frequency lock, on iodine frequency stabilization absworption peak, has the advantages that frequency stability is high, and semiconductor laser light resource output laser Energy is big, and light echo energy is strong, and signal to noise ratio is higher, advantageously in the measurement of distance, overcomes general gas to a certain extent Body laser is faint and light echo energy that lead to is faint due to output light energy, and signal to noise ratio is low, or even causes system normal The problem of work.This is the three of the innovative point that the present invention distinguishes existing apparatus.
Brief description
Fig. 1 is the general structure schematic diagram of the laser ranging system of the present invention;
Fig. 2 is the structural representation surveying chi signal generating unit;
Fig. 3 is the structural representation of laser shift frequency unit;
Fig. 4 is the structural representation of optical path and circuit unit.
In figure piece number illustrate: 1, survey chi signal generating unit, 2, laser shift frequency unit, 3, beam-expanding collimation microscope group, 4, optical path And circuit unit, 5, frequency reference laser instrument, 6, beam splitter, 7, spectroscope, 8, No. two spectroscopes, 9, No. three spectroscopes, 10th, photodetector, 11, No. two photodetectors, 12, No. three photodetectors, 13, chamber length adjustment executor, 14, single Piece machine, 15, semiconductor laser, 16, No. two semiconductor lasers, 17, No. three semiconductor lasers, 18, No. four light splitting Mirror, 19, No. five spectroscopes, 20, No. six spectroscopes, 21, polaroid, 22, No. two polaroids, 23, No. three polaroids, 24 1 Number polarization spectroscope, 25, half-wave plate, 26, No. two polarization spectroscopes, 27, reflecting mirror, 28, dds signal source, 29th, laser frequency shifter, 30, No. two reflecting mirrors, 31, No. three polarization spectroscopes, 32, No. eight spectroscopes, 33, No. three reflections Mirror, 34, No. two half-wave plates, 35, No. four polarization spectroscopes, 36, No. four reflecting mirrors, 37, No. two dds signal sources, 38, No. two laser Frequency shifter, 39, No. five reflecting mirrors, 40, No. five polarization spectroscopes, 41, No. six reflecting mirrors, 42, No. nine spectroscopes, 43, No. seven anti- Penetrate mirror, 44, No. ten spectroscopes, 45, No. four polaroids, 46, No. four photodetectors, 47, low pass filter, 48, No. one Frequency mixer, 49, No. three dds signal sources, 50, phase discriminator, 51, No. five polaroids, 52, No. five photodetectors, 53, No. two Low pass filter, 54, No. two phase discriminators, 55, No. six polarization spectroscopes, 56, quarter-wave plate, 57, No. eight reflecting mirrors, 58th, No. two quarter-wave plates, 59, No. nine reflecting mirrors, 60, ride on Bus No. 11 spectroscope, 61, No. six polaroids, 62, No. six light electrical resistivity surveys Survey device, 63, No. three low pass filters, 64, No. three frequency mixers, 65, No. seven polaroids, 66, No. seven photodetectors, 67, No. four Low pass filter, 68, No. ten reflecting mirrors, 69, No. seven spectroscopes.
Specific embodiment
Below in conjunction with the accompanying drawings embodiment of the present invention is described in detail.
A kind of based on the semiconductor laser range device surveying chi high-precise synchronization more,
Described device is by surveying chi signal generating unit 1, laser shift frequency unit 2, beam-expanding collimation microscope group 3 and optical path and circuit list Unit 4 composition, the laser that survey chi signal generating unit 1 sends exports the input of laser shift frequency unit 2, and laser shift frequency unit 2 exports A road laser export an input of optical path and circuit unit 4, laser shift frequency unit by beam-expanding collimation microscope group 3 Another road laser of 2 outputs is directly inputted to another input of optical path and circuit unit 4;
The structure of described survey chi signal generating unit 1 is: the laser beam of frequency reference laser instrument 5 transmitting reaches the defeated of beam splitter 6 Enter end, first outfan of beam splitter 6 connects an input of No. seven spectroscopes 69, the outfan of No. seven spectroscopes 69 Connect the input of No. three photodetectors 12, second outfan of beam splitter 6 connects an input of a spectroscope 7 End, the outfan of a spectroscope 7 connects the input of a photodetector 10, and the 3rd outfan of beam splitter 6 connects One input of No. two spectroscopes 8, the input of outfan No. two photodetectors 11 of connection of No. two spectroscopes 8, No. one The outfan of 10, No. two photodetectors 11 of photodetector and No. three photodetectors 12 all connects the input of single-chip microcomputer 14 End, three outfans difference connecting cavity length of single-chip microcomputer 14 adjust the input of executor 13, and chamber length adjusts the defeated of executor 13 Go out the input that end connects 15, No. two semiconductor lasers 16 of a semiconductor laser and No. three semiconductor lasers 17 respectively End, an outfan of a semiconductor laser 15 connects an input of No. four spectroscopes 18, No. four spectroscopes 18 1 Individual outfan connects the input of a spectroscope 7, and another outfan of No. four spectroscopes 18 connects a polaroid 21 Input, an outfan of No. two semiconductor lasers 16 connects an input of No. five spectroscopes 19, No. five spectroscopes 19 1 outfans connect the input of No. two spectroscopes 8, and another outfan of No. five spectroscopes 19 connects No. two polaroids 22 input, the outfan of No. two polaroids 22 connects an input of No. six spectroscopes 20, No. three semiconductor lasers 17 outfan connects an input of No. three spectroscopes 9, and an outfan of No. three spectroscopes 9 connects No. seven light splitting The input of mirror 69, another outfan of No. three spectroscopes 9 connects the input of No. three polaroids 23, No. three polaroids 23 Outfan passes through another input that No. ten reflecting mirrors 68 connect No. six spectroscopes 20;
The structure of described laser shift frequency unit 2 is: an outfan surveying chi signal generating unit 1 connects No. six reflecting mirrors 41 Input, the outfan of No. six reflecting mirrors 41 connects an input of No. eight spectroscopes 32, the outfan of No. eight spectroscopes 32 Connect an input of No. nine spectroscopes 42, another outfan surveying chi signal generating unit 1 connects a polarization spectroscope 24 Input, outfan of a polarization spectroscope 24 connects the input of a half-wave plate 25, a half-wave plate 25 Outfan connects the input of No. two polarization spectroscopes 26, and an outfan of No. two polarization spectroscopes 26 connects No. three polarizations point One input of light microscopic 31, the input of another outfan number reflecting mirror 27 of connection of No. two polarization spectroscopes 26, one The outfan of number reflecting mirror 27 connects an input of a laser frequency shifter 29, and the outfan of a dds signal source 28 is even Connect another input of a laser frequency shifter 29, the outfan of a laser frequency shifter 29 connects the defeated of No. two reflecting mirrors 30 Enter end, the outfan of No. two reflecting mirrors 30 connects another input of No. three polarization spectroscopes 31, No. three polarization spectroscopes 31 Outfan connect another inputs of No. eight spectroscopes 32, the outfan of No. eight spectroscopes 32 connects No. nine spectroscopes 42 One input, another outfan of a polarization spectroscope 24 connects the input of No. three reflecting mirrors 33, No. three reflecting mirrors 33 outfan connects the input of No. four polarization spectroscopes 35 through No. two half-wave plates 34, one of No. four polarization spectroscopes 35 Outfan connects an input of No. five polarization spectroscopes 40, and another outfan of No. four polarization spectroscopes 35 connects No. four The input of reflecting mirror 36, the outfan of No. four reflecting mirrors 36 connects an input of No. two laser frequency shifters 38, No. two dds The outfan of signal source 37 connects another input of No. two laser frequency shifters 38, and the outfan of No. two laser frequency shifters 38 is even Connect the input of No. five reflecting mirrors 39, the outfan of No. five reflecting mirrors 39 connects another input of No. five polarization spectroscopes 40 End, the outfan of No. five polarization spectroscopes 40 connects another input of No. nine spectroscopes 42;
The structure of described optical path and circuit unit 4 is: an outfan of laser shift frequency unit 2 connects No. seven reflections The input of mirror 43, the input of outfan No. ten spectroscopes 44 of connection of No. seven reflecting mirrors 43, one of No. ten spectroscopes 44 Outfan is connected with the input of No. four photodetectors 46 by No. four polaroids 45, the outfan of No. four photodetectors 46 Connect the input of a low pass filter 47, one of an outfan number frequency mixer 48 of connection of a low pass filter 47 defeated Enter end, an outfan of No. three dds signal sources 49 connects another input of a frequency mixer 48, a frequency mixer 48 Outfan connects an input of a phase discriminator 50, and another outfan of No. ten spectroscopes 44 passes through No. five polaroids 51 Connect with the input of No. five photodetectors 52, the outfan of No. five photodetectors 52 connects No. two low pass filters 53 Input, the outfan of No. two low pass filters 53 connects an input of No. two phase discriminators 54, beam-expanding collimation microscope group 3 defeated Go out the input that end connects No. six polarization spectroscopes 55, an outfan of No. six polarization spectroscopes 55 passes through No. one four points One of wave plate 56 connect with the input of No. eight reflecting mirrors 57, the outfan of No. eight reflecting mirrors 57 passes through a quarter-wave plate 56 are connected with an input of No. six polarization spectroscopes 55, and another outfan of No. six polarization spectroscopes 55 passes through No. two four / mono- wave plate 58 is connected with the input of No. nine reflecting mirrors 59, and the outfan of No. nine reflecting mirrors 59 passes through No. two quarter-waves Piece 58 is connected with another input of No. six polarization spectroscopes 55, and another outfan of No. six polarization spectroscopes 55 connects ten One input of a number spectroscope 60, an outfan of ride on Bus No. 11 spectroscope 60 passes through No. six polaroids 61 and No. six photoelectricity The input connection of detector 62, the input of outfan No. three low pass filters 63 of connection of No. six photodetectors 62, three The outfan of number low pass filter 63 connects an input of No. three frequency mixers 64, and another of No. three dds signal sources 49 is defeated Go out another input that end connects No. three frequency mixers 64, the outfan of No. three frequency mixers 64 connects the another of a phase discriminator 50 Individual input, another outfan of ride on Bus No. 11 spectroscope 60 passes through the input of No. seven polaroids 65 and No. seven photodetectors 66 End connection, the outfan of No. seven photodetectors 66 connects the input of No. four low pass filters 67, No. four low pass filters 67 Outfan connect No. two phase discriminators 54 another input.
One, No. two laser frequency shifters 29,38 of described laser shift frequency unit 2 include acousto-optic frequency shifters, electro-optic frequency translation device, and Laser frequency can be adjusted.
Described survey chi signal generating unit 1 medium frequency benchmark laser 5 includes iodine saturated absorption frequency stabilization laser instrument, femtosecond laser frequency Rate combs laser instrument, and frequency stability is better than 10-12.
A kind of based on the semiconductor laser range method surveying chi high-precise synchronization more, it specifically comprises the following steps that
Step one, open frequency benchmark laser 15, No. two semiconductor lasers 16 and three of 5, semiconductor laser Number semiconductor laser 17, after preheating and frequency stabilization, by feedback control, by a semiconductor laser 15, two Semiconductor laser 16 and No. three semiconductor laser 17 output frequencies are locked in the certain frequency scope of frequency reference laser instrument 5 Within, sending after polaroid only surplus frequency from a semiconductor laser 15 isv 1Laser, from No. two semiconductor lasers Device 16 sends after polaroid only surplus frequencyv 2Laser, and by spectroscope with from No. three semiconductor lasers 17 Going out remaining frequency after polaroid isv 3Laser converge;
Step 2, the laser of the three kinds of frequencies being formed by step one enter laser shift frequency unit 2, and wherein a branch of double frequency swashs Light separates frequency with a polarization spectroscope 24v 2Withv 3Two bundle laser, after half-wave plate more respectively with No. two partially Shake spectroscope 26 and No. four polarization spectroscopes 35 separate two bundle double-frequency lasers, wherein one tunnel through laser frequency shifter, by dds signal Source drives laser frequency shifter, and frequency is respectivelyf 1Withf 2, finally the laser of various frequencies collect, wherein have five kinds of frequencies, It is respectivelyv 1v 2v 3v 2+f 1Withv 3+f 2, this restraints laser light incident and is divided into two-beam, Yi Shuzuo to Amici prism For reference laser beam, another Shu Zuowei Laser Measurement bundle shines measurement target;
Step 3, reference laser beam are divided into two bundle laser through Amici prism, wherein beam of laser through polarization direction withv 1Phase After No. four same polaroids 45, frequency isv 1v 2Withv 3The polarization laser of horizontal direction enter into No. four photodetections Device 46 is changed, and it exports the signal of telecommunication, and frequency isv 1 -v 2 ,In this, as bigness scale chi, another beam of laser is through polarization direction Withv 1No. five photodetectors 52, the telecommunications of No. five photodetector 52 outputs is incided after No. five polaroids 51 becoming 45 degree Number filter high frequency electrical signal through low pass filter, retain low-frequency electrical signal, its frequency isf 1-f 2, in this, as accurate measurement Chi;
When step 4, measurement start, No. eight reflecting mirrors 57 of the plane of reference maintain static, and mobile No. nine reflecting mirrors 59 are to target End, measurement distance is l, and after measuring beam reflects through No. nine reflecting mirrors 59, the light beam being reflected with the plane of reference is polarized at No. six Converge at spectroscope 55, enter measuring circuit, Laser Measurement bundle is divided into two bundle laser beams, wherein one laser beam through Amici prism Through polarization direction withv 1After No. six polaroids 61 of identical, frequency isv 1v 2Withv 3The polarization laser of horizontal direction enter Enter and changed to No. six photodetectors 62, it exports the signal of telecommunication, its frequency isv 1 -v 2 ,In this, as bigness scale chi, survey Chi is a length of, another beam of laser through polarization direction withv 1No. seven photoelectricity are incided after No. seven polaroids 65 becoming 45 degree Detector 66, the signal of telecommunication of No. five photodetector 52 outputs has filtered high frequency electrical signal through low pass filter, retains low frequency The signal of telecommunication, its frequency isf 1-f 2, in this, as accurate measurement chi, survey chi a length of
Step 5, respectively obtain frequency by a phase discriminator 50 and No. two phase discriminators 54 and bev 1-v 2Withf 1-f 2's The phase contrast of two path signalφ 1Withφ 2, according to formulaTry to achieve the distance measure of bigness scale chil c , And substituted into the phase integer value that formula tries to achieve accurate measurement chi;Whereinfloor(x) function ReturnxThe integer part of value, tries to achieve tested distance value finally according to formula:, in formula: c is light Speed, n is the air refraction of environment.
The phase contrast of described two path signalφ 1With phase contrastφ 2Measurement carry out in synchronization.
Accurate measurement chi used and bigness scale chi all can be traced to the source.

Claims (6)

1. a kind of based on the semiconductor laser range device surveying chi high-precise synchronization more it is characterised in that: described device is by surveying chi Signal generating unit (1), laser shift frequency unit (2), beam-expanding collimation microscope group (3) and optical path and circuit unit (4) composition, survey chi life The laser that unit (1) sends is become to export the input of laser shift frequency unit (2), the road that laser shift frequency unit (2) exports is swashed Light exports an input of optical path and circuit unit (4), laser shift frequency unit (2) by beam-expanding collimation microscope group (3) Another road laser of output is directly inputted to optical path and another input of circuit unit (4);
The structure of described survey chi signal generating unit (1) is: the laser beam that frequency reference laser instrument (5) is launched reaches beam splitter (6) Input, first outfan of beam splitter (6) connects an input of No. seven spectroscopes (69), No. seven spectroscopes (69) Outfan connect the input of No. three photodetectors (12), second outfan of beam splitter (6) connects a spectroscope (7) a input, the outfan of a spectroscope (7) connects the input of a photodetector (10), beam splitter (6) The 3rd outfan connect an input of No. two spectroscopes (8), the outfan of No. two spectroscopes (8) connects No. two photoelectricity The input of detector (11), a photodetector (10), No. two photodetectors (11) and No. three photodetectors (12) Outfan all connect the input of single-chip microcomputer (14), three outfans connecting cavity length adjustment executors respectively of single-chip microcomputer (14) (13) input, the outfan that chamber length adjusts executor (13) connects a semiconductor laser (15) respectively, two and half leads Body laser (16) and the input of No. three semiconductor lasers (17), an outfan of a semiconductor laser (15) is even Connect an input of No. four spectroscopes (18), (18) outfans of No. four spectroscopes connect the input of a spectroscope (7) End, another outfan of No. four spectroscopes (18) connects the input of a polaroid (21), No. two semiconductor lasers (16) a outfan connects an input of No. five spectroscopes (19), and (19) outfans of No. five spectroscopes connect two The input of number spectroscope (8), another outfan of No. five spectroscopes (19) connects the input of No. two polaroids (22), and two The outfan of number polaroid (22) connects an input of No. six spectroscopes (20), one of No. three semiconductor lasers (17) Outfan connects an input of No. three spectroscopes (9), and an outfan of No. three spectroscopes (9) connects No. seven spectroscopes (69) input, another outfan of No. three spectroscopes (9) connects the input of No. three polaroids (23), No. three polaroids (23) outfan passes through another input that No. ten reflecting mirrors (68) connect No. six spectroscopes (20);
The structure of described laser shift frequency unit (2) is: an outfan surveying chi signal generating unit (1) connects No. six reflecting mirrors (41) Input, the outfan of No. six reflecting mirrors (41) connects an input of No. eight spectroscopes (32), No. eight spectroscopes (32) Outfan connect No. nine spectroscopes (42) an input, survey chi signal generating unit (1) another outfan connect No. one The input of polarization spectroscope (24), an outfan of a polarization spectroscope (24) connects the input of a half-wave plate (25) End, the outfan of a half-wave plate (25) connects the input of No. two polarization spectroscopes (26), No. two polarization spectroscopes (26) One outfan connects an input of No. three polarization spectroscopes (31), another outfan of No. two polarization spectroscopes (26) Connect the input of a reflecting mirror (27), the outfan of a reflecting mirror (27) connects one of a laser frequency shifter (29) Input, the outfan of a dds signal source (28) connects another input of a laser frequency shifter (29), a laser The outfan of frequency shifter (29) connects the input of No. two reflecting mirrors (30), and the outfan of No. two reflecting mirrors (30) connects No. three partially Shake another input of spectroscope (31), and the outfan of No. three polarization spectroscopes (31) connects the another of No. eight spectroscopes (32) Individual input, the outfan of No. eight spectroscopes (32) connects an input of No. nine spectroscopes (42), a polarization spectroscope (24) another outfan connects the input of No. three reflecting mirrors (33), and the outfan of No. three reflecting mirrors (33) is through two and half Wave plate (34) connects the input of No. four polarization spectroscopes (35), and an outfan of No. four polarization spectroscopes (35) connects No. five One input of polarization spectroscope (40), another outfan of No. four polarization spectroscopes (35) connects No. four reflecting mirrors (36) Input, the outfan of No. four reflecting mirrors (36) connects an input of No. two laser frequency shifters (38), No. two dds signals The outfan in source (37) connects another input of No. two laser frequency shifters (38), the outfan of No. two laser frequency shifters (38) Connect the input of No. five reflecting mirrors (39), the outfan of No. five reflecting mirrors (39) connects the another of No. five polarization spectroscopes (40) Individual input, the outfan of No. five polarization spectroscopes (40) connects another input of No. nine spectroscopes (42);
The structure of described optical path and circuit unit (4) is: an outfan of laser shift frequency unit (2) connects No. seven reflections The input of mirror (43), the outfan of No. seven reflecting mirrors (43) connects the input of No. ten spectroscopes (44), No. ten spectroscopes (44) a outfan is connected with the input of No. four photodetectors (46) by No. four polaroids (45), No. four light electrical resistivity surveys The outfan surveying device (46) connects the input of a low pass filter (47), and the outfan of a low pass filter (47) connects One input of a number frequency mixer (48), an outfan of No. three dds signal sources (49) connects a frequency mixer (48) Another input, the outfan of a frequency mixer (48) connects an input of a phase discriminator (50), No. ten spectroscopes (44) another outfan is connected with the input of No. five photodetectors (52) by No. five polaroids (51), No. five photoelectricity The outfan of detector (52) connects the input of No. two low pass filters (53), and the outfan of No. two low pass filters (53) is even Connect an input of No. two phase discriminators (54), the outfan of beam-expanding collimation microscope group (3) connects No. six polarization spectroscopes (55) One input, an outfan of No. six polarization spectroscopes (55) passes through a quarter-wave plate (56) and No. eight reflecting mirrors (57) input connection, the outfan of No. eight reflecting mirrors (57) passes through a quarter-wave plate (56) and No. six polarization spectros One input connection of mirror (55), another outfan of No. six polarization spectroscopes (55) passes through No. two quarter-wave plates (58) connect with the input of No. nine reflecting mirrors (59), the outfan of No. nine reflecting mirrors (59) passes through No. two quarter-wave plates (58) connect with another input of No. six polarization spectroscopes (55), another outfan of No. six polarization spectroscopes (55) is even Connect an input of ride on Bus No. 11 spectroscope (60), an outfan of ride on Bus No. 11 spectroscope (60) passes through No. six polaroids (61) Connect with the input of No. six photodetectors (62), the outfan of No. six photodetectors (62) connects No. three low pass filters (63) input, the outfan of No. three low pass filters (63) connects an input of No. three frequency mixers (64), No. three dds Another outfan of signal source (49) connects another input of No. three frequency mixers (64), the output of No. three frequency mixers (64) End connects another input of a phase discriminator (50), and another outfan of ride on Bus No. 11 spectroscope (60) passes through No. seven and polarizes Piece (65) is connected with the input of No. seven photodetectors (66), and the outfan of No. seven photodetectors (66) connects No. four low passes The input of wave filter (67), the outfan of No. four low pass filters (67) connects another input of No. two phase discriminators (54) End.
2. according to claim 1 based on the semiconductor laser range device surveying chi high-precise synchronization more it is characterised in that: One, No. two laser frequency shifters (29,38) of described laser shift frequency unit (2) include acousto-optic frequency shifters, electro-optic frequency translation device, and laser Frequency can be adjusted.
3. according to claim 1 based on the semiconductor laser range device surveying chi high-precise synchronization more it is characterised in that: Described survey chi signal generating unit (1) medium frequency benchmark laser (5) includes iodine saturated absorption frequency stabilization laser instrument, femtosecond laser frequency comb Laser instrument, and frequency stability is better than 10-12.
4. a kind of range finding side based on the semiconductor laser range device surveying chi high-precise synchronization as claimed in claim 1 more Method it is characterised in that: specifically comprise the following steps that
Step one, open frequency benchmark laser (5), a semiconductor laser (15), No. two semiconductor lasers (16) and No. three semiconductor lasers (17), after passing through preheating and frequency stabilization, by feedback control, by a semiconductor laser (15), No. two semiconductor lasers (16) and No. three semiconductor laser (17) output frequencies are locked in frequency reference laser instrument (5), within the scope of certain frequency, sending after polaroid only surplus frequency from a semiconductor laser (15) isv 1Swash Light, sending after polaroid only surplus frequency from No. two semiconductor lasers (16) isv 2Laser, and by spectroscope with from No. three semiconductor lasers (17) send remaining frequency after polaroid and arev 3Laser converge;
Step 2, the laser of the three kinds of frequencies being formed by step one enter laser shift frequency unit (2), wherein a branch of double-frequency laser Separating frequency with a polarization spectroscope (24) isv 2Withv 3Two bundle laser, after half-wave plate more respectively with No. two partially Shake spectroscope (26) and No. four polarization spectroscopes (35) separate two bundle double-frequency lasers, wherein one tunnel through laser frequency shifter, by dds Signal source drives laser frequency shifter, and frequency is respectivelyf 1Withf 2, finally the laser of various frequencies collect, wherein have five kinds Frequency, respectivelyv 1v 2v 3v 2+f 1Withv 3+f 2, this restraints laser light incident and is divided into two-beam to Amici prism, and one Shu Zuowei reference laser beam, another Shu Zuowei Laser Measurement bundle shines measurement target;
Step 3, reference laser beam are divided into two bundle laser through Amici prism, wherein beam of laser through polarization direction withv 1Identical After No. four polaroids (45), frequency isv 1v 2Withv 3The polarization laser of horizontal direction enter into No. four photodetectors (46) changed, it exports the signal of telecommunication, frequency isv 1-v 2 ,In this, as bigness scale chi, another beam of laser is through polarization direction Withv 1No. five photodetectors (52), No. five photodetector (52) outputs are incided after No. five polaroids (51) becoming 45 degree The signal of telecommunication filtered high frequency electrical signal through low pass filter, retain low-frequency electrical signal, its frequency isf 1-f 2, made with this For accurate measurement chi;
When step 4, measurement start, No. eight reflecting mirrors (57) of the plane of reference maintain static, and mobile No. nine reflecting mirrors (59) are to target End, measurement distance is l, and after measuring beam reflects through No. nine reflecting mirrors (59), the light beam reflecting with the plane of reference is at No. six partially Spectroscope (55) place that shakes converges, and enters measuring circuit, Laser Measurement bundle is divided into two bundle laser beams through Amici prism, wherein a branch of swashs Light beam through polarization direction withv 1After No. six polaroids (61) of identical, frequency isv 1v 2Withv 3Horizontal direction polarization Laser enters into No. six photodetectors (62) and is changed, and it exports the signal of telecommunication, and its frequency isv 1-v 2 ,In this, as Bigness scale chi, surveys chi a length of, another beam of laser through polarization direction withv 1Enter after No. seven polaroids (65) becoming 45 degree It is mapped to No. seven photodetectors (66), the signal of telecommunication that No. five photodetectors (52) export has filtered high frequency through low pass filter The signal of telecommunication, retains low-frequency electrical signal, and its frequency isf 1-f 2, in this, as accurate measurement chi, survey chi a length of
Step 5, respectively obtain frequency by a phase discriminator (50) and No. two phase discriminators (54) and bev 1-v 2Withf 1-f 2's The phase contrast of two path signalφ 1Withφ 2, according to formulaTry to achieve the distance measure of bigness scale chil c , And substituted into the phase integer value that formula tries to achieve accurate measurement chi;Whereinfloor(x) function returnx The integer part of value, tries to achieve tested distance value finally according to formula:, in formula: c is the light velocity, n is environment Air refraction.
5. the distance-finding method based on the semiconductor laser range device surveying chi high-precise synchronization according to claim 4 more, It is characterized in that: the phase contrast of described two path signalφ 1With phase contrastφ 2Measurement carry out in synchronization.
6. the distance-finding method based on the semiconductor laser range device surveying chi high-precise synchronization according to claim 4 more, It is characterized in that: accurate measurement chi used and bigness scale chi all can be traced to the source.
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Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003149341A (en) * 2001-11-09 2003-05-21 Nikon Geotecs Co Ltd Distance measuring device
JP2008267893A (en) * 2007-04-18 2008-11-06 Sokkia Topcon Co Ltd Electro-optical range finder
CN101533096A (en) * 2009-04-23 2009-09-16 哈尔滨工业大学 Dual-frequency laser ranging method and device based on polarization state regulation and wavelength synthesis
CN102305591A (en) * 2011-08-17 2012-01-04 哈尔滨工业大学 Multi-frequency synchronization phase laser ranging device and method based on dual-acousto-optic shift frequency
CN102419166A (en) * 2011-08-17 2012-04-18 哈尔滨工业大学 High-precision multi-frequency phase-synchronized laser distance measurement device and method

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003149341A (en) * 2001-11-09 2003-05-21 Nikon Geotecs Co Ltd Distance measuring device
JP2008267893A (en) * 2007-04-18 2008-11-06 Sokkia Topcon Co Ltd Electro-optical range finder
CN101533096A (en) * 2009-04-23 2009-09-16 哈尔滨工业大学 Dual-frequency laser ranging method and device based on polarization state regulation and wavelength synthesis
CN102305591A (en) * 2011-08-17 2012-01-04 哈尔滨工业大学 Multi-frequency synchronization phase laser ranging device and method based on dual-acousto-optic shift frequency
CN102419166A (en) * 2011-08-17 2012-04-18 哈尔滨工业大学 High-precision multi-frequency phase-synchronized laser distance measurement device and method

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