ABSOLUTE DISTANCE MEASUREMENT APPARATUS AND METHOD USING LASER INTERFEROMETRIC WAVELENGTH LEVERAGE

Abstract

An absolute distance measurement apparatus and method using laser interferometric wavelength leverage includes a light source system, a wavelength-leverage laser interferometric system and an interference signal processing and controlling system. The light source system outputs a orthogonally linearly polarized beam with the wavelength λ1 and the wavelength λ2. The orthogonally linearly polarized beam projects onto the wavelength-leverage laser interferometric system to form the interference beam. The interference beam projects onto the interference signal processing and controlling system. In the wavelength-leverage laser interferometric system, the synthetic wavelength and the single wavelength as well as the measured absolute distance and the moving displacement of the cube-corner prism in the reference arm form a wavelength-leverage absolute distance measurement relationship.

Description

BACKGROUND OF THE INVENTION

Technical Field

The present invention relates to an optical measuring apparatus and method and particularly relates to an absolute distance measurement apparatus and method using laser interferometric wavelength leverage.

Description of Related Art

With the development of science and technology, absolute distance measurement of large length with high accuracy are applied more and more widely to high-end equipment manufacturing, spatial engineering, metrological technique and so on. For example, the measurement of racks of heavy machines, the measurement of beds of large precision machine tools, the measurement of lengths of steam and hydraulic turbine spindles, the measurement of diameters of stators and rotors of water-turbine generator sets of hydropower stations, the measurement of installing positions of aircraft fixtures in the aerospace industry, the monitoring of positions and postures and the high-resolution distance measurement of satellites in satellite formation flying and so on not only demand distance measurement accuracy to reach micrometer level and even lower in the scope from few tens of meters to hundreds of meters but also need these measurement instruments to have high efficiency and good flexibility and to be suitable for measuring conditions without guide rails.

The absolute distance measurement methods are mainly divided into two types: time-of-flight measurement and interferometric measurement. Among the time-of-flight measurement, the distance measurement with laser pulses is limited by picosecond time measurement accuracy, and thus the distance measurement accuracy is in the millimeter level; although the measurement accuracy of the balanced optical cross-correlation based on femtosecond pulses superposition can realize the sub-micrometer order, the measured distance must be an integer multiple of the femtosecond interpulse distance, then arbitrary absolute distance cannot be measured; the phase shifting method achieves the time of flight by measuring the phase delay generated by the measured round-tripping distance of modulated light waves, the measurement resolution depends on the phase resolution of the maximum modulating frequency, and the measured distance is limited by the non-ambiguity distance corresponding to the minimum modulating frequency. The laser interferometric absolute distance measurement mainly includes frequency-sweeping interferometry, femtosecond pulse dispersive interferometry and multiple-wavelength interferometry. For frequency-sweeping interferometry, the variations of the measured distance will induce large errors during the sweep, and the relative uncertainty is 10⁻⁶; the femtosecond pulse dispersive interferometry is limited by the resolution of spectrum analyzer, and the relative uncertainty is 10⁻⁵; the multiple-wavelength interferometry uses multiple wavelengths to constitute a gradually increasing synthetic-wavelength chain and gradually obtains the measured distance by starting from the maximum synthetic wavelength according to the initial estimate of the measured distance and the fractional fringe order corresponding to each synthetic wavelength. In the multiple-wavelength interferometry, the fractional fringe order is usually determined by using beat-wave detection, heterodyne detection, superheterodyne detection and son on, wherein the beat-wave detection is affected by direct-current drift of light intensity, and relative uncertainty is less than 10⁻⁶; in the optical configurations of the heterodyne detection and the superheterodyne detection, heterodyne light sources are affected by frequency modulators and the stability of synthetic wavelength is low, and thus the distance measurement accuracy is difficult to improve.

BRIEF SUMMARY OF THE INVENTION

The present invention aims to disclose an absolute distance measurement apparatus and method using laser interferometric wavelength leverage. According to the one-to-one correspondence between the synthetic wavelength formed by two single wavelengths and a single wavelength, a leverage relation is formed between the measured absolute distance and the moving displacement of the cube-corner prism in the reference arm. The measured absolute distance of large length is obtained by determining the moving displacement of the cube-corner prism in the reference arm. The present invention has the advantages of large measurement range, high measurement accuracy and traceability to the definition of the meter.

The present invention adopts the following technical solutions to solve the technical problem:

1. An absolute distance measurement apparatus using laser interferometric wavelength leverage:

comprising a light source system, a wavelength-leverage laser interferometric system and an interference signal processing and controlling system. The light source system outputs a orthogonally linearly polarized beam with the wavelength λ₁ and wavelength λ₂. The orthogonally linearly polarized beam projects onto the wavelength-leverage laser interferometric system to form the interference beam. The interference beam projects onto the interference signal processing and controlling system. The controller in the interference signal processing and controlling system is used for controlling the change of the wavelength λ₂ in the light source system.

The light source system comprises a first laser, a second laser, a first beam expander, a second beam expander, a first reflector and a first polarizing beam splitter. The linearly polarized beam with a constant wavelength λ₁ emitted from the first laser passes through the first beam expander and projects onto the first polarizing beam splitter. The linearly polarized beam with a variable wavelength λ₂ emitted from the second laser, whose polarization direction is perpendicular to that of the beam from the first laser, passes through the second beam expander, is reflected by the first reflector and projects onto the first polarizing beam splitter. The linearly polarized beam with the constant wavelength λ₁ transmitted by the first polarizing beam splitter and the linearly polarized beam with the variable wavelength λ₂ reflected by the first polarizing beam splitter combine one orthogonally linearly polarized beam.

The wavelength-leverage laser interferometric system comprises a first beam splitter, a second polarizing beam splitter, a first cube-corner prism, a second beam splitter, a first shutter, a second shutter, a second reflector, a third reflector, a third beam splitter, a second cube-corner prism and a third cube-corner prism. Being incident on the first beam splitter, the orthogonally linearly polarized beam is divided into the reflected reference beam and the transmitted measurement beam. The reflected reference beam projects onto the second polarizing beam splitter, wherein the linearly polarized beam with the wavelength λ₂ is reflected twice by the second polarizing beam splitter and projects onto the first beam splitter, and the linearly polarized beam with the wavelength λ₁ passes through the second polarizing beam splitter, projects onto the first cube-corner prism, returns after being reflected, and projects onto the first beam splitter after passing through the second polarizing beam splitter again. Being incident on the second beam splitter, the transmitted measurement beam is divided into the reflected near-end measurement beam and the transmitted far-end measurement beam. The near-end measurement beam projects onto the first beam splitter after passing through the first shutter, the second reflector, the second cube-corner prism and the third beam splitter in sequence. And the far-end measurement beam projects onto the first beam splitter after passing through the second shutter, the third cube-corner prism, the third reflector and the third beam splitter in sequence. Being reflected by the first beam splitter, the near-end or far-end measurement beam recombines with the reference beam transmitted by the first beam splitter to form the interference beam.

The interference signal processing and controlling system comprises a third polarizing beam splitter, a first photodetector, a second photodetector, a data acquisition module, a computer and a controller. The interference beam from the wavelength-leverage laser interferometric system projects onto the third polarizing beam splitter. The interference beam with the wavelength λ₂ reflected by the third polarizing beam splitter is received by the first photodetector, and the interference beam with the wavelength λ₁ transmitted by the third polarizing beam splitter is received by the second photodetector. The interference signals output by the two photodetectors are respectively sent to the data acquisition module, and then transmitted to the computer after being processed by the data acquisition module. According to the calculated result, the computer changes the value of the wavelength λ₂ emitted from the second laser by means of the controller.

In the light source system, the wavelength λ₁ of the laser beam emitted from the first laser is a constant value and the wavelength λ₂ of the laser beam emitted from the second laser is a variable value.

In the wavelength-leverage laser interferometric system, the reference arm is composed of the second polarizing beam splitter and the first cube-corner prism while the measurement arm is composed of the second beam splitter, the first shutter, the second shutter, the second reflector, the third reflector, the third beam splitter, the second cube-corner prism and the third cube-corner prism.

In the wavelength-leverage laser interferometric system, there is a one-to-one correspondence between the synthetic wavelength λ_S formed by the linearly polarized beams with the wavelengths λ₁, and λ₂ in the measurement arm and the wavelength λ₁ of the linearly polarized beam projecting onto the first cube-corner prism in the reference arm. The measured absolute distance in the measurement arm and the moving displacement of the first cube-corner prism in the reference arm form a leverage relationship.

2. An absolute distance measurement method using laser interferometric wavelength leverage: the method adopts the apparatus to perform measurement, and the specific steps are as follows:

1) The first laser emits the linearly polarized beam with the wavelength λ₁. Controlling the second laser to emit the linearly polarized beam with the wavelength λ₂ makes one half of the primary synthetic wavelength λ_S1 formed by the wavelengths λ₁ and λ₂ be larger than the measured absolute distance L which is the distance between the second cube-corner prism and the third cube-corner prism;

2) Adjust the open and close states of the first shutter and the second shutter. Move the first cube-corner prism along the axial direction of light path. Establish the wavelength-leverage relationship. The primary coarse measurement value of the measured absolute distance is achieved;

3) Keep the wavelength λ₁ output from the first laser constant. The computer changes the wavelength λ₂ output from the second laser by means of the controller so that the wavelength λ₁ and the wavelength λ₂ form a series of synthetic wavelengths λ_S2, λ_S3, . . . , λ_Si, . . . , λ_Sn. The measurement is performed repeatedly with respect to each change of the wavelength λ₂. The fractional fringe order ε_Si and the integral fringe order M_Si of the synthetic wavelength included in the measured absolute distance L are obtained through calculation;

4) According to the synthetic wavelength and its fractional fringe order ε_Si and integral fringe order M_Si obtained in the above steps, the computer calculates each estimate value of the measured absolute distance L during each measurement. The measured absolute distance L is obtained through calculation. Then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

Step 2) specifically includes;

2.1) When the first shutter is opened and the second shutter is closed, the near-end measurement beam returned from the second cube-corner prism and the reference beam form the interference signals. Moving the first cube-corner prism along the axial direction of light path makes the phase difference Δφ between the interference signals of wavelengths λ₂ and λ₁ detected respectively by the first photodetector and the second photodetector be equal to zero;

2.2) When the first shutter is closed and the second shutter is opened, the far-end measurement beam returned from the third cube-corner prism and the reference beam form the interference signals. The phase difference Δφ between the two interference signals received by the first photodetector and the second photodetector is changed. Moving again the first cube-corner prism along the axial direction of light path makes the phase difference Δφ be equal to zero. The moving displacement of the first cube-corner prism is recorded as Δl;

2.3) The wavelength-leverage relationship among the primary synthetic wavelength λ_S1, the wavelength λ₁ output from the first laser, the measured absolute distance L and the moving displacement Δl of the first cube-corner prism is established as follows:

$\frac{L}{{\lambda }_{S1}}=\frac{\Delta l}{{\lambda }_1}$

where λ_S1=λ₁λ₂/|λ₁−λ₂| is the primary synthetic wavelength formed by the wavelengths λ₁ and λ₂. λ₁ and λ₂ are the wavelengths output from the first laser and the second laser, respectively;

According to the wavelength-leverage relationship, the primary coarse measurement value L₁ of the measured absolute distance is calculated by the computer using the following equation:

$L_1=\frac{{\lambda }_{S1}}{{\lambda }_1}·\Delta l.$

Step 3) specifically includes:

A series of synthetic wavelengths meets λ_S2, >λ_S3> . . . >λ_Sn, and each synthetic wavelength λ_Si meets

λ_Si>4u(L_i-1′), i=2,3, . . . ,n

where i represents the sequence number of measurement times, n represents the total number of measurement times, L_i-1′) is the estimate value of the measured distance, and u(L_i-1′) is the measurement uncertainty of the estimate value L_i-1′ of the measured distance when the synthetic wavelength is λ_Si-1; when i=2, L_i-1′=L₁, namely L₁′=L₁;

For each synthetic wavelength λ_Si, repeat Step 2). When the wavelength λ₂ of the second laser is changed, the moving displacement of the first cube-corner prism is recorded as Δl_i during each measurement. The following approach is adopted to perform measurement during each measurement:

According to the wavelength-leverage relationship, the coarse measurement value L_i of the measured absolute distance corresponding to the fractional part of the synthetic wavelength λ_Si is calculated by the computer using the following equation:

$L_i=\frac{{\lambda }_{Si}}{{\lambda }_1}·\Delta l_i$

With the coarse measurement value L_i of the measured absolute distance, the fractional fringe order ε_Si of the synthetic wavelength λ_Si included in the measured absolute distance L is calculated by the computer using the following equation:

${\varepsilon }_{\mathrm{Si}}=\frac{2L_i}{{\lambda }_{\mathrm{Si}}}$

Then, with the estimate value L_i-1′ of the measured absolute distance and the fractional fringe order ε_Si of the synthetic wavelength λ_Si, the integral fringe order M_Si of the synthetic wavelength λ_Si included in the measured absolute distance is calculated by the computer using the following equation:

$M_{\mathrm{Si}}=\mathrm{int}\left[\frac{2L_{i-1}^{\prime }}{{\lambda }_{\mathrm{Si}}}+0.5-{\varepsilon }_{\mathrm{Si}}\right]$

where int[ ] is rounded down.

Step 4) specifically includes:

4.1) For the measuring process with respect to i=2, 3, . . . , n, each estimate value L_i′ of the measured absolute distance L is calculated by the computer using the following equation:

$L_i^{\prime }=\left(M_{\mathrm{Si}}+{\varepsilon }_{\mathrm{Si}}\right)·\frac{{\lambda }_{\mathrm{Si}}}{2}$

When 4u(L_n′)<λ₁ is satisfied, where u(L_n′) is the measurement uncertainty of the estimate value L_n′ of the measured absolute distance when the final synthetic wavelength is λ_Sn, the measured absolute distance L is calculated by the computer using the following equation:

$L=\left(M_n+{\varepsilon }_n\right)·\frac{{\lambda }_1}{2}$

where M_n represents the integral fringe order of the wavelength λ₁ included in the measured absolute distance L, ε_n represents the fractional fringe order of the wavelength λ₁ included in the measured absolute distance L, and M_n and ε_n are respectively calculated by using the following equations:

$M_n=\mathrm{int}\left[\frac{2L_n^{\prime }}{{\lambda }_1}+0.5-{\varepsilon }_n\right]$ ${\varepsilon }_n=\frac{2\Delta l_n}{{\lambda }_1}$

where L_n′ is the estimate value of the measured absolute distance L and Δl_n is the moving displacement of the first cube-corner prism in the final measurement.

The wavelength λ₁ output from the first laser is a fixed wavelength and the wavelength λ₂ output from the second laser can be changed.

Compared with the background of the invention, the present invention has the advantages that:

(1) Using the wavelength leverage principle, the measured distance of large length is converted into the measurement of easily detected displacement of the cube-corner prism in the reference arm, instead of acquiring the fractional fringe order of the synthetic wavelength through phase determination. The method is easy to realize;

(2) The method can realize the absolute measurement of arbitrary distance. And when the synthetic wavelength is gradually decreased and transited to the single wavelength, the measurement accuracy of the measured distance can reach nanometer level. Thus the method has high measurement accuracy.

(3) The method can realize the transition from synthetic wavelength to single wavelength. The method is simple in structure, low in cost and convenient to use.

The present invention is mainly applied to the measurement of absolute distance of large length or large size with high accuracy in the field of large precision equipment manufacturing, spatial engineering and metrological technique.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is the optical configuration of the present invention.

FIG. 2 is the schematic diagram of the absolute distance measurement using wavelength leverage of the present invention.

In the figures: 10. first laser, 11. second laser, 12. first beam expander, 13. second beam expander, 14. first reflector, 15. first polarizing beam splitter, 20. first beam splitter, 21. second polarizing beam splitter, 22. first cube-corner prism, 23. second beam splitter, 24. first shutter, 25. second shutter, 26. second reflector, 27. third reflector, 28. third beam splitter, 29. second cube-corner prism, 210. third cube-corner prism, 30. third polarizing beam splitter, 31. first photodetector, 32. second photodetector, 33. data acquisition module, 34. computer, and 35. controller.

DETAILED DESCRIPTION OF THE INVENTION

The present invention is further described in details hereinafter with the Figures and Embodiments.

As shown in FIG. 1, the apparatus of the present invention comprises a light source system I, a wavelength-leverage laser interferometric system II and an interference signal processing and controlling system III. The light source system I outputs a orthogonally linearly polarized beam with the wavelength λ₁ and wavelength λ₂. The orthogonally linearly polarized beam projects onto the wavelength-leverage laser interferometric system II to form the interference beam. The interference beam projects onto the interference signal processing and controlling system III. The controller 35 in the interference signal processing and controlling system III is used for controlling the change of the wavelength λ₂ in the light source system I.

The light source system I comprises a first laser 10, a second laser 11, a first beam expander 12, a second beam expander 13, a first reflector 14 and a first polarizing beam splitter 15. The linearly polarized beam with a constant wavelength λ₁ and the polarization direction parallel to the page plane emitted from the first laser 10 passes through the first beam expander 12 and projects onto the first polarizing beam splitter 15. The linearly polarized beam with a variable wavelength λ₂ and the polarization direction perpendicular to the page plane emitted from the second laser 11 passes through the second beam expander 13, is reflected by the first reflector 14 and projects onto the first polarizing beam splitter 15. The polarization direction of the beam from the first laser 10 is perpendicular to that of the beam from the second laser 11. In FIG. 1, the vertical short line in the light path represents the beam with the wavelength λ₁ whose polarization direction is parallel to the page plane, and the black dot represents the beam with the wavelength λ₂ whose polarization direction is perpendicular to the page plane. The linearly polarized beam with the wavelength λ₁ transmitted by the first polarizing beam splitter 15 and the linearly polarized beam with the wavelength λ₂ reflected by the first polarizing beam splitter 15 combine one orthogonally linearly polarized beam.

The wavelength-leverage laser interferometric system II comprises a first beam splitter 20, a second polarizing beam splitter 21, a first cube-corner prism 22, a second beam splitter 23, a first shutter 24, a second shutter 25, a second reflector 26, a third reflector 27, a third beam splitter 28, a second cube-corner prism 29 and a third cube-corner prism 210. Being incident on the first beam splitter 20, the orthogonally linearly polarized beam is divided into the reflected reference beam and the transmitted measurement beam. The reference beam projects onto the second polarizing beam splitter 21, wherein the linearly polarized beam with the wavelength λ₂ is reflected twice by the second polarizing beam splitter 21 and projects onto the first beam splitter 20, and the linearly polarized beam with the wavelength λ₂ passes through the second polarizing beam splitter 21, projects onto the first cube-corner prism 22, returns after being reflected, and projects onto the first beam splitter 20 after passing through the second polarizing beam splitter 21 again. Being incident on the second beam splitter 23, the measurement beam is divided into the reflected near-end measurement beam and the transmitted far-end measurement beam. The near-end measurement beam projects onto the first beam splitter 20 after passing through the first shutter 24, the second reflector 26, the second cube-corner prism 29 and the third beam splitter 28 in sequence. And the far-end measurement beam projects onto the first beam splitter 20 after passing through the second shutter 25, the third cube-corner prism 210, the third reflector 27 and the third beam splitter 28 in sequence. Being reflected by the first beam splitter 20, the near-end or far-end measurement beam recombines with the reference beam transmitted by the first beam splitter 20 to form the interference beam.

The interference signal processing and controlling system III comprises a third polarizing beam splitter 30, a first photodetector 31, a second photodetector 32, a data acquisition module 33, a computer 34 and a controller 35. The interference beam from the wavelength-leverage laser interferometric system II projects onto the third polarizing beam splitter 30. The interference beam with the wavelength λ₂ reflected by the third polarizing beam splitter 30 is received by the first photodetector 31, and the interference beam with the wavelength λ₁ transmitted by the third polarizing beam splitter 30 is received by the second photodetector 32. The interference signals output by the two photodetectors are respectively sent to the data acquisition module 33, and then transmitted to the computer 34 after being processed by the data acquisition module 33. According to the calculated result, the computer 34 changes the value of the wavelength λ₂ emitted from the second laser 11 by means of the controller 35.

In the light source system I, the wavelength λ₁ of the beam emitted from the first laser 10 is a constant value and the wavelength λ₂ of the beam emitted from the second laser 11 is a variable value.

In the wavelength-leverage laser interferometric system II, the reference arm is composed of the second polarizing beam splitter 21 and the first cube-corner prism 22 while the measurement arm is composed of the second beam splitter 23, the first shutter 24, the second shutter 25, the second reflector 26, the third reflector 27, the third beam splitter 28, the second cube-corner prism 29 and the third cube-corner prism 210.

In the wavelength-leverage laser interferometric system II, there is a one-to-one correspondence between the synthetic wavelength λ_S formed by the linearly polarized beams with the wavelengths λ₁ and λ₂ in the measurement arm and the wavelength λ₁ of the linearly polarized beam projecting onto the first cube-corner prism 22 in the reference arm. The measured absolute distance in the measurement arm and the moving displacement of the first cube-corner prism 22 in the reference arm form a leverage relationship.

In the wavelength-leverage laser interferometric system II, when the first shutter 24 is opened and the second shutter 25 is closed, the near-end measurement beam incident on the first beam splitter 20 and the reference beam incident on the first beam splitter 20 form interference. When the first shutter 24 is closed and the second shutter 25 is opened, the far-end measurement beam incident on the first beam splitter 20 and the reference beam incident on the first beam splitter 20 form interference. That is, the near-end measurement beam and the far-end measurement beam respectively interfere with the reference beam by alternately opening and closing the first shutter 24 and the second shutter 25.

In the embodiment of the present invention, the first laser 10, which is one tunable diode laser with the model of DL Pro 633 made by Toptica Company from Germany, emits the constant wavelength λ₁ of 631 nm. The second laser 11, which is another tunable diode laser with the model of DL Pro 633 made by Toptica Company from Germany, emits the wavelength λ₂ with the range of 630 nm-637 nm. The first photodetector 31 and the second photodetector 32 are PIN photodetectors with the model of S09105 made by Beijing Suoyang Photoelectric Technology Co., Ltd. The data acquisition module 33 is a data acquisition card with the model of PCI-9820 made by Adlink Technology Company. The computer 34 is a desktop computer with the model of Pro4500 made by the HP Company. And the controller 35 is a controller with the model of Digilock110 made by Toptica Company from Germany.

Combined with FIG. 2, the specific implementation for measuring absolute distance using laser interferometric wavelength leverage includes the following steps:

1) The first laser 10 emits the linearly polarized beam with a constant wavelength λ₁. Controlling the second laser 11 to emit the linearly polarized beam with a variable wavelength λ₂ makes one half of the primary synthetic wavelength λ_S1 formed by the wavelengths λ₁ and λ₂ be larger than the measured absolute distance L, which is the distance between the second cube-corner prism 29 and the third cube-corner prism 210;

2) Adjust the open and close states of the first shutter 24 and the second shutter 25. Move the first cube-corner prism 22 along the axial direction of light path. Establish the wavelength-leverage relationship. The primary coarse measurement value of the measured absolute distance is achieved;

2.1) When the first shutter 24 is opened and the second shutter 25 is closed, the near-end measurement beam returned from the second cube-corner prism 29 interferes with the reference beam. The interference signals of the wavelength λ₂ and wavelength λ₁ detected respectively by the first photodetector 31 and the second photodetector 32 are respectively shown as follows:

$\begin{array}{cc}{\varphi }_2=4\pi \frac{L_R}{{\lambda }_2}& \left(1\right)\\ {\varphi }_1=4\pi \left(\frac{L_R}{{\lambda }_1}-\frac{L_M}{{\lambda }_1}\right)& \left(2\right)\end{array}$

where φ₁ and φ₂ are the phases of the interference signals of the wavelengths λ₁ and λ₂ detected by the first photodetector 31 and the second photodetector 32, respectively. L_R is the distance difference between the first beam splitter 20 to the second cube-corner prism 29 and the first beam splitter 20 to the second polarizing beam splitter 21. And L_M is the distance between the second polarizing beam splitter 21 and the first cube-corner prism 22. λ₁ and λ₂ are the laser wavelengths in the air, λ₁=λ₁₀/n₁ and λ₂=λ₂₀/n₂ (λ₁₀ and λ₂₂ are the laser wavelengths in the vacuum, n₁ and n₂ are the refractive index of air, n₁ and n₂ are calculated with the Edlen equation by measuring the temperature, humidity, pressure and CO₂ concentration of the air);

Moving the first cube-corner prism 22 along the axial direction of light path makes the phase difference between the two interference signals determined by the data acquisition module 33 be equal to zero, that is, there is:

$\begin{array}{cc}\mathrm{\Delta \varphi }={\varphi }_2-{\varphi }_1=4\pi \left(\frac{L_R}{{\lambda }_{S1}}+\frac{L_{M1}}{{\lambda }_1}\right)=0& \left(3\right)\end{array}$

where L_M1 is the distance between the second polarizing beam splitter 21 and the first cube-corner prism 22 with respect to the primary synthetic wavelength; λ_S1=λ₁λ₂/|λ₁−λ₂| is the primary synthetic wavelength formed by λ₁ and λ₂;

2.2) When the first shutter 24 is closed and the second shutter 25 is opened, the far-end measurement beam returned from the third cube-corner prism 210 interferes with the reference beam. As the measured distance L is introduced, the phase difference Δφ′ between the two interference signals is changed as follows:

$\begin{array}{cc}{\mathrm{\Delta \varphi }}^{\prime }=4\pi \left(\frac{L_R+L}{{\lambda }_{S1}}+\frac{L_{M1}}{{\lambda }_1}\right)& \left(4\right)\end{array}$

In order to measure the measured distance L, the first cube-corner prism 22 is moved a smaller distance Δl (less than λ₁/2) along the axial direction of light path, namely L_M1→L_M1±Δl. The phase difference Δφ″ between the two interference signals is changed as follows:

$\begin{array}{cc}{\mathrm{\Delta \varphi }}^{″}=4\pi \left(\frac{L_R+L}{{\lambda }_{S1}}+\frac{L_{M1}\pm \Delta l}{{\lambda }_1}\right)& \left(5\right)\end{array}$

When λ₂>/λ₁, the first cube-corner prism 22 moves towards the second polarizing beam splitter 21, and the sign before Δl is plus. When λ₂</λ₁, the first cube-corner prism 22 moves far away from the second polarizing beam splitter 21, and the sign before Δl is minus;

2.3) The smaller distance Δl moved by the first cube-corner prism 22 shall satisfy to make Δφ″=0. According to Eq. (3) and Eq. (5), the wavelength-leverage relationship among the primary synthetic wavelength λ_S1 the wavelength λ₁, the measured absolute distance L and the moving displacement Δl of the first cube-corner prism 22 is established as follows:

$\begin{array}{cc}\frac{L}{{\lambda }_{S1}}+\frac{\Delta l}{{\lambda }_1}& \left(6\right)\end{array}$

The wavelength-leverage relationship is shown in FIG. 2. The primary coarse measurement value L₁ of the measured absolute distance is calculated by the computer 34 as follows:

$\begin{array}{cc}{L}_1=\frac{{\lambda }_{S1}}{{\lambda }_1}·\Delta l& \left(7\right)\end{array}$

3) Keep the wavelength λ₁ output from the first laser 10 constant. The computer 34 changes the wavelength λ₂ output from the second laser 11 by means of the controller 35 so that the wavelength λ₁ and the wavelength λ₂ form a series of synthetic wavelengths λ_S2, λ_S3, . . . , λ_Si, . . . , λ_Sn. The measurement is performed repeatedly with respect to each change of the wavelength λ₂. The fractional fringe order ε_Si and the integral fringe order M_Si of the synthetic wavelength λ_Si included in the measured absolute distance L are obtained through calculation;

A series of synthetic wavelengths meets λ_S2>λ_S3> . . . >λ_Sn, and each synthetic wavelength λ_Si meets:

λ_Si>4u(L_i-1′), i=2,3, . . . ,n

where i represents the sequence number of measurement times, n represents the total number of measurement times, L_i-1′ is the estimate value of the measured distance, and u(L_i-1′) is the measurement uncertainty of the estimate value L_i-1′ of the measured distance when the synthetic wavelength is λ_Si-1 (when i=L_i-1′=L₁, that is L₁′=L₁);

For each synthetic wavelengths λ_Si, repeat Steps 2.1) and 2.2). When the wavelength λ₂ of the second laser 11 is changed every time, the moving displacement of the first cube-corner prism 22 is recorded as Δl_i. According to Eq. (4), the phase difference Δφ′″ between the two interference signals during each measurement is changed to:

$\begin{array}{cc}{\mathrm{\Delta \varphi }}^{\mathrm{\prime \prime \prime }}=4\pi \left(\frac{L_R+L_i^{\prime }}{{\lambda }_{\mathrm{Si}}}+\frac{L_{Mi}}{{\lambda }_1}\right)& \left(8\right)\end{array}$

where L_i′ is the estimate value of the measured distance L, and L_Mi is the distance between the second polarizing beam splitter 21 and the first cube-corner prism 22 with respect to the synthetic wavelength λ_Si;

In Eq. (8), when the measured distance L is larger than λ_Si/2, Δφ′″ includes the integral number and the fractional part of 2π. Δφ′″ is expressed as another expression:

$\begin{array}{cc}{\mathrm{\Delta \varphi }}^{\mathrm{\prime \prime \prime }}=2\pi \left(M_{\mathrm{Si}}+{\varepsilon }_{\mathrm{Si}}\right)+4\pi \left(\frac{L_R}{{\lambda }_{\mathrm{Si}}}+\frac{L_{Mi}}{{\lambda }_1}\right)& \left(9\right)\end{array}$

According to Eq. (8) and Eq. (9), the estimate value L_i′ of the measured distance is expressed as:

$\begin{array}{cc}{L}_i^{\prime }=\left(M_{\mathrm{Si}}+{\varepsilon }_{\mathrm{Si}}\right)·\frac{{\lambda }_{\mathrm{Si}}}{2}& \left(10\right)\end{array}$

where M_n and ε_n respectively represent the integral fringe order and the fractional fringe order of the synthetic wavelength λ_Si included in the measured distance;

Repeat Step 2.3). the coarse measurement value L_i of the measured absolute distance corresponding to the fractional part of the synthetic wavelength λ_Si is calculated by the computer 34 as follows:

$\begin{array}{cc}{L}_i=\frac{{\lambda }_{\mathrm{Si}}}{{\lambda }_1}·\Delta l_i& \left(11\right)\end{array}$

The fractional fringe order of the synthetic wavelength λ_Si included in the measured absolute distance L is given by:

$\begin{array}{cc}{\varepsilon }_{\mathrm{Si}}=\frac{2L_i}{{\lambda }_{\mathrm{Si}}}& \left(12\right)\end{array}$

With the estimate value L_i-1′ of the measured absolute distance determined by last synthetic wavelength λ_Si-1 and the fractional fringe order ε_Si currently determined, the integral fringe order M_Si of the synthetic wavelength λ_Si included in the measured absolute distance L is given by:

$\begin{array}{cc}{M}_{\mathrm{Si}}=\mathrm{int}\left[\frac{2L_{i-1}^{\prime }}{{\lambda }_{\mathrm{Si}}}+0.5-{\varepsilon }_{\mathrm{Si}}\right]& \left(13\right)\end{array}$

where int[ ] is rounded down.

4) According to the synthetic wavelength λ_Si and its fractional fringe order ε_Si and integral fringe order M_Si obtained in the above steps, the computer 34 calculates each estimate value of the measured absolute distance L during each measurement. The measured absolute distance L is obtained through calculation. Then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

4.1) For i=2, 3, . . . , n, substituting the obtained M_Si and ε_Si into Eq. (10), the estimate value L_i′ of the measured absolute distance corresponding to the synthetic wavelength λ_Si is calculated by the computer 34;

Substituting Eq. (11) into Eq. (12), we get:

$\begin{array}{cc}{\varepsilon }_{\mathrm{Si}}=\frac{2\Delta l_i}{{\lambda }_1}& \left(14\right)\end{array}$

Substituting Eq. (14) into Eq. (10), we get:

$\begin{array}{cc}{L}_i^{\prime }=M_{\mathrm{Si}}·\frac{{\lambda }_{\mathrm{Si}}}{2}+\frac{{\lambda }_{\mathrm{Si}}}{{\lambda }_1}·\Delta l_i& \left(15\right)\end{array}$

From Eq. (15), the measurement uncertainty of the estimate value L_i′ of the measured absolute distance is derived as follows:

$\begin{array}{cc}u\left(L_i^{\prime }\right)=\sqrt{\begin{array}{c}{\left(\frac{M_{\mathrm{Si}}}{2}·u\left({\lambda }_{\mathrm{Si}}\right)\right)}^2+{\left(\frac{{\lambda }_{\mathrm{Si}}}{{\lambda }_1}·u\left(\Delta l_i\right)\right)}^2+{\left(\frac{\Delta l_i}{{\lambda }_1}·u\left({\lambda }_{\mathrm{Si}}\right)\right)}^2+\\ {\left(\frac{\Delta l_i{\lambda }_{\mathrm{Si}}}{{\lambda }_1^2}·u\left({\lambda }_1\right)\right)}^2\end{array}}& \left(16\right)\end{array}$

Equation (16) shows that the measurement uncertainty u(L_i′) of the estimate value L_i′ of the measured absolute distance depends on the integer value M_Si of the synthetic wavelength λ_Si, the uncertainty u(λ_Si) of the synthetic wavelength λ_Si, the uncertainty u(λ₁) of the wavelength λ₁ and the uncertainty u(Δl_i) of the moving displacement Δl_i of the first cube-corner prism 22;

For different i, repeat Step 2). When the condition of 4u(L_n′)<λ₁ is satisfied, the measured absolute distance is calculated by the computer 34 according to the following equation:

$\begin{array}{cc}L=\left(M_n+{\varepsilon }_n\right)·\frac{{\lambda }_1}{2}& \left(17\right)\end{array}$

where M represents the integral fringe order of the wavelength λ₁ included in the measured absolute distance L, ε_n represents the fractional fringe order of the wavelength λ₁ included in the measured absolute distance L, and M_n and ε_n are respectively calculated by using the following equations:

$M_n=\mathrm{int}\left[\frac{2L_n^{\prime }}{{\lambda }_1}+0.5-{\varepsilon }_n\right]{\varepsilon }_n=\frac{2\Delta l_n}{{\lambda }_1}$

where L_n′ is the estimate value of the measured absolute distance L and Δl_n is the moving displacement of the first cube-corner prism 22 in the final measurement.

For the case that the condition of 4u(L_n′)<λ₁ is not satisfied, Step 3) is continuously repeated until the condition of 4u(L_n′)<λ₁ is satisfied, then the measured absolute distance L is calculated by using Eq. (17).

The absolute distance of 50 m is measured as an example. When the wavelength λ₁ output from the first laser 10 is equal to 631 m, u(λl_i) is equal to 0.0004 μm, the relative uncertainty of the vacuum wavelengths λ₁₀ and λ₂₀ is 10⁻¹⁰ and the relative uncertainty of the measurement of the air refractive index is 10⁻⁹, the relative uncertainty of the wavelengths λ₁, λ₂ and λ_Si in the air is 10⁻⁹, after measurements with four synthetic wavelengths are performed, the measurement uncertainty of the measured absolute distance reaches 0.04 μm, this satisfies the condition of 4u(L_n′)<λ₁. The specific data is shown in Table 1.

TABLE 1
Four synthetic wavelength values and corresponding measurement
results when the measured absolute distance L = 50 m
			Moving
			displacement	Estimate value		Relative
		Synthetic	Δli of first	Li′ of the	Measurement	measurement
	Wavelength	wavelength	cube-corner	absolute	uncertainty	accuracy of
	λ2	λSi	prism 22	distance	u(Li′)	the distance
No.	(nm)	(μm)	(μm)	(μm)	(μm)	L − Li′/L
1	631.0000020	199861638.70	0.1576	49917898.98	95021.38	1.64 × 10−3
2	631.0002656	1498962.29	0.2248	49999775.43	712.66	4.49 × 10−6
3	631.0332048	11991.70	0.0321	49999996.18	5.70	7.63 × 10−8
4	635.6829255	85.65	0.1048	49999999.96	0.06	8.76 × 10−10

According to Eq. (17), the measured absolute distance L=49999999.98 μm is obtained through calculation, and the relative accuracy of the measurement of the absolute distance is 3.54×10⁻¹⁰.

From the above description, these show that the present invention has realized precision measurement of the absolute distance of large length. The present invention has the advantages of high measurement accuracy, simple optical configuration, convenient to use and remarkable technical effects.

The above embodiment is intended to explain the present invention, but not to limit the present invention. Any modification and change made to the present invention within the protection scope of the spirit and the Claims of the present invention fall in the protection scope of the present invention.

Claims

1. An absolute distance measurement apparatus using laser interferometric wavelength leverage, comprising a light source system (I), a wavelength-leverage laser interferometric system (II) and an interference signal processing and controlling system (III), wherein the light source system (I) outputs a orthogonally linearly polarized beam with the wavelength λ1 and wavelength λ2, the orthogonally linearly polarized beam projects onto the wavelength-leverage laser interferometric system (II) to form the interference beam, the interference beam projects onto the interference signal processing and controlling system (III), and the controller in the interference signal processing and controlling system (III) is used for controlling the change of the wavelength λ2 in the light source system (I).

2. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 1, wherein the light source system (I) comprises a first laser (10), a second laser (11), a first beam expander (12), a second beam expander (13), a first reflector (14) and a first polarizing beam splitter (15), wherein the linearly polarized beam with a constant wavelength λ1 emitted from the first laser (10) passes through the first beam expander (12) and projects onto the first polarizing beam splitter (15), the linearly polarized beam with a variable wavelength λ2 emitted from the second laser (11), whose polarization direction is perpendicular to that of the beam from the first laser (10), passes through the second beam expander (13), is reflected by the first reflector (14) and projects onto the first polarizing beam splitter (15), and the linearly polarized beam with the constant wavelength λ1 transmitted by the first polarizing beam splitter (15) and the linearly polarized beam with the variable wavelength λ2 reflected by the first polarizing beam splitter (15) combine one orthogonally linearly polarized beam.

3. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 1, wherein the wavelength-leverage laser interferometric system (II) comprises a first beam splitter (20), a second polarizing beam splitter (21), a first cube-corner prism (22), a second beam splitter (23), a first shutter (24), a second shutter (25), a second reflector (26), a third reflector (27), a third beam splitter (28), a second cube-corner prism (29) and a third cube-corner prism (210), wherein being incident on the first beam splitter (20), the orthogonally linearly polarized beam is divided into the reflected reference beam and the transmitted measurement beam, wherein the reflected reference beam projects onto the second polarizing beam splitter (21), wherein the linearly polarized beam with the wavelength λ2 is reflected twice by the second polarizing beam splitter (21) and projects onto the first beam splitter (20), and the linearly polarized beam with the wavelength λ1 passes through the second polarizing beam splitter (21), projects onto the first cube-corner prism (22), returns after being reflected, and projects onto the first beam splitter (20) after passing through the second polarizing beam splitter (21) again, wherein being incident on the second beam splitter (23), the transmitted measurement beam is divided into the reflected near-end measurement beam and the transmitted far-end measurement beam, wherein the near-end measurement beam projects onto the first beam splitter (20) after passing through the first shutter (24), the second reflector (26), the second cube-corner prism (29) and the third beam splitter (28) n sequence, and the far-end measurement beam projects onto the first beam splitter (20) after passing through the second shutter (25), the third cube-corner prism (210), the third reflector (27) and the third beam splitter (28) in sequence, wherein being reflected by the first beam splitter (20), the near-end or far-end measurement beam recombines with the reference beam transmitted by the first beam splitter (20) to form the interference beam.

4. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 1, wherein the interference signal processing and controlling system (III) comprises a third polarizing beam splitter (30), a first photodetector (31), a second photodetector (32), a data acquisition module (33), a computer (34) and a controller (35), wherein the interference beam from the wavelength-leverage laser interferometric system (II) projects onto the third polarizing beam splitter (30), wherein the interference beam with the wavelength λ2 reflected by the third polarizing beam splitter (30) is received by the first photodetector (31), and the interference beam with the wavelength λ1 transmitted by the third polarizing beam splitter (30) is received by the second photodetector (32), wherein the interference signals output by the two photodetectors are respectively sent to the data acquisition module (33), and then transmitted to the computer (34) after being processed by the data acquisition module (33), wherein according to the calculated result, the computer (34) changes the value of the wavelength λ2 emitted from the second laser (11) by means of the controller (35).

5. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 2, wherein in the light source system (I), the wavelength λ1 of the laser beam emitted from the first laser (10) is a constant value and the wavelength λ2 of the laser beam emitted from the second laser (11) is a variable value.

6. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 3, wherein in the wavelength-leverage laser interferometric system (II), the reference arm is composed of the second polarizing beam splitter (21) and the first cube-corner prism (22) while the measurement arm is composed of the second beam splitter (23), the first shutter (24), the second shutter (25), the second reflector (26), the third reflector (27), the third beam splitter (28), the second cube-corner prism (29) and the third cube-corner prism (210).

7. The absolute distance measurement apparatus using laser interferometric wavelength leverage according to claim 3, wherein in the wavelength-leverage laser interferometric system (II), there is a one-to-one correspondence between the synthetic wavelength λS formed by the linearly polarized beams with the wavelengths λ1 and λ2 in the measurement arm and the wavelength λ1 of the linearly polarized beam projecting onto the first cube-corner prism (22) in the reference arm, wherein the measured absolute distance in the measurement arm and the moving displacement of the first cube-corner prism (22) in the reference arm form a leverage relationship.

8. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 1, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

9. The absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 8, wherein Step 2) specifically includes: 2.1) When the first shutter (24) is opened and the second shutter (25) is closed, the near-end measurement beam returned from the second cube-corner prism (29) and the reference beam form the interference signals, and moving the first cube-corner prism (22) along the axial direction of light path makes the phase difference Δφ between the interference signals of wavelengths λ2 and λ1 detected respectively by the first photodetector (31) and the second photodetector (32) be equal to zero;2.2) When the first shutter (24) is closed and the second shutter (25) is opened, the far-end measurement beam returned from the third cube-corner prism (210) and the reference beam form the interference signals, wherein the phase difference Δφ between the two interference signals received by the first photodetector (31) and the second photodetector (32) is changed. Moving again the first cube-corner prism (22) along the axial direction of light path makes the phase difference Δφ be equal to zero, wherein the moving displacement of the first cube-corner prism (22) is recorded as Δl;2.3) The wavelength-leverage relationship among the primary synthetic wavelength λS1, the wavelength λ1 output from the first laser (10), the measured absolute distance L and the moving displacement Δl of the first cube-corner prism (22) is established as follows:

10. The absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 8, wherein Step 3) specifically includes: A series of synthetic wavelengths meets λS2>λS3> . . . >λSn, and each synthetic wavelength λSi meets λSi>4u(Li-1′), i=2,3, . . . ,n

11. The absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 8, wherein Step 4) specifically includes: 4.1) For the measuring process with respect to i=2, 3, . . . , n, each estimate value Li′ of the measured absolute distance L is calculated by the computer (34) using the following equation:

12. The absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 8, wherein the wavelength λ1 output from the first laser (10) is a fixed wavelength and the wavelength λ2 output from the second laser (11) can be changed.

13. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 2, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

14. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 3, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

15. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 4, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

16. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 5, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λS1 and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

17. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 6, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.

18. An absolute distance measurement method using laser interferometric wavelength leverage applied to the apparatus according to claim 7, wherein the method adopts the apparatus to perform measurement, and the specific steps are as follows: 1) The first laser (10) emits the linearly polarized beam with the wavelength, wherein controlling the second laser (11) to emit the linearly polarized beam with the wavelength λ2 makes one half of the primary synthetic wavelength λS1 formed by the wavelengths λ1 and λ2 be larger than the measured absolute distance L which is the distance between the second cube-corner prism (29) and the third cube-corner prism (210);2) Adjust the open and close states of the first shutter (24) and the second shutter (25), move the first cube-corner prism (22) along the axial direction of light path, and establish the wavelength-leverage relationship, wherein the primary coarse measurement value of the measured absolute distance is achieved;3) Keep the wavelength λ1 output from the first laser (10) constant, wherein the computer (34) changes the wavelength λ2 output from the second laser (11) by means of the controller (35) so that the wavelength λ1 and the wavelength λ2 form a series of synthetic wavelengths λS2, λS3, . . . , λSi, . . . , λSn, wherein the measurement is performed repeatedly with respect to each change of the wavelength λ2, wherein the fractional fringe order εSi and the integral fringe order MSi of the synthetic wavelength λSi included in the measured absolute distance L are obtained through calculation;4) According to the synthetic wavelength λSi and its fractional fringe order εSi and integral fringe order MSi obtained in the above steps, the computer (34) calculates each estimate value of the measured absolute distance L during each measurement, wherein the measured absolute distance L is obtained through calculation, and then the measurement of absolute distance using laser interferometric wavelength leverage is realized.