CN103528525B - Three-optical axis compensation and air bath type linear displacement laser interferometer calibration method and device - Google Patents

Three-optical axis compensation and air bath type linear displacement laser interferometer calibration method and device Download PDF

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CN103528525B
CN103528525B CN201310475481.7A CN201310475481A CN103528525B CN 103528525 B CN103528525 B CN 103528525B CN 201310475481 A CN201310475481 A CN 201310475481A CN 103528525 B CN103528525 B CN 103528525B
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laser interferometer
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CN103528525A (en
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胡鹏程
谭久彬
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Harbin Institute of Technology
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Abstract

The invention discloses a three-optical axis compensation and air bath type linear displacement laser interferometer calibration method and a three-optical axis compensation and air bath type linear displacement laser interferometer calibration device, and belongs to the technical field of laser measurement. Measurement light beams of a calibrated laser interferometer penetrate through a middle through hole of a three-axis hollow laser interference mirror group, and are arranged in parallel at the central positions of three parallel standard measurement light beams which are distributed as side edges of a regular triangular prism; the standard measurement light beams are at short perpendicular distances away from the measurement light beams of the calibrated laser interferometer, and an average air refractivity value of the three standard measurement light beams is approximate to air refractivity values of the measurement light beams of the calibrated laser interferometer; air temperature, air humidity and air pressure in a stable air bath environment formed by an air bath device are approximately uniformly distributed, so that the average air refractivity value of the three standard measurement light beams is more approximate to the air refractivity values of the measurement light beams of the calibrated laser interferometer; a measurement error caused by the surface appearance of the reflecting surface of a target reflector is compensated into a linear displacement measurement result to ensure the accuracy of a linear displacement measurement value.

Description

Three optical axis compensations and gas bath type linear displacement laser interferometer calibration method and device
Technical field
The invention belongs to laser measuring technique field, relate generally to a kind of laser interferometer calibration method and device.
Background technology
Laser interferometry displacement of the lines technology is the standard assay techniques that precision is very high, be widely used in the fields such as accurate and ultraprecise machining, microelectronics equipment, nanometer technology industrial equipment and defence equipment, in order to ensure the accuracy of laser interferometer measurement displacement of the lines, need scientific and effective linear displacement laser interferometer calibration method and device.The general thinking of lubber-line displacement laser interferometer adopts the higher linear displacement laser interferometer of accuracy class to calibrate, and when both precision are close, is namely called comparison.In actual alignment work, linear displacement laser interferometer has suitable precision mostly, is thus realized by comparison the calibration of linear displacement laser interferometer.At present, the general calibration steps of linear displacement laser interferometer has parallel type, face-to-face formula and common light path type (Liao Chengqing, Zhu little Ping, Wang Weichen, Du Hua. the research of laser interferometer length measurement precision calibration steps. modern surveying and laboratory room managing, 2005,1:6-7).
Fig. 1 is parallel type laser interferometer calibrating installation structural representation, canonical measure mirror and be calibrated and measure mirror and be arranged on same movable platform, and when sports platform moves, the light paths of two cover laser interferometer measurement light beams increase and reduction simultaneously.Place because two cover laser interferometer are parallel, two-way light is affected by environment similar, and air refraction is less to two-way influence of light, but due to the vertical range between two-way light comparatively large, therefore during two cover laser interferometer calibrations, Abbe error is larger.
Fig. 2 is face-to-face formula laser interferometer calibrating installation structural representation, canonical measure mirror and being calibrated measures that mirror is aspectant is arranged on sports platform, its advantage is that two cover laser interferometer measurement beam axis can tune to almost on same measurement axis, both Abbe errors are very little, shortcoming is because the near-end of an interferometer is another far-end, not etc., the interference by environment is not different, and the light path impact of air refraction on two cover laser interferometer is inconsistent for both light paths.
2011, China National Measuring Science Research Inst. sets up domestic first 80 meters of large length laser interfering meter measuring device (Leng Yu states, Tao Lei, Xu Jian. based on two-frequency laser interferometer system accuracy and the analysis of Influential Factors of 80m measurement mechanism. metering and measuring technology, 2011, 38 (9): 47-49), accepted standard device puts parallel for the long distance two-frequency laser interferometer of three Agilent5530 types, become three path laser interferometers, the laser interferometer be calibrated is placed in the middle of them, thus carry out calibration calibration, this scheme belongs to the derivative schemes of parallel type calibration steps, and measure owing to adopting three road light simultaneously, therefore can compensating measure time Abbe error, but put owing to being that three laser instruments are parallel, therefore three road sign locating tab assembly light locus are far away, the measurement electrical distance every road sign locating tab assembly electrical distance being calibrated laser interferometer is also far away, all optical paths are different by the impact of environment, air refraction is inconsistent on all optical path impacts, cause calibration measurement result inaccurate.
Fig. 3 is common light path type laser interferometer calibrating installation structural representation, and light path type becomes 90 degree turn back modes unlike two laser instruments with receiver with parallel type laser interferometer calibrating installation altogether, and two cover laser interferometer share interference mirror group and measure mirror.Because two cover laser interferometer share an interference mirror group and measure mirror, cannot determine that the interference mirror group shared belongs to standard laser interferometer component with measurement mirror or belongs to and be calibrated standard laser interferometer component, therefore, not that on denotation, two calibrations of overlapping laser interferometer are calibrated.
1985, Dr-Ing H.-H.Schussler makes full use of space distribution (Dr-Ing H.-H.Schussler.Comparison and calibration of laser interferometer systems.Measurement, 1985,3 (4): 175-184), multipair linear displacement laser interferometer is carried out common light path calibration.Owing to just increasing the quantity of light path laser interferometer altogether, institute also has the shortcoming of common light path type laser interferometer calibrating installation above-mentioned in this approach.
Summary of the invention
For Abbe error larger in above-mentioned existing linear displacement laser interferometer calibrating installation, serious air refraction inconsistency be not that on denotation, two cover laser interferometer carry out the problem of calibrating, the present invention proposes and have developed three optical axis compensations and gas bath type linear displacement laser interferometer calibration method and device, this invention makes canonical measure light beam and is calibrated laser interferometer measurement beam orthogonal apart from very little, thus the impact of Abbe error, reduction air refraction inconsistency can be reduced, and be that on denotation, two cover laser interferometer are calibrated.
Object of the present invention is achieved through the following technical solutions:
A kind of three optical axis compensations and gas bath type linear displacement laser interferometer calibration method, the method step is as follows:
(1) the output light of standard laser interferometer laser instrument forms through three axle hollow laser interference mirror groups three the canonical measure light beams be parallel to each other, article three, canonical measure light beam incides on the level crossing of interstitial hole with regular triangular prism incline distribution form, after being reflected back toward three axle hollow laser interference mirror groups with the part light of level crossing displacement information in every bar canonical measure light beam, according to three interference signals corresponding respectively with three canonical measure light beams obtained from three axle hollow laser interference mirror groups, three shift values that the level crossing that can obtain interstitial hole moves along canonical measure beam direction, the remainder light of every bar canonical measure light beam is transmitted on three light-beam position detectors through there being the level crossing of interstitial hole,
(2) the output light being calibrated laser interferometer laser instrument is calibrated laser interferometer measurement light beam through being calibrated the formation of laser interferometer interference mirror group, be calibrated the intermediate throughholes of laser interferometer measurement light beam through three axle hollow laser interference mirror groups, parallel with three canonical measure light beams, and it is equal with the distance of every bar canonical measure light beam, be calibrated laser interferometer measurement light beam to incide and be calibrated on laser interferometer catoptron, after being reflected back toward and being calibrated laser interferometer interference mirror group, according to from being calibrated the interference signal obtained in laser interferometer interference mirror group, can obtain being calibrated the shift value that laser interferometer catoptron moves along canonical measure beam direction,
(3) gas bath device is along blowing uniform speed airflow perpendicular to three canonical measure beam directions, form stable gas bath environment, in the plane perpendicular to three canonical measure light beams, by three canonical measure light beams in the equilateral triangle region that this plane projection point is formed, gas bath environment makes air themperature, humidity and air pressure approaches uniformity distribute, and makes the air refraction mean value of three canonical measure light beams more close to the air refraction value being calibrated laser interferometer measurement light beam;
Article (4) three, canonical measure light beam is respectively (x with the original incident position coordinates being calibrated laser interferometer measurement light beam respective on the target mirror plane of incidence 1, y 1), (x 2, y 2), (x 3, y 3) and (x 4, y 4), on the target mirror plane of incidence, the original incident position coordinates of every bar measuring beam is after the coordinate displacement (x, y) of two-dimensional directional, and the displacement measurement caused because of target mirror reflecting surface shape characteristic is respectively function z 1(x 1+ x, y 1+ y), z 2(x 2+ x, y 2+ y), z 3(x 3+ x, y 3+ y) and z 4(x 4+ x, y 4+ y);
(5) sports platform along in canonical measure beam direction reciprocatory movement with in the derivative displacement perpendicular to random two-dimensional direction in canonical measure beam plane, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer three is measured shift value and is calibrated laser interferometer measurement shift value, is respectively S 1, S 2, S 3and S 4the synchronizing detection of three light-beam position detectors is to the derivative coordinate displacement value of three canonical measure beam and focus two-dimensional directional on the target mirror plane of incidence, ask for three coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every bar measuring beam, the displacement measurement errors that target mirror reflecting surface shape characteristic causes is compensated to and measures in shift value, obtain S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x ', y 2+ y '), S 3-z 3(x 3+ x ', y 3+ y ') and S 4-z 4(x 4+ x ', y 4+ y '), get S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x', y 2+ y ') and S 3-z 3(x 3+ x ', y 3+ y ') mean value and S 4-z 4(x 4+ x ', y 4+ y ') poor, obtain some sampled measurements error amounts.
A kind of three optical axis compensations and gas bath type linear displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument and three be configured in the receiver that can receive on standard laser interferometer interference signal position, three receivers are connected with standard laser interferometer signal disposal system by wire respectively; Standard laser interferometer laser instrument output light path is configured with can allowing of intermediate throughholes and is calibrated the three axle hollow standard laser interference mirror groups that laser interferometer measurement light beam passes; Three axle hollow standard laser interference mirror group side arrangement guide rails, sports platform is fitted on guide rail, sports platform is provided with the level crossing of interstitial hole, install in level crossing interstitial hole and be calibrated laser interferometer catoptron, be calibrated laser interferometer catoptron and form by the level crossing of interstitial hole the target mirror that the coplanar and relative position of the plane of incidence fixes; Three light-beam position detector configuration are having after the level crossing regional transmission of interstitial hole, and lay respectively on three parallel standards measuring beam transmitted light paths; At three parallel standards measuring beam sidepiece configuration gas bath devices; Be calibrated laser interferometer interference mirror group and be calibrated laser interferometer laser instrument in three axle hollow standard laser interference mirror group opposite sides configurations, described in be calibrated laser interferometer interference mirror group and be positioned at and be calibrated on laser interferometer laser instrument output light path; Being calibrated laser interferometer receiver is configured on the position that can receive and be calibrated laser interferometer interference signal, and wire will be calibrated laser interferometer receiver and be calibrated laser interferometer signal disposal system and be connected.
The present invention has following characteristics and good result:
(1) compared with parallel type laser interferometer calibrating installation, owing to being calibrated the intermediate throughholes of laser interferometer measurement light beam by three axle hollow laser interference mirror groups, the vertical range be calibrated between laser interferometer measurement optical axis and parallel standards optical axis is shorter, both light paths are more close, and therefore during two cover laser interferometer calibrations, Abbe error is very little.
(2) compared with face-to-face formula laser interferometer calibrating installation, in the plane perpendicular to three canonical measure light beams, by three canonical measure light beams in the equilateral triangle region that this plane projection point is formed, article three, canonical measure light beam and to be calibrated laser interferometer measurement light beam very little by the degree difference of environmental interference, the air refraction mean value of three canonical measure light beams is close to the air refraction value being calibrated laser interferometer measurement light beam.
(3) light path type laser interferometer calibrating installation is compared together, shares interference mirror group and measures mirror, standard laser interferometer component and to be calibrated standard laser interferometer component ownership clear and definite, is that on denotation, two cover laser interferometer are calibrated.
(4) three light-beam position detectors can measure three canonical measure light beam relative target catoptrons deriving displacement perpendicular to random two-dimensional direction in canonical measure beam plane, after the derivative displacement of generation, the measurement displacement error that target mirror mirror surface pattern causes compensates in linear movement measuring result, ensures the accuracy of linear movement measuring value.
(5) perpendicular to three canonical measure beam planes and by three canonical measure light beams in the equilateral triangle region that its plane projection surrounds, the stable gas bath environment that the gas bath device configured by three parallel standards measuring beam sidepieces is formed makes air themperature, humidity and air pressure approaches uniformity distribute, and makes the air refraction mean value of three canonical measure light beams more close to the air refraction value being calibrated laser interferometer measurement light beam.
Accompanying drawing explanation
Fig. 1 is parallel type laser interferometer calibrating installation structural representation
Fig. 2 is face-to-face formula laser interferometer calibrating installation structural representation
Fig. 3 is for being total to light path type laser interferometer calibrating installation structural representation
Fig. 4 is three optical axis compensations and gas bath type linear displacement laser interferometer calibrating installation structural representation
Fig. 5 is by the level crossing of interstitial hole and hot spot position distribution schematic diagram on the plane of incidence being calibrated the target mirror that laser interferometer catoptron forms
In figure: 1 standard laser interferometer laser instrument, 2 three axle hollow standard laser interference mirror groups, 3, 4, article 5 three, parallel standards measuring beam, 6 level crossings having an interstitial hole, 7, 8, 9 standard laser interferometer receivers, 10 standard signal disposal systems, 11 are calibrated laser interferometer laser instrument, 12 are calibrated laser interferometer interference mirror group, 13 are calibrated laser interferometer measurement light beam, 14 intermediate throughholes, 15 are calibrated laser interferometer catoptron, 16 are calibrated laser interferometer receiver, 17 are calibrated laser interferometer signal disposal system, 18 sports platforms, 19 guide rails, 20 gas bath devices, 21, 22, 23 3 light-beam position detectors, 24, 25, article 26 3, parallel standards measuring beam facula position, 27 are calibrated laser interferometer beam and focus position.
Embodiment
Below in conjunction with accompanying drawing, the specific embodiment of the invention is described in further detail.
A kind of three optical axis compensations and gas bath type linear displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument 1 and three receivers 7,8,9 be configured on the interference signal position that can receive three parallel standards measuring beams 3,4,5 correspondence respectively, three receivers 7,8,9 are connected with standard laser interferometer signal disposal system 10 by wire respectively; Standard laser interferometer laser instrument 1 output light path is configured with can allowing of intermediate throughholes 14 and is calibrated the three axle hollow standard laser interference mirror groups 2 that laser interferometer measurement light beam 13 passes; Three axle hollow standard laser interference mirror group 2 side arrangement guide rails 19, sports platform 18 is equipped on rails 19, sports platform 18 is provided with the level crossing 6 of interstitial hole, install in level crossing 6 interstitial hole and be calibrated laser interferometer catoptron 15, be calibrated laser interferometer catoptron 15 and form the fixing target mirror of the coplanar and relative position of the plane of incidence by the level crossing 6 of interstitial hole; Three light-beam position detectors 21,22,23 are configured in after level crossing 6 regional transmission of interstitial hole, and lay respectively on three parallel standards measuring beams 3,4,5 transmitted light path; At three parallel standards measuring beam sidepiece configuration gas bath devices; Be calibrated laser interferometer interference mirror group 12 in three axle hollow standard laser interference mirror group 2 opposite sides configurations and be calibrated laser interferometer laser instrument 11, described in be calibrated laser interferometer interference mirror group 12 and be positioned at and be calibrated on laser interferometer laser instrument 11 output light path; Being calibrated laser interferometer receiver 16 is configured on the position that can receive and be calibrated laser interferometer interference signal, and wire will be calibrated laser interferometer receiver 16 and be calibrated laser interferometer signal disposal system 17 and be connected.
Described three parallel standards measuring beams 3,4,5 are with to be calibrated laser interferometer measurement light beam 13 all vertical with the target mirror plane of incidence.
The intermediate throughholes 14 of three described axle hollow standard laser interference mirror groups 2 comprises arbitrary shape, and number is one or more.
Described every bar parallel standards measuring beam 3,4,5 and be calibrated laser interferometer measurement light beam 13 had the level crossing 6 of interstitial hole respectively and be calibrated laser interferometer catoptron 15 reflect once or once more than.
The described laser interferometer catoptron 15 that is calibrated comprises level crossing, prism of corner cube, right-angle prism.
A kind of three optical axis compensations and gas bath type linear displacement laser interferometer calibration method, the method step is as follows:
(1) the output light of standard laser interferometer laser instrument 1 forms through three axle hollow laser interference mirror groups 2 three the canonical measure light beams 3 be parallel to each other, 4, 5, article three, canonical measure light beam 3, 4, 5 incide on the level crossing 6 of interstitial hole with regular triangular prism incline distribution form, after being reflected back toward three axle hollow laser interference mirror groups 2 with the part light of level crossing 6 displacement information in every bar canonical measure light beam, according to obtain from three axle hollow laser interference mirror groups 2 with three canonical measure light beams 3, 4, 5 three corresponding respectively interference signals, the level crossing 6 of interstitial hole can be obtained along canonical measure light beam 3, 4, three shift values of 5 direction motions, every bar canonical measure light beam 3, 4, the remainder light of 5 is transmitted to three light-beam position detectors 21 through there being the level crossing 6 of interstitial hole, 22, on 23,
(2) the output light being calibrated laser interferometer laser instrument 11 is calibrated laser interferometer measurement light beam 13 through being calibrated the formation of laser interferometer interference mirror group 12, be calibrated the intermediate throughholes 14 of laser interferometer measurement light beam 13 through three axle hollow laser interference mirror groups 2, with three canonical measure light beams 3, 4, 5 is parallel, and it is equal with the distance of every bar canonical measure light beam, be calibrated laser interferometer measurement light beam 13 to incide and be calibrated on laser interferometer catoptron 15, after being reflected back toward and being calibrated laser interferometer interference mirror group 12, according to from being calibrated the interference signal obtained in laser interferometer interference mirror group 12, can obtain being calibrated laser interferometer catoptron 15 along canonical measure light beam 3, 4, the shift value of 5 direction motions,
(3) gas bath device 20 blows uniform speed airflow along perpendicular to three canonical measure light beams 3,4,5 direction, form stable gas bath environment, in the plane perpendicular to three canonical measure light beams 3,4,5, by three canonical measure light beams 3,4,5 in the equilateral triangle region that this plane projection point is formed, gas bath environment makes air themperature, humidity and air pressure approaches uniformity distribute, and makes the air refraction mean value of three canonical measure light beams 3,4,5 more close to the air refraction value being calibrated laser interferometer measurement light beam 13;
Article (4) three, canonical measure light beam 3,4,5 and the original incident position coordinates that is calibrated laser interferometer measurement light beam 13 respective on the target mirror plane of incidence are respectively (x 1, y 1), (x 2, y 2), (x 3, y 3) and (x 4, y 4), on the target mirror plane of incidence, the original incident position coordinates of every bar measuring beam is after the coordinate displacement (x, y) of two-dimensional directional, and the displacement measurement caused because of target mirror reflecting surface shape characteristic is respectively function z 1(x 1+ x, y 1+ y), z 2(x 2+ x, y 2+ y), z 3(x 3+ x, y 3+ y) and z 4(x 4+ x, y 4+ y);
(5) sports platform 18 along in canonical measure light beam 3,4,5 direction reciprocatory movement with in the derivative displacement perpendicular to random two-dimensional direction in canonical measure light beam 3,4,5 plane, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer three is measured shift value and is calibrated laser interferometer measurement shift value, is respectively S 1, S 2, S 3and S 4the synchronizing detection of three light-beam position detectors 21,22,23 is to the derivative coordinate displacement value of three canonical measure beam and focus two-dimensional directional on the target mirror plane of incidence, ask for three coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every bar measuring beam, the displacement measurement errors that target mirror reflecting surface shape characteristic causes is compensated to and measures in shift value, obtain S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x ', y 2+ y '), S 3-z 3(x 3+ x ', y 3+ y ') and S 4-Z 4(x 4+ x ', y 4+ y '), get S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x ', y 2+ y ') and S 3-z 3(x 3+ x ', y 3+ y ') mean value and S 4-z 4(x 4+ x ', y 4+ y ') poor, obtain some sampled measurements error amounts.
Canonical measure beam and focus position 24, 25, 26 is three parallel standards measuring beams 3 successively respectively, 4, 5 positions inciding the level crossing 6 of interstitial hole, being calibrated laser interferometer beam and focus position 27 is be calibrated the position that laser interferometer measurement light beam 13 incidence is calibrated laser interferometer catoptron 15, can find out that being calibrated laser interferometer beam and focus position 27 is in canonical measure beam and focus position 24 from position distribution, 25, the center point of 26, i.e. three parallel standards measuring beams 3, 4, 5 will be calibrated laser interferometer measurement light beam 13 is clamped in center.

Claims (6)

1. three optical axis compensations and a gas bath type linear displacement laser interferometer calibration method, is characterized in that the method step is as follows:
(1) the output light of standard laser interferometer laser instrument forms through three axle hollow laser interference mirror groups three the canonical measure light beams be parallel to each other, article three, canonical measure light beam incides on the level crossing of interstitial hole with regular triangular prism incline distribution form, after being reflected back toward three axle hollow laser interference mirror groups with the part light of level crossing displacement information in every bar canonical measure light beam, according to three interference signals corresponding respectively with three canonical measure light beams obtained from three axle hollow laser interference mirror groups, three shift values that the level crossing that can obtain interstitial hole moves along canonical measure beam direction, the remainder light of every bar canonical measure light beam is transmitted on three light-beam position detectors through there being the level crossing of interstitial hole,
(2) the output light being calibrated laser interferometer laser instrument is calibrated laser interferometer measurement light beam through being calibrated the formation of laser interferometer interference mirror group, be calibrated the intermediate throughholes of laser interferometer measurement light beam through three axle hollow laser interference mirror groups, parallel with three canonical measure light beams, and it is equal with the distance of every bar canonical measure light beam, be calibrated laser interferometer measurement light beam to incide and be calibrated on laser interferometer catoptron, after being reflected back toward and being calibrated laser interferometer interference mirror group, according to from being calibrated the interference signal obtained in laser interferometer interference mirror group, can obtain being calibrated the shift value that laser interferometer catoptron moves along canonical measure beam direction,
(3) gas bath device is along blowing uniform speed airflow perpendicular to three canonical measure beam directions, form stable gas bath environment, in the plane perpendicular to three canonical measure light beams, by three canonical measure light beams in the equilateral triangle region that this plane projection point is formed, gas bath environment makes air themperature, humidity and air pressure approaches uniformity distribute, and makes the air refraction mean value of three canonical measure light beams more close to the air refraction value being calibrated laser interferometer measurement light beam;
Article (4) three, canonical measure light beam is respectively (x with the original incident position coordinates being calibrated laser interferometer measurement light beam respective on the target mirror plane of incidence 1, y 1), (x 2, y 2), (x 3, y 3) and (x 4, y 4), on the target mirror plane of incidence, the original incident position coordinates of every bar measuring beam is after the coordinate displacement (x, y) of two-dimensional directional, and the displacement measurement caused because of target mirror reflecting surface shape characteristic is respectively function z 1(x 1+ x, y 1+ y), z 2(x 2+ x, y 2+ y), z 3(x 3+ x, y 3+ y) and z 4(x 4+ x, y 4+ y);
(5) sports platform along in canonical measure beam direction reciprocatory movement with in the derivative displacement perpendicular to random two-dimensional direction in canonical measure beam plane, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer three is measured shift value and is calibrated laser interferometer measurement shift value, is respectively S 1, S 2, S 3and S 4the synchronizing detection of three light-beam position detectors is to the derivative coordinate displacement value of three canonical measure beam and focus two-dimensional directional on the target mirror plane of incidence, ask for three coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every bar measuring beam, the displacement measurement errors that target mirror reflecting surface shape characteristic causes is compensated to and measures in shift value, obtain S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x ', y 2+ y '), S 3-z 3(x 3+ x ', y 3+ y ') and S 4-z 4(x 4+ x ', y 4+ y '), get S 1-z 1(x 1+ x ', y 1+ y '), S 2-z 2(x 2+ x ', y 2+ y ') and S 3-z 3(x 3+ x ', y 3+ y ') mean value and S 4-z 4(x 4+ x ', y 4+ y ') poor, obtain some sampled measurements error amounts.
2. an optical axis compensation and gas bath type linear displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument (1) and three be configured in the receiver (7,8,9) that can receive on standard laser interferometer interference signal position, three receivers (7,8,9) are connected with standard laser interferometer signal disposal system (10) by wire respectively; It is characterized in that being configured with can allowing of intermediate throughholes (14) on standard laser interferometer laser instrument (1) output light path and be calibrated three axle hollow standard laser interference mirror group (2) that laser interferometer measurement light beam (13) passes; Three axle hollow standard laser interference mirror group (2) side arrangement guide rail (19), sports platform (18) is fitted on guide rail (19), sports platform (18) is provided with the level crossing (6) of interstitial hole, install in level crossing (6) interstitial hole and be calibrated laser interferometer catoptron (15), be calibrated laser interferometer catoptron (15) and have the level crossing of interstitial hole (6) the composition plane of incidence coplanar and the target mirror that relative position is fixing; Three light-beam position detectors (21,22,23) are configured in after level crossing (6) regional transmission of interstitial hole, and lay respectively on three parallel standards measuring beams (3,4,5) transmitted light path; At three parallel standards measuring beams (3,4,5) sidepiece configuration gas bath device (20); Be calibrated laser interferometer interference mirror group (12) in three axle hollow standard laser interference mirror group (2) opposite sides configurations and be calibrated laser interferometer laser instrument (11), described in be calibrated laser interferometer interference mirror group (12) and be positioned at and be calibrated on laser interferometer laser instrument (11) output light path; Being calibrated laser interferometer receiver (16) is configured on the position that can receive and be calibrated laser interferometer interference signal, and wire will be calibrated laser interferometer receiver (16) and be calibrated laser interferometer signal disposal system (17) and be connected.
3. three optical axis compensations according to claim 2 and gas bath type linear displacement laser interferometer calibrating installation, is characterized in that described three parallel standards measuring beams (3,4,5) and to be calibrated laser interferometer measurement light beam (13) all vertical with the target mirror plane of incidence.
4. three optical axis compensations according to claim 2 and gas bath type linear displacement laser interferometer calibrating installation, it is characterized in that the intermediate throughholes (14) of three described axle hollow standard laser interference mirror group (2) comprises arbitrary shape, number is one or more.
5. three optical axis compensations according to claim 2 and gas bath type linear displacement laser interferometer calibrating installation, is characterized in that described every bar parallel standards measuring beam (3,4,5) and is calibrated laser interferometer measurement light beam (13) had the level crossing of interstitial hole (6) respectively and be calibrated more than laser interferometer catoptron (15) reflection once or once.
6. three optical axis compensations according to claim 2 and gas bath type linear displacement laser interferometer calibrating installation, is characterized in that the described laser interferometer catoptron (15) that is calibrated comprises level crossing, prism of corner cube, right-angle prism.
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* Cited by examiner, † Cited by third party
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CN114877801A (en) * 2022-04-19 2022-08-09 中国测试技术研究院机械研究所 Range extending method and system in indoor large-length standard device magnitude transmission
CN115542300A (en) * 2022-11-24 2022-12-30 中国电子产品可靠性与环境试验研究所((工业和信息化部电子第五研究所)(中国赛宝实验室)) Pose measurement method and system

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE4208189A1 (en) * 1992-03-11 1993-04-08 Gerald Dipl Ing Sparrer Laser interferometer calibration system using direct comparison - using laser interferometer used as standard and arrangement of triple reflectors including displaceable common triple reflector
US7130056B2 (en) * 2004-02-20 2006-10-31 Agilent Technologies, Inc. System and method of using a side-mounted interferometer to acquire position information
CN103267581B (en) * 2013-05-17 2015-08-26 中山大学 Be applicable to the spectrum shearing interferometer measuring shaped pulse

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