CN103528503A - Double-optical axis compensation and air bath type angular displacement laser interferometer calibration method and device - Google Patents

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

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CN103528503A
CN103528503A CN201310475485.5A CN201310475485A CN103528503A CN 103528503 A CN103528503 A CN 103528503A CN 201310475485 A CN201310475485 A CN 201310475485A CN 103528503 A CN103528503 A CN 103528503A
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laser interferometer
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canonical measure
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CN103528503B (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 double-optical axis compensation and air bath type angular displacement laser interferometer calibration method and a double-optical axis compensation and air bath type angular displacement laser interferometer calibration device, and belongs to the technical field of laser measurement. Two measurement light beams of a calibrated laser interferometer penetrate through a middle through hole of a double-axis hollow laser interference mirror group, and are arranged in parallel at the middle positions of two parallel standard measurement light beams; the standard measurement light beams are at short perpendicular distances away from the measurement light beams of the calibrated laser interferometer, and air refractivity values of the standard measurement light beams are approximate to those 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 air refractivity values of the standard measurement light beams are more approximate to those of the measurement light beams of the calibrated laser interferometer; a displacement measurement error caused by the surface appearance of the reflecting surface of a target reflector is compensated into an angular displacement measurement result to ensure the accuracy of an angular displacement measurement value.

Description

Double-optical axis compensation and gas bath type angular displacement laser interferometer calibration steps and device
Technical field
The invention belongs to laser measuring technique field, relate generally to a kind of laser interferometer calibration steps and device.
Background technology
Angular displacement laser interferometer is the canonical measure technology 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, can be for the monitoring of micrometric displacement parts, mobile platform and litho machine angle variable quantity.Angular displacement laser interferometer can provide very high measuring accuracy, and the relative pivot angle in can kinetic measurement campaign, this is the unique advantage of other instruments of difference, in order to guarantee the accuracy of angular displacement laser interferometer measurement, scientificlly and effectively diagonal displacement laser interferometer is calibrated extremely important.The realization of angular displacement laser interferometer is the displacement of the lines laser interferometer on monochromatic light road to be modified into the displacement of the lines laser interferometer of multi-pass, can obtain the changing value of an anglec of rotation by two relative change in optical path length of light path that measure.Calibration steps and the device of angular displacement laser interferometer are not proposed in current documents and materials, but because angular displacement laser interferometer is the derivative schemes of displacement of the lines laser interferometer measurement, so the calibration of angular displacement laser interferometer can adopt the calibration steps of displacement of the lines laser interferometer: parallel type (Leng Yu state, Tao Lei, Xu Jian. two-frequency laser interferometer system accuracy and analysis of Influential Factors based on 80m measurement mechanism. metering and measuring technology, 2011, 38 (9): 47-49), back-to-back formula (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) with common light path formula (Dr-Ing H.-H.Schussler.Comparison and calibration of laser interferometer systems.Measurement, 1985, 3 (4): 175-184), therefore angular displacement laser interferometer calibrating installation also has the shortcoming of displacement of the lines laser interferometer calibrating installation: larger Abbe error, serious air refraction inconsistency and be not in accurate meaning two cover laser interferometer calibrate.
Summary of the invention
For Abbe error larger in above-mentioned existing angular displacement laser interferometer calibrating installation, serious air refraction inconsistency be not the problem that in accurate meaning, two cover laser interferometer are calibrated, the present invention proposes and has researched and developed double-optical axis compensation and gas bath type angular displacement laser interferometer calibration steps and device, this invention makes canonical measure light beam and is calibrated laser interferometer measurement light beam vertical range very little, thereby can reduce Abbe error, reduce the impact of air refraction inconsistency, and be that in accurate meaning, two cover laser interferometer are calibrated.
Object of the present invention is achieved through the following technical solutions:
And a gas bath type angular displacement laser interferometer calibration steps, the method step is as follows:
(1) the output light of standard laser interferometer laser instrument forms two canonical measure light beams that are parallel to each other through twin shaft hollow laser interference mirror group, and all incide on the level crossing of interstitial hole, in the plane perpendicular to two canonical measure light beams, article one, the connecting line segment M length and between second canonical measure light beam projecting location point is A, part light with level crossing displacement information in every canonical measure light beam is reflected back toward after twin shaft hollow laser interference mirror group, according to the interference signal obtaining from twin shaft hollow laser interference mirror group, obtain connecting line segment M place straight line and changing value the arctan ((a that has the level crossing plane of incidence angle of interstitial hole 1-a 2)/A), wherein, a 1and a 2the linear movement measuring value that is respectively article one and second canonical measure beam feeding sputtering area on the level crossing of interstitial hole, the remainder light of every canonical measure light beam is through there being the level crossing of interstitial hole to be transmitted on two light-beam position detectors,
(2) the output light that is calibrated laser interferometer laser instrument forms two of being parallel to each other and is calibrated laser interferometer measurement light beam through being calibrated laser interferometer interference mirror group, be calibrated the intermediate throughholes that two measuring beams of laser interferometer all pass twin shaft hollow laser interference mirror group, parallel with two canonical measure light beams, and all incide and be calibrated on laser interferometer plane mirror, in the plane perpendicular to two canonical measure light beams, article one and second to be calibrated connecting line segment m between laser interferometer measurement light beam projecting location point long be B, connecting line segment m and connecting line segment M conllinear, article two, with the laser interferometer measurement beam reflection that is calibrated that is calibrated laser interferometer plane mirror displacement information, return and be calibrated after laser interferometer interference mirror group, according to the interference signal obtaining from be calibrated laser interferometer interference mirror group, obtain connecting line segment m place straight line and changing value the arctan ((b that is calibrated laser interferometer plane mirror plane of incidence angle 1-b 2)/B), wherein, b 1and b 2be respectively and be calibrated the linear movement measuring value that article one and second on laser interferometer plane mirror are calibrated laser interferometer measurement beam feeding sputtering area,
(3) gas bath device is along blowing uniform speed airflow perpendicular to two canonical measure beam directions, form stable gas bath environment, in the plane perpendicular to two canonical measure light beams, in the line segment region being formed at this plane projection point by two canonical measure light beams, gas bath environment is uniformly distributed air themperature, humidity and air pressure, makes canonical measure light beam and be calibrated laser interferometer measurement light beam air refraction value more approaching;
(4) article one, second canonical measure light beam and article one, second are calibrated laser interferometer measurement light beam initial incoming position coordinate separately on the target mirror plane of incidence and 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, after the initial incoming position coordinate process coordinate displacement (x, y) of every measuring beam, the linear movement measuring value causing 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), sports platform carries out the low-angle beat of any sense of rotation and with the derivative displacement of random two-dimensional direction in the plane perpendicular to canonical measure light beam, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer variable angle value arctan ((a 1-a 2)/A) and be calibrated laser interferometer variable angle value arctan ((b 1-b 2)/B), the derivative coordinate displacement value of two light-beam position detectors synchronizing detection to two canonical measure beam and focus two-dimensional directional on the target mirror plane of incidence, ask for two coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every measuring beam, the linear movement measuring error compensation that target mirror reflecting surface shape characteristic is caused, in variable angle value, obtains arctan{[(a 1-z 1(x 1+ x ', y 1+ y '))-(a 2-z 2(x 2+ x ', y 2+ y '))]/A} and arctan{[(b 1-z 3(x 3+ x ', y 3+ y '))-(b 2-z 4(x 4+ x ', y 4+ y '))]/B}, finally obtains a series of angular displacement calibration measurement error amount arctan{[(a 1-z 1(x 1+ x ', y 1+ y '))-(a 2-z 2(x 2+ x ', y 2+ y '))]/A}-arctan{[(b 1-z 3(x 3+ x ', y 3+ y '))-(b 2-z 4(x 4+ x ', y 4+ y '))]/B}.
A kind of double-optical axis compensation and gas bath type angular displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument, can receive the locational receiver of standard laser interferometer interference signal, wire is connected receiver with standard laser interferometer signal disposal system; On standard laser interferometer laser instrument output light path, dispose can allowing of intermediate throughholes and be calibrated the twin shaft hollow standard laser interference mirror group that laser interferometer measurement light beam passes; Twin shaft hollow standard laser interference mirror group one side arrangement guide rail, sports platform is fitted on guide rail, the level crossing of interstitial hole is installed on sports platform, in level crossing interstitial hole, install and be calibrated laser interferometer plane mirror, be calibrated laser interferometer plane mirror and form by the level crossing of interstitial hole the target mirror that the plane of incidence is coplanar and relative position is fixing; Two light-beam position detector configuration are having after the level crossing regional transmission of interstitial hole, and lay respectively on two parallel standards measuring beam transmitted light paths; At two parallel standards measuring beam sidepiece configuration gas bath devices; In twin shaft hollow standard laser interference mirror group opposite side configuration, be calibrated laser interferometer interference mirror group and be calibrated laser interferometer laser instrument, described in be calibrated laser interferometer interference mirror group and be positioned at and be calibrated on laser interferometer laser instrument output light path; Be calibrated laser interferometer receiver and be configured in and can receive on the position that is calibrated laser interferometer interference signal, 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) owing to being calibrated laser interferometer measurement light beam by the intermediate throughholes of twin shaft hollow laser interference mirror group, be calibrated the vertical range of measuring between optical axis and parallel standards optical axis very short, both light paths are very approaching, and when therefore two cover laser interferometer are calibrated, Abbe error is very little.
(2) in the plane perpendicular to two canonical measure light beams, in the line segment region being formed at this plane projection point by two canonical measure light beams, article two, canonical measure light beam and two are calibrated laser interferometer measurement light beam and are subject to the degree difference of environmental interference very little, and canonical measure light beam is with to be calibrated laser interferometer measurement light beam air refraction value very approaching.
(3) there is no shared interference mirror group and measure mirror, standard laser interferometer component and to be calibrated standard laser interferometer component ownership clear and definite, is that the cover of two in accurate meaning laser interferometer is calibrated.
(4) two light-beam position detectors can be measured the derivative displacement of two relative target mirrors of canonical measure light beam random two-dimensional direction in perpendicular to canonical measure beam plane, after there is derivative displacement, the measurement displacement error that target mirror reflecting surface surface topography causes compensates in angle displacement measurement result, guarantees the accuracy of angle displacement measurement value.
(5) gas bath device is along blowing uniform speed airflow perpendicular to two canonical measure beam directions, form stable gas bath environment, in the plane perpendicular to two canonical measure light beams, in the line segment region being formed at this plane projection point by two canonical measure light beams, gas bath environment is uniformly distributed air themperature, humidity and air pressure, makes canonical measure light beam and be calibrated laser interferometer measurement light beam air refraction value more approaching.
Accompanying drawing explanation
Fig. 1 is double-optical axis compensation and gas bath type angular displacement laser interferometer calibrating installation structural representation
Fig. 2 for the level crossing by interstitial hole be calibrated hot spot position distribution schematic diagram on the plane of incidence of the target mirror that laser interferometer plane mirror forms
In figure: 1 standard laser interferometer laser instrument, 2 twin shaft hollow standard laser interference mirror groups, 3, article 4 two, parallel standards measuring beam, 5 have the level crossing of interstitial hole, 6 standard laser interferometer receivers, 7 standard signal disposal systems, 8 are calibrated laser interferometer laser instrument, 9 are calibrated laser interferometer interference mirror group, 10, article 11 two, be calibrated laser interferometer measurement light beam, 12 intermediate throughholes, 13 are calibrated laser interferometer plane mirror, 14 are calibrated laser interferometer receiver, 15 are calibrated laser interferometer signal disposal system, 16 sports platforms, 17 guide rails, 18 gas bath devices, 19, 20 two light-beam position detectors, 21, article 22 two, parallel standards measuring beam facula position, 23, article 24 two, be 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 double-optical axis compensation and gas bath type angular displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument 1, can receive the locational receiver 6 of standard laser interferometer interference signal, wire is connected receiver 6 with standard laser interferometer signal disposal system 7; On standard laser interferometer laser instrument 1 output light path, dispose can allowing of intermediate throughholes 12 and be calibrated the twin shaft hollow standard laser interference mirror group 2 that laser interferometer measurement light beam 10,11 passes; Twin shaft hollow standard laser interference mirror group 2 one side arrangement guide rails 17, sports platform 16 is fitted on guide rail 17, the level crossing 5 of interstitial hole is installed on sports platform 16, in level crossing 5 interstitial holes, install and be calibrated laser interferometer plane mirror 13, be calibrated laser interferometer plane mirror 13 and form by the level crossing 5 of interstitial hole the target mirror that the plane of incidence is coplanar and relative position is fixing; Two light- beam position detectors 19,20 are configured in after level crossing 5 regional transmissions of interstitial hole, and lay respectively on two parallel standards measuring beams, 3,4 transmitted light paths; At two parallel standards measuring beams, 3,4 sidepiece configuration gas bath devices 18; In the 2 opposite sides configurations of twin shaft hollow standard laser interference mirror group, be calibrated laser interferometer interference mirror group 9 and be calibrated laser interferometer laser instrument 8, described in be calibrated laser interferometer interference mirror group 9 and be positioned at and be calibrated on laser interferometer laser instrument 8 output light paths; Be calibrated laser interferometer receiver 14 and be configured in and can receive on the position that is calibrated laser interferometer interference signal, wire will be calibrated laser interferometer receiver 14 and be calibrated laser interferometer signal disposal system 15 and be connected.
The intermediate throughholes 12 of described twin shaft hollow standard laser interference mirror group 2 comprises arbitrary shape, and number is one or more.
Described every parallel standards measuring beam 3,4 and every are calibrated laser interferometer measurement light beam 10,11 to be had respectively the level crossing 5 of interstitial hole and is calibrated 13 reflections of laser interferometer plane mirror once or once.
Described standard laser interferometer receiver 6 is respectively one or more with the number that is calibrated laser interferometer receiver 14.
And a gas bath type angular displacement laser interferometer calibration steps, the method step is as follows:
(1) the output light of standard laser interferometer laser instrument 1 forms through twin shaft hollow laser interference mirror group 2 two canonical measure light beams 3 that are parallel to each other, 4, and all incide on the level crossing 5 of interstitial hole, perpendicular to two canonical measure light beams 3, in 4 plane, article one, the connecting line segment M length and between second canonical measure light beam projecting location point is A, part light with level crossing 5 displacement informations in every canonical measure light beam is reflected back toward after twin shaft hollow laser interference mirror group 2, according to the interference signal obtaining from twin shaft hollow laser interference mirror group 2, obtain connecting line segment M place straight line and changing value the arctan ((a that has level crossing 5 plane of incidence angles of interstitial hole 1-a 2)/A), wherein, a 1and a 2the linear movement measuring value that is respectively article one and second canonical measure beam feeding sputtering area on the level crossing 5 of interstitial hole, the remainder light of every canonical measure light beam 3,4 is through there being the level crossing 5 of interstitial hole to be transmitted on two light- beam position detectors 19,20,
(2) the output light that is calibrated laser interferometer laser instrument 8 forms two of being parallel to each other and is calibrated laser interferometer measurement light beam 10 through being calibrated laser interferometer interference mirror group 9, 11, be calibrated two measuring beams 10 of laser interferometer, 11 all pass the intermediate throughholes 12 of twin shaft hollow laser interference mirror group 2, with two canonical measure light beams 3, 4 is parallel, and all incide and be calibrated on laser interferometer plane mirror 13, perpendicular to two canonical measure light beams 3, in 4 plane, article one and second to be calibrated connecting line segment m between laser interferometer measurement light beam projecting location point long be B, connecting line segment m and connecting line segment M conllinear, article two, with what be calibrated laser interferometer plane mirror 13 displacement informations, be calibrated laser interferometer measurement light beam 10, 11 are reflected back and are calibrated after laser interferometer interference mirror group 9, according to the interference signal obtaining from be calibrated laser interferometer interference mirror group 9, obtain connecting line segment m place straight line and changing value the arctan ((b that is calibrated laser interferometer plane mirror 13 plane of incidence angles 1-b 2)/B), wherein, b 1and b 2be respectively and be calibrated the linear movement measuring value that article one and second on laser interferometer plane mirror 13 are calibrated laser interferometer measurement beam feeding sputtering area,
(3) gas bath device 18 is along blowing uniform speed airflow perpendicular to two canonical measure light beams, 3,4 directions, form stable gas bath environment, in the plane perpendicular to two canonical measure light beams 3,4, in the line segment region being formed at this plane projection point by two canonical measure light beams 3,4, gas bath environment is uniformly distributed air themperature, humidity and air pressure, makes canonical measure light beam and be calibrated laser interferometer measurement light beam air refraction value more approaching;
(4) article one, second canonical measure light beam and article one, second are calibrated laser interferometer measurement light beam initial incoming position coordinate separately on the target mirror plane of incidence and 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, after the initial incoming position coordinate process coordinate displacement (x, y) of every measuring beam, the linear movement measuring value causing 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), sports platform 16 carries out the low-angle beat of any sense of rotation and with the derivative displacement of random two-dimensional direction in the plane perpendicular to canonical measure light beam 3,4, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer variable angle value arctan ((a 1-a 2)/A) and be calibrated laser interferometer variable angle value arctan ((b 1-b 2)/B), the derivative coordinate displacement value of two light- beam position detector 19,20 synchronizing detections to a two canonical measure light beam 3,4 hot spots two-dimensional directional on the target mirror plane of incidence, ask for two coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every measuring beam, the linear movement measuring error compensation that target mirror reflecting surface shape characteristic is caused, in variable angle value, obtains arctan{[(a 1-z 1(x 1+ x', y 1+ y '))-(a 2-z 2(x 2+ x', y 2+ y '))]/A} and arctan{[(b 1-z 3(x 3+ x ', y 3+ y '))-(b 2-z 4(x 4+ x ', y 4+ y '))]/B}, finally obtains a series of angular displacement calibration measurement error amount arctan{[(a 1-z 1(x 1+ x ', y 1+ y '))-(a 2-z 2(x 2+ x ', y 2+ y '))]/A}-arctan{[(b 1-z 3(x 3+ x ', y 3+ y '))-(b 2-z 4(x 4+ x ', y 4+ y '))]/B}.
Canonical measure beam and focus position 21, 22 is respectively two parallel standards measuring beams 3 successively, 4 incide the position of the level crossing 5 of interstitial hole, be calibrated laser interferometer beam and focus position 23, the 24th, be calibrated laser interferometer measurement light beam 10, 11 incidents are calibrated the position of laser interferometer plane mirror 13, from position distribution, can find out and be calibrated laser interferometer beam and focus position 23, 24 are in canonical measure beam and focus position 21, 22 centre, i.e. two parallel standards measuring beams 3, 4 will be calibrated laser interferometer measurement light beam 10, 11 are clamped in centre position.

Claims (5)

1. double-optical axis compensation and a gas bath type angular displacement laser interferometer calibration steps, is characterized in that the method step is as follows:
(1) the output light of standard laser interferometer laser instrument forms two canonical measure light beams that are parallel to each other through twin shaft hollow laser interference mirror group, and all incide on the level crossing of interstitial hole, in the plane perpendicular to two canonical measure light beams, article one, the connecting line segment M length and between second canonical measure light beam projecting location point is A, part light with level crossing displacement information in every canonical measure light beam is reflected back toward after twin shaft hollow laser interference mirror group, according to the interference signal obtaining from twin shaft hollow laser interference mirror group, obtain connecting line segment M place straight line and changing value the arctan ((a that has the level crossing plane of incidence angle of interstitial hole 1-a 2)/A), wherein, a 1and a 2the linear movement measuring value that is respectively article one and second canonical measure beam feeding sputtering area on the level crossing of interstitial hole, the remainder light of every canonical measure light beam is through there being the level crossing of interstitial hole to be transmitted on two light-beam position detectors,
(2) the output light that is calibrated laser interferometer laser instrument forms two of being parallel to each other and is calibrated laser interferometer measurement light beam through being calibrated laser interferometer interference mirror group, be calibrated the intermediate throughholes that two measuring beams of laser interferometer all pass twin shaft hollow laser interference mirror group, parallel with two canonical measure light beams, and all incide and be calibrated on laser interferometer plane mirror, in the plane perpendicular to two canonical measure light beams, article one and second to be calibrated connecting line segment m between laser interferometer measurement light beam projecting location point long be B, connecting line segment m and connecting line segment M conllinear, article two, with the laser interferometer measurement beam reflection that is calibrated that is calibrated laser interferometer plane mirror displacement information, return and be calibrated after laser interferometer interference mirror group, according to the interference signal obtaining from be calibrated laser interferometer interference mirror group, obtain connecting line segment m place straight line and changing value the arctan ((b that is calibrated laser interferometer plane mirror plane of incidence angle 1-b 2)/B), wherein, b 1and b 2be respectively and be calibrated the linear movement measuring value that article one and second on laser interferometer plane mirror are calibrated laser interferometer measurement beam feeding sputtering area,
(3) gas bath device is along blowing uniform speed airflow perpendicular to two canonical measure beam directions, form stable gas bath environment, in the plane perpendicular to two canonical measure light beams, in the line segment region being formed at this plane projection point by two canonical measure light beams, gas bath environment is uniformly distributed air themperature, humidity and air pressure, makes canonical measure light beam and be calibrated laser interferometer measurement light beam air refraction value more approaching;
(4) article one, second canonical measure light beam and article one, second are calibrated laser interferometer measurement light beam initial incoming position coordinate separately on the target mirror plane of incidence and 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, after the initial incoming position coordinate process coordinate displacement (x, y) of every measuring beam, the linear movement measuring value causing because of target mirror reflecting surface shape characteristic is respectively function z1 (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), sports platform carries out the low-angle beat of any sense of rotation and with the derivative displacement of random two-dimensional direction in the plane perpendicular to canonical measure light beam, with at the uniform velocity or non-at the uniform velocity sampling rate, synchronized sampling standard laser interferometer variable angle value arctan ((a 1-a 2)/A) and be calibrated laser interferometer variable angle value arctan ((b 1-b 2)/B), the derivative coordinate displacement value of two light-beam position detectors synchronizing detection to two canonical measure beam and focus two-dimensional directional on the target mirror plane of incidence, ask for two coordinate displacement values arithmetic mean (x ', y ') as the derivative coordinate displacement value of every measuring beam, the linear movement measuring error compensation that target mirror reflecting surface shape characteristic is caused, in variable angle value, obtains arctan{[(a 1-z 1(x 1+ x ', y 1+ y '))-(a 2-z 2(x 2+ x ', y 2+ y '))]/A} and arctan{[(b 1-z 3(x 3+ x', y 3+ y'))-(b 2-z 4(x 4+ x', y 4+ y'))]/B}, finally obtains a series of angular displacement calibration measurement error amount arctan{[(a 1-z 1(x 1+ x', y 1+ y '))-(a 2-z 2(x 2+ x', y 2+ y '))]/A}-arctan{[(b 1-z 3(x 3+ x ', y 3+ y '))-(b 2-z 4(x 4+ x', y 4+ y '))]/B}.
2. a double-optical axis compensation and gas bath type angular displacement laser interferometer calibrating installation, comprise standard laser interferometer laser instrument (1), can receive the locational receiver of standard laser interferometer interference signal (6), wire is connected receiver (6) with standard laser interferometer signal disposal system (7); It is characterized in that disposing can allowing of intermediate throughholes (12) and be calibrated the twin shaft hollow standard laser interference mirror group (2) that laser interferometer measurement light beam (10,11) passes on standard laser interferometer laser instrument (1) output light path; Twin shaft hollow standard laser interference mirror group (2) one side arrangement guide rails (17), sports platform (16) is fitted on guide rail (17), the level crossing (5) of interstitial hole is installed on sports platform (16), in level crossing (5) interstitial hole, install and be calibrated laser interferometer plane mirror (13), be calibrated laser interferometer plane mirror (13) and have the level crossing (5) of interstitial hole to form the target mirror that the plane of incidence is coplanar and relative position is fixing; Two light-beam position detectors (19,20) are configured in after level crossing (5) regional transmission of interstitial hole, and lay respectively on two parallel standards measuring beams (3,4) transmitted light path; At two parallel standards measuring beams (3,4) sidepiece configuration gas bath device (18); In twin shaft hollow standard laser interference mirror group (2) opposite side configuration, be calibrated laser interferometer interference mirror group (9) and be calibrated laser interferometer laser instrument (8), described in be calibrated laser interferometer interference mirror group (9) and be positioned at and be calibrated on laser interferometer laser instrument (8) output light path; Be calibrated laser interferometer receiver (14) and be configured in and can receive on the position that is calibrated laser interferometer interference signal, wire will be calibrated laser interferometer receiver (14) and be calibrated laser interferometer signal disposal system (15) and be connected.
3. double-optical axis compensation according to claim 2 and gas bath type angular displacement laser interferometer calibrating installation, the intermediate throughholes (12) that it is characterized in that described twin shaft hollow standard laser interference mirror group (2) comprises that arbitrary shape, number are one or more.
4. double-optical axis compensation according to claim 2 and gas bath type angular displacement laser interferometer calibrating installation, is characterized in that described every parallel standards measuring beam (3,4) and every are calibrated laser interferometer measurement light beam (10,11) and are had respectively the level crossing (5) of interstitial hole and be calibrated that laser interferometer plane mirror (13) reflects once or once.
5. double-optical axis compensation according to claim 2 and gas bath type angular displacement laser interferometer calibrating installation, the number that it is characterized in that described standard laser interferometer receiver (6) and be calibrated laser interferometer receiver (14) is respectively one or more.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115327560A (en) * 2022-08-11 2022-11-11 天津市特种设备监督检验技术研究院(天津市特种设备事故应急调查处理中心) Device and method for detecting natural glide quantity of fork of forklift based on laser reflection

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1657865A (en) * 2004-02-20 2005-08-24 安捷伦科技有限公司 System and method of using a side-mounted interferometer to acquire position information
CN103267581A (en) * 2013-05-17 2013-08-28 中山大学 Spectrum shearing interferometer suitable for measuring shaped pulses

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1657865A (en) * 2004-02-20 2005-08-24 安捷伦科技有限公司 System and method of using a side-mounted interferometer to acquire position information
CN103267581A (en) * 2013-05-17 2013-08-28 中山大学 Spectrum shearing interferometer suitable for measuring shaped pulses

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
冷玉国等: "基于80m测量装置的双频激光干涉仪系统精度及影响因素分析", 《计量与测试技术》 *
廖澄清等: "激光干涉仪测长精度校准方法的研究", 《现代测量与实验室管理》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115327560A (en) * 2022-08-11 2022-11-11 天津市特种设备监督检验技术研究院(天津市特种设备事故应急调查处理中心) Device and method for detecting natural glide quantity of fork of forklift based on laser reflection
CN115327560B (en) * 2022-08-11 2024-05-07 天津市特种设备监督检验技术研究院(天津市特种设备事故应急调查处理中心) Device and method for detecting natural slipping quantity of forklift fork based on laser reflection

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