CN204514568U - A kind of sagnac interferometer two-arm angular error measuring system - Google Patents
A kind of sagnac interferometer two-arm angular error measuring system Download PDFInfo
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- CN204514568U CN204514568U CN201420820436.0U CN201420820436U CN204514568U CN 204514568 U CN204514568 U CN 204514568U CN 201420820436 U CN201420820436 U CN 201420820436U CN 204514568 U CN204514568 U CN 204514568U
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- transit
- sagnac interferometer
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- light pipe
- arm
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Abstract
The utility model belongs to optical testing art, is specifically related to a kind of sagnac interferometer two-arm angular error measuring system.This system comprises the first transit, the second transit, rotation platform and Auto-collimation angular measurement light pipe; Concrete measuring method is: the primary importance 1) obtaining target beam; 2) second place of target beam is obtained; 3) according to the primary importance of target beam on Auto-collimation angular measurement light pipe and the distance calculating sagnac interferometer two-arm angular error of the second place; By the measuring accuracy using system and method for the present utility model to substantially increase sagnac interferometer two-arm angular error, and system architecture is simple.
Description
Technical field
The utility model belongs to optical testing art, is specifically related to a kind of sagnac interferometer two-arm angular error measuring system.
Background technology
Because two-arm angular error directly affects Sagnac (hereinafter referred to as Sagnac) interferometer interference fringe spacing, thus affect the spectral resolution of interference spectroscope.The error that takes measurement of an angle can be debug in process at interferometer and control alignment error, also can be revised this error in the end spectroscopic data process.
The angle required between current employing Sagnac interferometer two-arm angle is 45 °, but owing to adding the error in man-hour, the angle value of 45 ° is difficult to ensure in process, therefore can affect the use of interferometer;
The system of existing measurement Sagnac interferometer two-arm angular error is:
Use two transits mutually to aim in 90 ° of settings, wherein the first transit is for launching target beam, and the second transit is used for receiving target light beam; When measuring, the outgoing target beam of the first transit is received by the second transit after Sagnac interferometer reflection, now, if the angle value that the second transit reads is 0 °, then proves that Sagnac interferometer two-arm angle error value is 0; If the angle value that the second transit reads is δ °, because the angle between the emergent light of the first transit and the incident light of the second transit is the twice of Sagnac interferometer two-arm angle, then the error amount of Sagnac interferometer two-arm angle is δ/2 °.
But said method introduces when two transits aimings set up 90 ° and there will be error, and two transits aimings can be set up 90 ° of errors produced when spending during measurement and bring in final measurement, the precision of measurement is not high.
Utility model content
In order to solve the problem in background technology, the utility model provides that a kind of measuring accuracy is high, structure is simple, be easy to the Sagnac interferometer two-arm angular error measuring system that realizes.
Concrete technical scheme of the present utility model is:
A kind of Sagnac interferometer two-arm angular error measuring system, is characterized in that: comprise the first transit, the second transit, rotation platform and Auto-collimation angular measurement light pipe;
The target beam that described first transit sends is incident in the image planes of Sagnac interferometer outgoing to the second transit after the reflection of Sagnac interferometer two-arm;
Described Auto-collimation angular measurement light pipe is arranged towards the second transit, makes the target beam entering the second transit can be imaged in the image planes of Auto-collimation angular measurement light pipe;
The axis of rotation of described rotation platform is arranged on the intersection point of the first transit optical axis and Sagnac interferometer light splitting surface.
Auto-collimation angular measurement light pipe in above-mentioned measuring system is replaced by transit.
The utility model has the advantage of:
1, the utility model obtains the position of target beam by twice, Sagnac interferometer two-arm angular error is determined by the difference of twice position, effectively prevent prior art two transits and place the error occurred when aiming at, and two-arm angle error value is exaggerated 4 times, improves the precision of measurement.
2, the utility model is only on the basis of original measuring system, adds a transit or Auto-collimation angular measurement light pipe more, and structure is simple, is easy to realize.
3, the utility model have employed rotation platform make the anglec of rotation of Sagnac interferometer be easy to control, the stability when system of ensure that is measured.
Accompanying drawing explanation
Fig. 1 is the structural representation of existing measuring system;
Fig. 2 and Fig. 3 is the structural representation of measuring system of the present utility model;
Fig. 4 is the imaging schematic diagram of Auto-collimation angular measurement light pipe target surface center and target beam primary importance, the second place.
1-first transit, 2-second transit, 3-Sagnac interferometer, 4-Auto-collimation angular measurement light pipe.
Embodiment
In order to overcome the not high problem of the measuring accuracy that occurs when prior art is measured the two-arm angular error of Sagnac interferometer, the utility model proposes a kind of Sagnac interferometer two-arm angular error measuring system.
Below in conjunction with accompanying drawing 1 and accompanying drawing 2, system of the present utility model is described:
This measuring system comprises the first transit 1, second transit 2 and Auto-collimation angular measurement light pipe 4;
The target beam that first transit sends is incident in the image planes of Sagnac interferometer outgoing to the second transit after the reflection of Sagnac interferometer two-arm;
Auto-collimation angular measurement light pipe is arranged towards the second transit, makes the target beam entering the second transit can be imaged in the image planes of Auto-collimation angular measurement light pipe;
The axis of rotation of rotation platform is arranged on the intersection point of the first transit optical axis and Sagnac interferometer light splitting surface.
Adopt said system, the placement location of the first transit and the second transit does not need very accurate, and (this case is 90 °) only needs the second transit can receive in image planes by target beam, avoid measuring error.
Especially, it should be noted that: in this measuring system, Auto-collimation angular measurement light pipe 4 can replace with the instrument for light beam imaging, such as: transit.
According to said system, now the method for this system is utilized to be described:
Step 1) obtain the primary importance of target beam;
Step 1.1) Sagnac interferometer is arranged on rotation platform;
Step 1.2) open the first transit, the second transit and Auto-collimation angular measurement light pipe, the first transit sends target beam, and target beam is received by the second transit after the reflection of Sagnac interferometer two-arm;
Step 1.3) pull down Sagnac interferometer, in the image planes being imaged on Auto-collimation angular measurement light pipe of the target beam that the second transit receives, obtain the primary importance of target beam;
Step 2) obtain the second place of target beam;
Step 2.1) again Sagnac interferometer to be measured is installed on a spinstand, by Sagnac interferometer according to step 1.1) be arranged on position half-twist;
Step 2.2) the first transit sends target beam, and target beam is received by Auto-collimation angular measurement light pipe after the reflection of Sagnac interferometer two-arm, obtains the second place of target beam;
Step 3) according to the primary importance of target beam on Auto-collimation angular measurement light pipe and the distance calculating Sagnac interferometer two-arm angular error of the second place, physical relationship formula is:
δ=(1/2)arctg(θ/2f)
If: δ is Sagnac interferometer two-arm angular error, and θ is the distance of target beam on Auto-collimation angular measurement light pipe between primary importance and the second place; F is Auto-collimation angular measurement light pipe focal length.
Wherein, it should be noted that: the step 2 completing said method) time, Sagnac interferometer half-twist can be completed by hand by operating personnel.
Claims (2)
1. a sagnac interferometer two-arm angular error measuring system, is characterized in that: comprise the first transit, the second transit, rotation platform and Auto-collimation angular measurement light pipe;
The target beam that described first transit sends is incident in the image planes of sagnac interferometer outgoing to the second transit after the reflection of sagnac interferometer two-arm;
Described Auto-collimation angular measurement light pipe is arranged towards the second transit, makes the target beam entering the second transit can be imaged in the image planes of Auto-collimation angular measurement light pipe;
The axis of rotation of described rotation platform is arranged on the intersection point of the first transit optical axis and sagnac interferometer light splitting surface.
2. sagnac interferometer two-arm angular error measuring system according to claim 1, is characterized in that: the Auto-collimation angular measurement light pipe in described measuring system is replaced by transit.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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CN201420820436.0U CN204514568U (en) | 2014-12-20 | 2014-12-20 | A kind of sagnac interferometer two-arm angular error measuring system |
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CN201420820436.0U CN204514568U (en) | 2014-12-20 | 2014-12-20 | A kind of sagnac interferometer two-arm angular error measuring system |
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CN201420820436.0U Expired - Fee Related CN204514568U (en) | 2014-12-20 | 2014-12-20 | A kind of sagnac interferometer two-arm angular error measuring system |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104568382A (en) * | 2014-12-20 | 2015-04-29 | 中国科学院西安光学精密机械研究所 | System and method for measuring angle error of two arms of Sagnac interferometer |
CN111240032A (en) * | 2020-02-20 | 2020-06-05 | 中国科学院西安光学精密机械研究所 | Spectrometer debugging method based on Sagnac entity interferometer |
-
2014
- 2014-12-20 CN CN201420820436.0U patent/CN204514568U/en not_active Expired - Fee Related
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104568382A (en) * | 2014-12-20 | 2015-04-29 | 中国科学院西安光学精密机械研究所 | System and method for measuring angle error of two arms of Sagnac interferometer |
CN104568382B (en) * | 2014-12-20 | 2017-04-19 | 中国科学院西安光学精密机械研究所 | System and method for measuring angle error of two arms of Sagnac interferometer |
CN111240032A (en) * | 2020-02-20 | 2020-06-05 | 中国科学院西安光学精密机械研究所 | Spectrometer debugging method based on Sagnac entity interferometer |
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C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20150729 Termination date: 20171220 |
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CF01 | Termination of patent right due to non-payment of annual fee |