CN109579739A - A kind of off-axis refraction-reflection type part compensator system and design method - Google Patents

A kind of off-axis refraction-reflection type part compensator system and design method Download PDF

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CN109579739A
CN109579739A CN201910011881.XA CN201910011881A CN109579739A CN 109579739 A CN109579739 A CN 109579739A CN 201910011881 A CN201910011881 A CN 201910011881A CN 109579739 A CN109579739 A CN 109579739A
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compensator
aberration
rotational symmetry
reflection type
type part
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CN109579739B (en
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郝群
鹿丽华
胡摇
付诗航
赵亚如
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Beijing Institute of Technology BIT
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • G01B11/2441Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures using interferometry

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Abstract

The present invention relates to a kind of off-axis refraction-reflection type part compensator system and design methods, belong to photoelectric detection technology field.The compensator system includes two-stage compensator, system design optimization method establishes the unified spherical aberration of system, astigmatism relational expression using third-order aberration theory, the equation group about compensator structure parameter is established in conjunction with paraxial rays formula, genetic algorithm is combined to solve initial structure parameter and model in optical design software later, setting optimization aim, optimization operand and optimized variable optimize, and realize the detection to non-rotational symmetry non-spherical surface pattern.Structure is simple and easy to implement for present system, one-to-many surface testing can be achieved, reduce the design difficulty and processing cost of compensator, simultaneously, the design of Compensator method can effectively obtain initial configuration global optimum, the self-defect of existing optical design software is effectively avoided, non-rotational symmetry Aspherical-surface testing precision is improved.

Description

A kind of off-axis refraction-reflection type part compensator system and design method
Technical field
The present invention relates to a kind of compensator system for being detected to non-rotational symmetry non-spherical element and design sides Method belongs to photoelectric detection technology field.
Background technique
Aspherical is widely applied one kind optical element in contemporary optics system.It is aspherical, especially non-rotational symmetry It is aspherical, a variety of aberrations can be corrected simultaneously, can be effectively improved system imaging quality, increase optical design freedom, improve system The advantages such as the flexibility for design of uniting, make it play highly important role in various fields.But for non-rotating right Claim aspherical detection then relative difficulty, its machining accuracy is caused to be difficult to ensure always, therefore, finds a kind of high-precision, structure Simple non-rotational symmetry Aspherical-surface testing method, is the problem that field of photodetection is in the urgent need to address at this stage.
In existing non-rotational symmetry Aspherical-surface testing method, interferometry measurement is a kind of high-precision, high sensitivity Detection means is broadly divided into two classes: zero-compensation interferometry and part compensating interferometer method.Wherein, zero-compensation interferometry is to compensate The normal aberration of tested surface is fully compensated when device designs, to realize interferometry.Currently, common zero-compensation interferometry side Method mainly has: computed hologram penalty method, Dall penalty method, Offner penalty method, etc..But the common spy of these methods Point is: design of Compensator and difficulty of processing are higher, and a kind of compensator is only capable of compensating the aspherical of a certain special parameter, Measurement dynamic range is small, poor universality.Part compensating interferometer method overcome zero-compensation interferometry there are the problem of, effectively increase The versatility of compensator, and the design and difficulty of processing of compensator also relative reduction.But it is aspherical for non-rotational symmetry Detection, because tested surface introduces such as astigmatism, coma non-rotational symmetry aberration, the aberration for needing to compensate is relative complex, this for The calculating and design of compensator structure have extremely challenging.
In the existing part compensating interferometer method aspherical for non-rotational symmetry, Chinese invention patent CN105352451B gives a kind of omnipotent compensating glass of standard and design method based on deformable mirror.But this method design knot Fruit is very big to the design accuracy dependence of first order compensator, that is, lens or lens group, and second level compensator, that is, deformable mirror Face type designs the optimization for the optical design software that places one's entire reliance upon, and optimization process easily falls into local optimum, leads to not obtain Meet the compensator of design objective, and deformable mirror itself has the shortcomings that control difficulty is high, at high cost.
The aspherical interferometry difficult point of non-rotational symmetry is the calculating, design and processing of compensator.In order to solve The deficiencies in the prior art, need to study that a kind of structure is simple, the higher compensator of detection accuracy, and carry out to its calculation method excellent Change, design result is avoided to fall into local optimum in optimization process.
Summary of the invention
The purpose of the present invention is to solve structure is complicated existing for existing compensator, component is at high cost and optimum results The problems such as easily falling into local optimum proposes a kind of off-axis refraction-reflection type part compensator system and design method, it is intended to utilize The relatively simple lens of structure or lens group and spherical reflector constitute off-axis refraction-reflection type part compensator, realize to non-rotating right Claim the compensation of aberration, can meet interference fringe it is detectable under the premise of, the aspherical inspection of raising non-rotational symmetry as far as possible Survey precision.
The purpose of the present invention is what is be achieved through the following technical solutions.
A kind of off-axis refraction-reflection type part compensator system aspherical for non-rotational symmetry, comprising: ccd detector, at As object lens, collimation laser, spectroscope, reference mirror, first order compensator, second level compensator, first order compensator and the second level Compensator together constitutes off-axis refraction-reflection type part compensator.
Wherein, first order compensator is made of lens or lens group, for generating aberration (such as ball with rotational symmetry Difference), realize the compensation to tested surface rotational symmetry aberration, meanwhile, by controlling the bias and inclination of first order compensator, generate Non-rotational symmetry aberration, for compensating the low order non-rotational symmetry aberration of tested surface.Second level compensator is that off-axis spherical surface is anti- Mirror is penetrated, by controlling its eccentric and inclination, realizes the compensation to non-rotational symmetry higher order aberratons.
The optical path that above-mentioned building block is constituted are as follows: collimation laser passes through spectroscope, and light beam reflects to form reference light, a branch of Light transmission forms measurement light, measures light through reference mirror, first order compensator, second level compensator, non-rotational symmetry aspheric to be measured It is reflected behind face, again passes by second level compensator, first order compensator, and penetrate reference mirror, formed and interfered with reference light Striped is observed at ccd detector by image-forming objective lens.
The present invention proposes a kind of design optimization method for above system simultaneously.Firstly, based on third-order aberration theory, Equation is analyzed whole system and established to paraxial rays theory etc., is derived and is calculated initial configuration.Later, with optical design Software is design platform, and system initial structure parameter is arranged, and according to actual needs, initial optimization is carried out to initial system, with full The geometrical relationship requirement of pedal system structure.Finally, carrying out two to system using the system after initial optimization as new initial configuration Suboptimization, to obtain the system for meeting the aspherical face shape error detection of non-rotational symmetry.
Beneficial effect
1, the configuration of the present invention is simple is easily realized, only needs the relatively simple lens of structure, spherical reflector that non-rotation can be realized Turn the detection of symmetric aspheres, the calibration and adjustment of system are relatively easy, and as part compensator, may be implemented one-to-many Surface testing effectively reduces the design difficulty and processing cost of compensator;
2, the design method of the compensator fully considers the characteristics of non-rotational symmetry aberration, and combines genetic algorithm, obtains The global optimum of initial structure parameter effectively avoids that design result is caused to fall into part most because of optical design software self-defect The figure of merit and the problem of be unable to satisfy design objective.
Detailed description of the invention
Fig. 1 is application schematic diagram example of the part compensator of the present invention in fizeau interferometer;
Fig. 2 is compensator detection method flow chart in part of the present invention;
Wherein, 1- collimation laser, 2- spectroscope, 3- reference mirror, 4- first order compensator, the second level 5- compensator, 6- at As object lens, 7-CCD detector, 8- non-rotational symmetry to be measured is aspherical.
Specific embodiment
It elaborates with reference to the accompanying drawings and examples to the present invention.
As shown in Figure 1, a kind of off-axis refraction-reflection type part compensator system aspherical for non-rotational symmetry, comprising: quasi- Straight laser 1, spectroscope 2, reference mirror 3, first order compensator 4, second level compensator 5, image-forming objective lens 6 and ccd detector 7.The First-order compensators 4 and second level compensator 5 together constitute off-axis refraction-reflection type part compensator.
Wherein, first order compensator 4 is made of lens or lens group, for generating the aberration with rotational symmetry (such as Spherical aberration), realize the compensation of 8 rotational symmetry aberration aspherical to non-rotational symmetry to be measured, meanwhile, by controlling first order compensator 4 bias and inclination generates non-rotational symmetry aberration, the low order non-rotational symmetry picture for non-rotational symmetry to be measured aspherical 8 Difference.Second level compensator 5 is off-axis spherical reflector, by controlling its eccentric and inclination, is realized to non-rotational symmetry high-order The compensation of aberration.
The optical path that above-mentioned building block is constituted are as follows: collimation laser 1 passes through spectroscope 2, and light beam reflects to form reference light, and one Beam light transmission forms measurement light.Light is measured through reference mirror 3, first order compensator 4, second level compensator 5, non-rotational symmetry to be measured It is reflected after aspherical 8, second level compensator 5, first order compensator 4 is again passed by, and penetrate reference mirror 3, with reference light Interference fringe is formed, is observed at ccd detector 7 by image-forming objective lens 6.
A kind of off-axis refraction-reflection type part compensator system design method, specifically includes the following steps:
Step 1: determining the basic parameter of system.
Basic parameter, including Entry pupil diameters D and wavelength X are set based on system structure.
Step 2: establishing the equation group about system structure parameter.
Firstly, establishing the aberration coefficients relational expression of whole system by third-order aberration theory.In order to simplify design, consider Not with the spherical aberration S of off-axis amount variationAnd non-rotational symmetry aberration astigmatism S, to realize the benefit of non-rotational symmetry aspherical aberration It repays.Spherical aberration SAnd astigmatism SExpression formula be respectively as follows:
SI=∑ hP+ ∑ h Δ P (1)
Wherein:
J=n (uhz-uzh) (7)
In formula, h is the first auxiliary light i.e. height of incidence of rim ray, hzIt is the incidence height of the second auxiliary light Degree, i are incidence angles, and i' is the angle of emergence, and u is object space angular aperture, and u' is image space angular aperture, and n and n' respectively indicate the refraction of incidence side Rate and transmission or reflection side's refractive index, k are secondary aspherical coefficient, R0For the vertex curvature radius of tested surface, uzIt is the second auxiliary Angle of incidence of light.
Secondly as light passes through off-axis refraction-reflection type part compensator twice, and on non-rotational symmetry to be measured is aspherical Only reflection is primary, and the aberration governing equation established between system and tested surface is as follows:
2SI is mended+SI is non-=0 (8)
2SIII mends+SIII is non-=0 (9)
Wherein, SI mendsIt is the spherical aberration of off-axis refraction-reflection type part compensator, SI is non-It is the ball of the aspherical generation of non-rotational symmetry to be measured Difference.SIII mendsIt is the astigmatism of off-axis refraction-reflection type part compensator, SIII mendsIt is the astigmatism of the aspherical generation of non-rotational symmetry to be measured.It is establishing When aberration relational expression, to consider off-axis refraction-reflection type part compensator and tested surface it is unified between aberration relationship, sufficiently to examine Consider the aberration introduced due to system non-rotational symmetry.
Again, using paraxial rays expression formula, each refraction, reflecting surface image side angular aperture are established about radius of curvature Equation:
Wherein, r is each refraction, the corresponding radius of curvature of reflecting surface.To sum up, by formula (8), (9), (10) establish about from The equation group of axis refraction-reflection type part compensator structure parameter.
Step 3: utilizing Mathematical tool, solve above-mentioned equation group, obtain off-axis refraction-reflection type part compensator and initially tie Structure parameter.
According to priori knowledge and the design requirement of real system, be arranged lens (group) vertex to spherical reflector vertex it Between distance d1And spherical reflector vertex is to the distance d between non-rotational symmetry aspheric vertex of surface to be measured2.It is asked based on genetic algorithm Off-axis refraction-reflection type part compensator initial structure parameter is solved, the overall situation of off-axis refraction-reflection type part compensator initial structure parameter is obtained Optimal value is iterated calculating on this basis, obtains the off-axis refraction-reflection type part compensator initial configuration eventually for modeling Parameter.
Step 4: utilizing optical design software, system structure is modeled and is optimized.
Firstly, the initial structure parameter obtained according to step 3 models system in optical design software, avoid The problem of causing design result to fall into local optimum because of optical design software self-defect.
Secondly, the bias of initial structure parameter and off-axis refraction-reflection type part compensator that setting acquires and inclination are optimization Variable carries out initial optimization to system using wavefront PV as optimization aim, with overcome because it is paraxial it is approximate caused by rim ray without Method enters the problem of system.If there is light occlusion issue in system, by combining ZPL instruction to control ray position, and Using the system after initial optimization as new initial system.
System after the completion of initial optimization can guarantee that rim ray enters system and dull thread occlusion issue.In this base On plinth, double optimization is carried out to system, optimized variable and optimization aim are identical as initial optimization, interfere at image planes to obtain Striped is relatively sparse as a result, the remaining wavefront of record at this time.
Step 5: judging whether design result is feasible.
The maximum wavefront slope K for calculating remaining wavefront, judges whether interference fringe at this time is detectable.In general, selected CCD The pixel number of detector is 1024 pixels × 1024 pixels, and the maximum spatial frequency of corresponding detectable interference fringe is about 0.45 When λ/pixel, i.e. K≤0.45 λ/pixel, interference fringe is detectable, and otherwise, interference fringe is not detectable, the structural parameters of system Design objective is not met, return step 4 is needed to re-start system parameter settings, and optimizes and is up to meeting design objective Only.
Embodiment
The aspherical non-rotational symmetry of this example measurement is the relatively simple off axis paraboloid mirror of structure, and bore is 76.2mm, vertex curvature radius 889mm, asphericity coefficient are -1, and off-axis amount is 10mm.Design off-axis refraction-reflection type part compensation Device detection system, it is as shown in Figure 2 to the detailed process of non-rotational symmetry aspheric surface error-detecting to realize.
Step 1: determining system basic parameter.
Based on system structure, the Entry pupil diameters D=81mm of system, wavelength X=532nm are set.
Step 2: establishing the equation group about system structure parameter.
The equation group of system initial structure parameter is established according to third-order aberration theory, paraxial rays formula, wherein astigmatism and Spherical aberration relational expression need to consider it is unified, to fully consider the influence of the introduced aberration of non-rotational symmetry tested surface.
Step 3: solving above-mentioned equation group using Mathematical tool, solve off-axis refraction-reflection type part compensator initial configuration Parameter.
According to priori knowledge and the design requirement of real system, be arranged lens (group) vertex to spherical reflector vertex it Between distance d1=100mm and spherical reflector vertex are to the distance d between non-rotational symmetry aspheric vertex of surface to be measured2=-500mm. Solve the global optimum of off-axis refraction-reflection type part compensator initial configuration based on genetic algorithm, and in this, as iterative initial value, Solution obtains the initial structure parameter for system modelling, i.e. the radius of curvature r of two optical surfaces of lens1=-8.5787mm, r2=-8.2617mm, the radius of curvature r of spherical reflector3=-323.0668mm
Step 4: utilizing optical design software, system structure is modeled and is optimized.
The present embodiment selects ZEMAX as optical design software.In ZEMAX, the initial configuration that is obtained according to step 3 Parameter models system, and optimized variable, optimization aim and optimization operand is arranged, and unites to system and carries out initial optimization, To guarantee that light is able to enter system and dull thread circumstance of occlusion.On this basis, double optimization is carried out to system, finally obtained System optical parameter be r1=168.217619mm, r2=-1030.439322mm, r3=-89.718106mm, spherical surface are anti- Penetrate aperture of mirror D3=9.375m3m3,2d1=291.980398mm, d2=-843.885967mm, lens and spherical reflector it is inclined The heart and inclination are respectively L1decenter=1.173455mm, L1tilt=0.005740054 °, M1decenter=-0.038789mm, M1tilt=-10 °.
Step 5: judging whether design result is feasible.
Read the system spare wavefront after the completion of optimization, calculate residue wavefront maximum wavefront slope K=0.373 λ 8 as/it is plain, Maximum 0.45 λ of the wavefront slope/pixel for meeting the detectable interference fringe of detector then can determine whether to obtain in the embodiment and interfere item Line can be detected, and designed off-axis refraction-reflection type part compensator is suitble to.

Claims (3)

1. a kind of off-axis refraction-reflection type part compensator system, which is characterized in that including collimation laser (1), spectroscope (2), reference Mirror (3), first order compensator (4), second level compensator (5), image-forming objective lens (6) and ccd detector (7);First order compensator (4) and second level compensator (5) together constitutes off-axis refraction-reflection type part compensator;
Wherein, first order compensator (4) is made of lens or lens group, for generating aberration (such as ball with rotational symmetry Difference), realize the compensation of (8) rotational symmetry aberration aspherical to non-rotational symmetry to be measured, meanwhile, by controlling first order compensator (4) bias and inclination generate non-rotational symmetry aberration, and the low order for non-rotational symmetry to be measured aspherical (8) is non-rotating right Claim aberration;Second level compensator (5) is off-axis spherical reflector, by controlling its eccentric and inclination, is realized to non-rotating right Claim the compensation of higher order aberratons;
The optical path that above-mentioned building block is constituted are as follows: collimation laser (1) passes through spectroscope (2), and light beam reflects to form reference light, and one Beam light transmission forms measurement light;Light is measured through reference mirror (3), first order compensator (4), second level compensator (5), non-rotation to be measured Turn symmetric aspheres (8) to reflect afterwards, again passes by second level compensator (5), first order compensator (4), and through reference Mirror (3) forms interference fringe with reference light, is observed at ccd detector (7) by image-forming objective lens (6).
2. a kind of off-axis refraction-reflection type part compensator system design method, which comprises the following steps:
Step 1: determining the basic parameter of system;
Basic parameter, including Entry pupil diameters D and wavelength X are set based on system structure;
Step 2: establishing the equation group about system structure parameter;
Firstly, establishing the aberration coefficients relational expression of whole system by third-order aberration theory;Consider not with off-axis amount variation Spherical aberration SAnd non-rotational symmetry aberration astigmatism S, to realize the compensation of non-rotational symmetry aspherical aberration, spherical aberration SAnd astigmatism S Expression formula be respectively as follows:
SI=∑ hP+ ∑ h Δ P (1)
Wherein:
J=n (uhz-uzh) (7)
In formula, h is the first auxiliary light i.e. height of incidence of rim ray, hzIt is the height of incidence of the second auxiliary light, i is Incidence angle, i' are the angles of emergence, and u is object space angular aperture, and u' is image space angular aperture, and n and n' respectively indicate incidence side's refractive index and thoroughly It penetrates or reflection side refractive index, k is secondary aspherical coefficient, R0For the vertex curvature radius of tested surface, uzIt is that the second auxiliary light enters Firing angle;
Secondly, the aberration governing equation established between system and tested surface is as follows:
2SI is mended+SI is non-=0 (8)
2SIII mends+SIII is non-=0 (9)
Wherein, SI mendsIt is the spherical aberration of off-axis refraction-reflection type part compensator, SI is non-It is the spherical aberration of the aspherical generation of non-rotational symmetry to be measured; SIII mendsIt is the astigmatism of off-axis refraction-reflection type part compensator, SIII mendsIt is the astigmatism of the aspherical generation of non-rotational symmetry to be measured;Establishing picture When poor relational expression, to consider off-axis refraction-reflection type part compensator and tested surface it is unified between aberration relationship, to fully consider Due to the introduced aberration of system non-rotational symmetry;
Again, using paraxial rays expression formula, each refraction, equation of the reflecting surface image side angular aperture about radius of curvature are established Formula:
Wherein, r is each refraction, the corresponding radius of curvature of reflecting surface;To sum up, it is established by formula (8), (9), (10) about off-axis folding The equation group of trans- part compensator structure parameter;
Step 3: utilizing Mathematical tool, solve above-mentioned equation group, obtain off-axis refraction-reflection type part compensator initial configuration ginseng Number;
According to priori knowledge and the design requirement of real system, the distance between setting lens apex to spherical reflector vertex d1And spherical reflector vertex is to the distance d between non-rotational symmetry aspheric vertex of surface to be measured2;Off-axis folding is solved based on genetic algorithm Trans- part compensator initial structure parameter obtains the global optimum of off-axis refraction-reflection type part compensator initial structure parameter, It is iterated calculating on this basis, obtains the off-axis refraction-reflection type part compensator initial structure parameter eventually for modeling;
Step 4: utilizing optical design software, system structure is modeled and is optimized;
Firstly, the initial structure parameter obtained according to step 3 models system in optical design software, avoid because of light Learn the problem of design software self-defect causes design result to fall into local optimum;
Secondly, the bias of initial structure parameter and off-axis refraction-reflection type part compensator that setting acquires and inclination become for optimization Amount carries out initial optimization to system using wavefront PV as optimization aim, with overcome because it is paraxial it is approximate caused by rim ray can not The problem of into system;If there is light occlusion issue in system, by combining ZPL instruction to control ray position, and will System after initial optimization is as new initial system;
System after the completion of initial optimization can guarantee that rim ray enters system and dull thread occlusion issue;On this basis, Double optimization is carried out to system, optimized variable and optimization aim are identical as initial optimization, to obtain the interference fringe at image planes It is relatively sparse as a result, record remaining wavefront at this time;
Step 5: judging whether design result is feasible;
The maximum wavefront slope K for calculating remaining wavefront, judges whether interference fringe at this time is detectable;If interference fringe can not be visited It surveys, illustrates that the structural parameters of system do not meet design objective, need return step 4 to re-start system parameter settings, and carry out excellent Change until meeting design objective.
3. a kind of off-axis refraction-reflection type part compensator system design method as claimed in claim 2, which is characterized in that step 5 In, judge the whether detectable method of interference fringe are as follows:
If the pixel number of selected ccd detector (7) is 1024 pixels × 1024 pixels, the maximum of corresponding detectable interference fringe Spatial frequency is about 0.45 λ/pixel, i.e., when maximum wavefront slope K≤0.45 λ/pixel of remaining wavefront, interference fringe can be visited It surveys, otherwise, interference fringe is not detectable.
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CN113409256A (en) * 2021-06-08 2021-09-17 沈阳化工大学 Axial size detection method for pipeline corrugated compensator

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JPH08249669A (en) * 1995-03-07 1996-09-27 Nec Corp Method and apparatus for correcting astigmatic difference of optical head
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Publication number Priority date Publication date Assignee Title
CN113409256A (en) * 2021-06-08 2021-09-17 沈阳化工大学 Axial size detection method for pipeline corrugated compensator
CN113409256B (en) * 2021-06-08 2023-09-15 沈阳化工大学 Method for detecting axial dimension of pipeline corrugated compensator

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