CN104807548A - Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method - Google Patents

Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method Download PDF

Info

Publication number
CN104807548A
CN104807548A CN201510216017.5A CN201510216017A CN104807548A CN 104807548 A CN104807548 A CN 104807548A CN 201510216017 A CN201510216017 A CN 201510216017A CN 104807548 A CN104807548 A CN 104807548A
Authority
CN
China
Prior art keywords
computing machine
shearing
light modulator
spatial light
measured
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201510216017.5A
Other languages
Chinese (zh)
Inventor
戴凤钊
王向朝
唐锋
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Optics and Fine Mechanics of CAS
Original Assignee
Shanghai Institute of Optics and Fine Mechanics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CN201510216017.5A priority Critical patent/CN104807548A/en
Priority to PCT/CN2015/080419 priority patent/WO2016173079A1/en
Publication of CN104807548A publication Critical patent/CN104807548A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J9/00Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength
    • G01J9/02Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength by interferometric methods
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M11/00Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
    • G01M11/02Testing optical properties

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Instruments For Measurement Of Length By Optical Means (AREA)
  • Testing Of Optical Devices Or Fibers (AREA)

Abstract

Disclosed are a digital phase-shifting lateral shearing interferometer and an optical system wave aberration measurement method. The interferometer is composed of a light source, a small-hole mask, a first spatial light modulator, a second spatial light modulator, a two-dimensional photoelectric detector and a computer. The first spatial light modulator is arranged as a grating by computer programming to serve as a shearing light splitter, the second spatial light modulator is arranged as a double-window mask to serve as a filter for filtering high-order diffraction light at zero order and more than two orders, and only diffraction light at +1 order and -1 order takes part in interference. The problem that the high-order diffraction light takes part in interference is solved, the interferometer has the advantage that changeable shearing direction and adjustable shearing rate can be realized without replacing or rotating any device.

Description

Digital phase-shifting technique lateral shearing interferometer and optical system wavefront aberration measuring method
Technical field
The invention belongs to field of optical detection, be specifically related to the measuring method of a kind of digital phase-shifting technique lateral shearing interferometer and optical system wavefront aberration.
Background technology
Lateral shearing interference tool has the following advantages:
1) wavefront to be measured and the transverse translation of himself produce and interfere, and eliminate the demand to high precision reference wavefront, therefore have very high measuring accuracy;
2) be a kind of concurrent path interference system, therefore insensitive to mechanical vibration, air turbulence, measuring system is stablized;
3) low to the spatial coherence requirement of light source, traditional two-beam interference based on reference wave requires wavefront to be measured all spatial coherence in whole pupil to be measured, and lateral shearing interference only requires that the Spatially coherent length of light source is not less than shear distance;
4) sensitivity of measuring system is adjustable, can change the sensitivity of measuring system by changing shearing displacement.Therefore, lateral shear is widely used in wavefront measurement field, as the surface topography measurement of optical element, the wave aberration measurement, X ray wavefront measurement etc. of optical system.
Particularly this technology has been applied in high-end litho machine, for the in site measurement of photoetching projection objective lens.Litho machine is the representative of global high-end equipment, it is the height fusion of ultraprecise, Iarge-scale system, the engineering limit, it is all very high to the index request of each subsystem, wherein the wave aberration of projection objective system has controlled at below 0.6nm, and this proposes high requirement to the precision of wave aberration detection technique.And the 193nm wave aberration of photoetching projection objective in situ detection technology that lateral shearing interference technology is commercial just, range of application contains the litho machine of 90nm node to 1x nm node.In addition, lateral shearing interference technology is also the mainstream technology that extreme ultraviolet lithography projection objective wave aberration detects.
The device producing wave front shearing has a lot of method, as flat plate shear, prism shearing, grating shearing, polarization shearing etc.For high-precision wavefront measurement, usually need to adopt phase shift interference technology, grating shearing is interfered owing to being convenient to introduce phase shift, become mainstream technology scheme in high precision wavefront measurement field, the projection objective wave aberration detection as 193nm photoetching and extreme ultraviolet photolithographic all have employed grating as shearing light-splitting device.Grating shearing is interfered by adopting PZT to drive spectro-grating at shear direction transverse shifting, phase differential between the secondary light of different diffraction level is changed, grating moves one-period, phase differential between 0 grade and ± 1 order diffraction light changes 2 π, is participating in introducing phase shift between the two-beam of interfering in this way.And use PZT generation phase shift usually to need to calibrate its voltage, and PZT phase shift is easily subject to the impact of nonlinear effect (as hesitation, thermal drift etc.).Document (S.Zhao andP.Chung, " Digital speckle shearing interferometer using a liquid-crystal spatial lightmodulator, " Opt.Eng.45, 105606 (2006)) a kind of digital speckle-shearing interferometry instrument is proposed, reflection type liquid crystal spatial light modulator (LC-SLM) is adopted to replace grating, and produce digital raster with calculating control LC-SLM, as shearing light-splitting device, can be moved by computer programming control LC-SLM grating lines, realize phase shift, avoid conventional P ZT phase shift Problems existing.But this theoretical method is two-beam interference, and the light participating in interfering is+1 and-1 order diffraction light of LC-SLM grating, but in fact there is Advanced Diffraction light, and the light participating in interfering not only has+1 grade and-1 light, also comprises the Advanced Diffraction light of more than 0 grade and 2 grades.
The method solving Advanced Diffraction optical issue has three kinds: (1) is by optimal design LC-SLM grating, suppress 0 grade and Advanced Diffraction light (in first technology [1]: A.Cornejo and D.Malacara, " Ronchi Test of AsphericalSurfaces; Analysis; and Accuracy; " Appl.Opt.9,1897-1901 (1970); (2) by optimal design LC-SLM grating, suppress the Advanced Diffraction light of more than 2 grades, retain 0 grade and+1 grade and-1 order diffraction beche-de-mer without spike and interference, i.e. Three-beam Interfere, phase place is extracted (at first technology [2] Si-Hong Zhai by special phase extraction method, Jianping Ding, Jing Chen, Ya-Xian Fan, and Hui-Tian Wang, " Three-wave shearinginterferometer based on spatial light modulator, " Opt.Express 17,970-977 (2009)); (3) by adopting Dual-window mask, filtering 0 grade and Advanced Diffraction light, ensure that two-beam interference is (at first technology [3]: YucongZhu, Katsumi Sugisaki, Katsuhiko Murakami, et al., Shearing Interferometry for atWavelength Wavefront Measurement of Extreme-Ultraviolet Lithography ProjectionOptics, Jpn.J.Appl.Phys 42,5844 – 5847 (2003)).In actual applications, for common LC-SLM, method (1) is difficult to the Advanced Diffraction light simultaneously eliminating more than 0 grade and 2 grades, method (2) needs the phase extraction method adopting particular design, range of application is restricted, and method (3) can be good at the Advanced Diffraction light of filtering more than 0 grade and 2 grades, makes+1 order diffraction beche-de-mer without spike and interference, also by changing Dual-window mask, 0 grade of light and+1 grade of (or-1 grade) beche-de-mer without spike and interference can be selected.But method (3) needs when changing shear direction or shearing rate to change (or rotation) wave filter, makes troubles, also can introduce extra measuring error to measurement simultaneously.
Summary of the invention
The object of the invention is to overcome the above-mentioned deficiency in first technology, a kind of digital phase-shifting technique lateral shearing interferometer and optical system wavefront aberration measuring method are provided, this interferometer structure adopts spatial light modulator as the digital space wave filter of image planes, can with Physical space digital filter with the use of, make the change of shear direction and shearing rate more convenient, eliminate because of the measuring error changed or rotary device brings.
Technical solution of the present invention is as follows:
A kind of digital phase-shifting technique lateral shearing interferometer, its feature is that this interferometer comprises light source, be little aperture mask, the first spatial light modulator, second space photomodulator and 2 D photoelectric detector successively along this light source output beam direction, the output terminal of this 2 D photoelectric detector is connected with the input end of computing machine; The first described spatial light modulator and second space photomodulator are placed on the first three-D displacement platform and the second three-D displacement platform respectively; The first described spatial light modulator is connected with the output terminal of computing machine respectively with the input end of second space photomodulator;
Described little aperture mask is one piece of square shadow shield, has the aperture of a printing opacity at the center of this shadow shield, and the diameter of this printing opacity aperture is less than the object space resolution of optical system to be measured;
The first described spatial light modulator is transmissive spatial photomodulator, control to produce digital raster by computing machine, as shearing light-splitting device, wavefront to be measured is diffracted to multi-level diffraction light, when carrying out the shearing measurement of x direction, the lines shearing grating distribute in the y-direction, comprise light transmission part and lightproof part; When carrying out the shearing measurement of y direction, the lines shearing grating in the x-direction, comprise light transmission part and lightproof part;
Described second space photomodulator is transmissive spatial photomodulator, control to produce Dual-window mask by computing machine, as spatial filter, filtering 0 grade and the Advanced Diffraction light of more than 2 grades, when carrying out the shearing measurement of x direction, in the x-direction, comprise two optical transmission windows, other parts are set to light tight the line of centres of Dual-window mask, when carrying out the shearing measurement of y direction, in the y-direction, comprise two optical transmission windows, other parts are set to light tight Dual-window mask center line;
Described two-dimension photoelectric sensor is CCD, CMOS or 2 D photoelectric detector array.
Digital phase-shifting technique lateral shearing interferometer described in utilization is to the measuring method of optical system wavefront aberration, and its feature is that the method includes the steps of:
1) interferometer system parameter is calculated:
The shearing rate s of setting interferometer, shearing rate s is value between 1% ~ 20% generally, measures for high-precision wave aberration, generally value between 1% to 5%, the interference fringe quantity N of setting interferometer, generally value between 20 ~ 100; According to the shearing rate s of setting, the image-side numerical aperture NA of optical system to be measured and the wavelength X of light source, calculate the screen periods p of the first spatial light modulator by formula p=λ/(s × NA); According to the number of interference fringes N of setting, the image-side numerical aperture NA of screen periods p and optical system to be measured, calculates the distance d between the first spatial light modulator and second space photomodulator by formula d=N × p/NA; By screen periods p, the wavelength X of light source, the distance d between the first spatial light modulator and second space photomodulator of the first spatial light modulator, calculate the distance, delta between second space photomodulator Dual-window mask two window center by formula Δ=2d λ/p; According to intending the phase shift algorithm adopted and the phase-shift phase ΔΦ often walked, calculate the grating lines amount of movement Δ p often walking phase shift by formula Δ p=p × ΔΦ/4 π;
2) interferometer system is adjusted:
Optical system to be measured is placed between little aperture mask and the first spatial light modulator, adjust optical system to be measured, little aperture mask is made to be in the object plane of optical system, optical axis is made to pass the center of the printing opacity aperture of little aperture mask, the displacement platform of adjustment second space photomodulator, make the surface of second space photomodulator perpendicular to optical axis, and be in the object plane of optical system to be measured, adjust the displacement platform of the first spatial light modulator, make the surface of the first spatial light modulator perpendicular to optical axis and and distance between second space photomodulator be step 1) the value d that calculates;
3) optical system wavefront aberration is measured:
1. x direction shear interference is measured:
Controlled by computing machine, the first spatial light modulator is set to y direction grating, namely grating lines in the y-direction, and screen periods is set to described p; Controlled by computing machine, second space photomodulator is set to Dual-window mask in the x-direction, namely the line of centres of two windows is parallel to x-axis, and the distance between two window center is set to described Δ, and makes optical axis be in the center of two window center lines; Open light source, detect interference light intensity signal I by photodetector x1, and by I x1import computing machine into preserve; Computing machine controls the first spatial light modulator grating, and make it along the translation of+x (or-x) direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector x2, and by I x2import computing machine into preserve; The step of above-mentioned phase shift, interferogram detection, preservation is carried out n time, and n is the phase shift step number of phase shift algorithm, and n width phase shifting interference I preserved by final computing machine x1, I x2..., I xn; By phase shift algorithm, by the interference signal I of computer calculate by preserving x1, I x2..., I xncalculate the difference wavefront Δ W in x direction x(see D.Malacara, Optical Shop Testing, 3rd ed, (CRC Press, Taylor & Francis, 2007));
2. y direction shear interference is measured:
Controlled by computing machine, the first spatial light modulator is set to x direction grating, namely grating lines in the x-direction, and screen periods is set to the value p that step 1 calculates; Controlled by computer programming, second space photomodulator is set to Dual-window mask in the y-direction, namely two window center lines are parallel to y-axis, and the distance between two window center is set to the value Δ that step 1 calculates, and make optical axis be in the center of two window lines; Interference light intensity signal I is detected by photodetector y1, and by I y1import computing machine into preserve; Computing machine controls the first spatial light modulator grating, and make it along the translation of+y (or-y) direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector y2, and by I y2import computing machine into preserve; The step of above-mentioned phase shift, interferogram detection, preservation is carried out n time, and n is the phase shift step number of phase shift algorithm, and n width phase shifting interference I preserved by final computing machine y1, I y2..., I yn; By phase shift algorithm, by the interference signal I of computer calculate by preserving y1, I y2..., I yncalculate the difference wavefront Δ W in y direction y;
3. wavefront reconstruction:
By described x direction difference wavefront Δ W xwith the difference wavefront Δ W in y direction y, wavefront W to be measured is reconstructed by wavefront reconstruction algorithm, described wavefront reconstruction algorithm can be that type method or field method are (see Fengzhao Dai, Feng Tang, Xiangzhao Wang, Osami Sasaki, and Peng Feng, " Modal wavefrontreconstruction based on Zernike polynomials for lateral shearing interferometry:comparisons of existing algorithms, " Appl.Opt.51, 5028-5037 (2012)), systematic error is eliminated (see Jie Li to wavefront W to be measured, Feng Tang, Xiangzhao Wang, Fengzhao Dai, Feibin Wu, " Calibration of system errors in lateral shearing interferometer for EUV-wavefrontmetrology, " Proc.SPIE 9422, 94222O (2015), obtain the wave aberration of optical system to be measured.
Described phase shift algorithm is from n width interferogram, extract the method for phase place, and n represents phase shift step number, and choosing of n is determined according to real needs.
Principle of the present invention is: by adopting spatial light modulator to produce digital Dual-window mask, the Advanced Diffraction light of filtering more than 0 grade and 2 grades, the light that participation is interfered is only+1 grade and-1 order diffraction light, avoids the impact of Advanced Diffraction light, improves measuring accuracy; Match with the first spatial light modulator, make measuring system more flexible, shearing rate is not realized and shear direction is adjustable under not needing to change the condition of any device, the equal half-twist of Dual-window mask making the grating of the first spatial light modulator and second space photomodulator is controlled by computing machine, realize the change of shear direction, by calculating the cycle of control break first spatial light modulator grating, and by the distance between computing machine control break second space optical modulation Dual-window mask two window, realize the adjustment of shearing rate.
The present invention, with compared with first technology, has the following advantages:
1, with compared with first technology [1], the present invention uses Dual-window mask filtering more than 0 grade and 2 grades Advanced Diffraction light, than the better effects if adopting the method for optimization system parameter designing to suppress more than 0 grade and 2 grades Advanced Diffraction light, improves measuring accuracy;
2, with compared with first technology [2], the present invention is two-beam interference, avoids the problem that Three-beam Interfere phase shift algorithm is limited, can adopt phase shift algorithm more flexibly for actual conditions;
3, with compared with first technology [3], the present invention controls spatial light modulator by computing machine and produces Dual-window mask, present system is more flexible, can under the condition do not changed or rotate any device, realizes that shearing rate is adjustable and shear direction is variable by means of only computer programming.
Accompanying drawing explanation
Fig. 1 is digital phase-shifting technique lateral shearing interferometer structural representation of the present invention;
Fig. 2 is the little aperture mask schematic diagram in the present invention's numeral lateral shearing interferometer;
Fig. 3 is the grating schematic diagram carrying out the y direction arranged in the first spatial light modulator when x direction is sheared and measured with the present invention's numeral lateral shearing interferometer;
Fig. 4 is the grating schematic diagram carrying out the x direction arranged in the first spatial light modulator when y direction is sheared and measured with the present invention's numeral lateral shearing interferometer;
Fig. 5 is the Dual-window mask schematic diagram carrying out the x direction arranged on second space photomodulator when x direction is sheared and measured with the present invention's numeral lateral shearing interferometer;
The y direction Dual-window mask schematic diagram that Fig. 6 is arranged when being and carrying out the shearing measurement of y direction with the present invention's numeral lateral shearing interferometer on second space photomodulator;
Embodiment
Below in conjunction with embodiment and accompanying drawing, the invention will be further described, but should not limit the scope of the invention with this.
First refer to Fig. 1, Fig. 1 is the light channel structure figure of the present invention's numeral lateral shearing interferometer, as seen from Figure 1, digital phase-shifting technique shearing interferometer of the present invention, comprise light source 1, be little aperture mask 2, first spatial light modulator 4, second space photomodulator 6 and 2 D photoelectric detector 8 successively along this light source 1 output beam direction, the output terminal of this 2 D photoelectric detector 8 is connected with the input end of computing machine 9; The first described spatial light modulator 4 and second space photomodulator 6 are placed on an XYZ three-D displacement platform 5 and the 2nd XYZ three-D displacement platform 7 respectively; The first described spatial light modulator 4 is connected with the output terminal of computing machine 9 respectively with the input end of second space photomodulator 6;
Described little aperture mask 2 is one piece of square shadow shield, has the aperture 21 of a printing opacity at the center of this shadow shield, and the diameter of this printing opacity aperture 21 is less than the object space resolution of optical system 3 to be measured;
The first described spatial light modulator 4 is transmissive spatial photomodulator, control to produce digital raster by computing machine 9, as shearing light-splitting device, wavefront to be measured is diffracted to multi-level diffraction light, when carrying out the shearing measurement of x direction, the lines shearing grating distribute in the y-direction, comprise light transmission part 401 and lightproof part 402; When carrying out the shearing measurement of y direction, the lines shearing grating in the x-direction, comprise light transmission part 411 and lightproof part 412;
Described second space photomodulator 6 is transmissive spatial photomodulator, control to produce Dual-window mask by computing machine 9, as spatial filter, filtering 0 grade and the Advanced Diffraction light of more than 2 grades, when carrying out the shearing measurement of x direction, the line of centres of Dual-window mask in the x-direction, comprise two optical transmission windows 501,502, other parts are set to light tight, when carrying out the shearing measurement of y direction, in the y-direction, comprise two optical transmission windows 511,512, other parts are set to light tight Dual-window mask center line;
Described two-dimension photoelectric sensor 6 is CCD, CMOS, or 2 D photoelectric detector array;
Use above-mentioned digital lateral shearing interferometer to carry out the measuring method of optical system wavefront aberration, comprise following steps:
1) interferometer system parameter is calculated:
The shearing rate s of setting interferometer, shearing rate s is value between 1% ~ 20% generally, measures for high-precision wave aberration, generally value between 1% to 5%, the interference fringe quantity N of setting interferometer, generally value between 20 ~ 100; According to the shearing rate s of setting, the image-side numerical aperture NA of optical system 3 to be measured and the wavelength X of light source 1, calculate the screen periods p of the first spatial light modulator 4 by formula p=λ/(s × NA); According to the number of interference fringes N of setting, the image-side numerical aperture NA of screen periods p and optical system to be measured 3, calculates the distance d between the first spatial light modulator 4 and second space photomodulator 6 by formula d=N × p/NA; By screen periods p, the wavelength X of light source 1, the distance d between the first spatial light modulator 4 and second space photomodulator 6 of the first spatial light modulator 4, calculate the distance, delta between second space photomodulator 6 Dual-window mask two window center by formula Δ=2d λ/p; According to intending the phase shift algorithm adopted and the phase-shift phase ΔΦ often walked, calculate the grating lines amount of movement Δ p often walking phase shift by formula Δ p=p × ΔΦ/4 π;
2) interferometer system is adjusted
Optical system 3 to be measured is placed between little aperture mask 2 and the first spatial light modulator 4, adjust optical system 3 to be measured, little aperture mask 2 is made to be in the object plane of optical system 3, optical axis is made to pass the center of the printing opacity aperture 21 of little aperture mask 2, the displacement platform 7 of adjustment second space photomodulator 6, make the surface of second space photomodulator 6 perpendicular to optical axis, and be in the object plane of optical system 3 to be measured, adjust the displacement platform 5 of the first spatial light modulator 4, make the surface of the first spatial light modulator 4 perpendicular to optical axis and and distance between second space photomodulator 6 be step 1) the value d that calculates,
3) optical system wavefront aberration is measured:
1. x direction shear interference is measured:
Controlled by computing machine 9, the first spatial light modulator 4 is set to y direction grating, namely in the y-direction, screen periods is set to described p to grating lines 401 and 402; Controlled by computing machine 9, second space photomodulator 6 is set to Dual-window mask in the x-direction, namely the line of centres of two windows 601,602 is parallel to x-axis, distance between two window 601,602 centers is set to described Δ, and makes optical axis be in the center of two window 601,602 lines of centres; Open light source 1, detect interference light intensity signal I by photodetector 8 x1, and by I x1import computing machine 9 into preserve; Computing machine 9 controls the first spatial light modulator grating 4, and make it along the translation of+x (or-x) direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector 8 x2, and by I x2import computing machine 9 into preserve; The step of above-mentioned phase shift, interferogram detection, preservation is carried out n time, and n is the phase shift step number of phase shift algorithm, and n width phase shifting interference I preserved by final computing machine 9 x1, I x2..., I xn; By phase shift algorithm, calculate the interference signal I by preserving by computing machine 9 x1, I x2..., I xncalculate the difference wavefront Δ W in x direction x;
2. y direction shear interference is measured:
Controlled by computing machine 9, the first spatial light modulator 4 is set to x direction grating, namely in the x-direction, screen periods is set to the value p that step 1 calculates to grating lines 411 and 412; By computing machine 9 programming Control, second space photomodulator 6 is set to Dual-window mask in the y-direction, namely two window 611,612 lines of centres are parallel to y-axis, distance between two window 611,612 centers is set to the value Δ that step 1 calculates, and makes optical axis be in the center of two window 611,612 lines; Interference light intensity signal I is detected by photodetector 8 y1, and by I y1import computing machine 9 into preserve; Computing machine 9 controls the first spatial light modulator grating 4, and make it along the translation of+y (or-y) direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector 8 y2, and by I y2import computing machine 9 into preserve; The step of above-mentioned phase shift, interferogram detection, preservation is carried out n time, and n is the phase shift step number of phase shift algorithm, and n width phase shifting interference I preserved by final computing machine 9 y1, I y2..., I yn; By phase shift algorithm, calculate the interference signal I by preserving by computing machine 9 y1, I y2..., I yncalculate the difference wavefront Δ W in y direction y;
3. wavefront reconstruction:
By described x direction difference wavefront Δ W xwith the difference wavefront Δ W in y direction yreconstruct wavefront W to be measured by wavefront reconstruction algorithm, described wavefront reconstruction algorithm can be type method or field method, after eliminating systematic error, can obtain the wave aberration of optical system to be measured to wavefront W to be measured.
Give the design parameter of an embodiment below:
Light source adopts He-Ne laser instrument, wavelength is 632.8nm, shearing rate is set to 1.5%, optical system image-side numerical aperture to be measured is 0.3, image space resolution is 1.05 μm, enlargement ratio is 1/4, object-side numerical aperture is 0.075, object space resolution is 4.2 μm, the diameter of the printing opacity aperture on the little aperture mask of object space is set to 1 μm, substrate thickness is 100nm, material is chromium, the amplitude type transmissive spatial photomodulator that first spatial light modulator and second space optical modulation all select Chinese Academy of Sciences's Xi'an ray machine to research and develop, model is TSLM029-A, Pixel Dimensions is 18 μm, pixel count is 1024 × 768, the screen periods of the first spatial light modulation is 144 μm, i.e. 8 pixels, distance between second space photomodulator two window center is 90 μm, i.e. 5 pixels, two windows are square window, the length of side is 18 μm, namely 1 pixel is 1 window, number of interference fringes is 20, distance between first spatial light modulator and second space photomodulator is 10mm, experiment employing three step phase shift algorithm, often walk phase-shift phase pi/2, computing formula is for PHASE DISTRIBUTION to be measured, I 1, I 2, I 3be the interferogram intensity distributions that three phase shifts obtain, each moved further of grating distance p/8, namely 18 μm, 2 D photoelectric detector to be pixel count be 1024 × 768 CCD.
With compared with first technology, the present invention suppress 0 grade good with Advanced Diffraction light effect, measuring accuracy is higher, and system is flexible, does not need mobile or rotating optical element when changing shearing rate and shear direction.

Claims (4)

1. a digital phase-shifting technique lateral shearing interferometer, it is characterized in that this interferometer comprises light source (1), be little aperture mask (2), the first spatial light modulator (4), second space photomodulator (6) and 2 D photoelectric detector (8) successively along this light source (1) output beam direction, the output terminal of this 2 D photoelectric detector (8) is connected with the input end of computing machine (9); Described the first spatial light modulator (4) and second space photomodulator (6) are placed on the first three-D displacement platform (5) and the second three-D displacement platform (7) respectively; Described the first spatial light modulator (4) is connected with the output terminal of computing machine (9) respectively with the input end of second space photomodulator (6);
Described little aperture mask (2) is one piece of square shadow shield, have the aperture (21) of a printing opacity at the center of this shadow shield, the diameter of this printing opacity aperture (21) is less than the object space resolution of optical system to be measured (3);
Described the first spatial light modulator (4) is transmissive spatial photomodulator, control to produce digital raster by computing machine (9), as shearing light-splitting device, wavefront to be measured is diffracted to multi-level diffraction light, when carrying out the shearing measurement of x direction, the lines shearing grating distribute in the y-direction, comprise light transmission part (401) and lightproof part (402); When carrying out the shearing measurement of y direction, the lines shearing grating in the x-direction, comprise light transmission part (411) and lightproof part (412);
Described second space photomodulator (6) is transmissive spatial photomodulator, control to produce Dual-window mask by computing machine (9), as spatial filter, filtering 0 grade and the Advanced Diffraction light of more than 2 grades, when carrying out the shearing measurement of x direction, the line of centres of Dual-window mask in the x-direction, comprise two optical transmission windows (501,502), other parts are set to light tight, when carrying out the shearing measurement of y direction, in the y-direction, comprise two optical transmission windows (511,512), other parts are set to light tight Dual-window mask center line.
2. digital phase-shifting technique lateral shearing interferometer according to claim 1, is characterized in that described two-dimension photoelectric sensor (8) is CCD, CMOS or 2 D photoelectric detector array.
3. utilize digital phase-shifting technique lateral shearing interferometer described in claim 1 to the measuring method of optical system wavefront aberration, it is characterized in that the method includes the steps of:
1) interferometer system parameter is calculated:
The shearing rate s of setting interferometer, shearing rate s is value between 1% ~ 20% generally, measures for high-precision wave aberration, generally value between 1% to 5%, the interference fringe quantity N of setting interferometer, generally value between 20 ~ 100; According to the shearing rate s of setting, the image-side numerical aperture NA of optical system to be measured (3) and the wavelength X of light source (1), calculate the screen periods p of the first spatial light modulator (4) by formula p=λ/(s × NA); According to the number of interference fringes N of setting, the image-side numerical aperture NA of screen periods p and optical system to be measured (3), calculates the distance d between the first spatial light modulator (4) and second space photomodulator (6) by formula d=N × p/NA; By screen periods p, the wavelength X of light source (1), the distance d between the first spatial light modulator (4) and second space photomodulator (6) of the first spatial light modulator (4), calculate the distance, delta between second space photomodulator (6) Dual-window mask two window center by formula Δ=2d λ/p; According to intending the phase shift algorithm adopted and the phase-shift phase ΔΦ often walked, calculate the grating lines amount of movement Δ p often walking phase shift by formula Δ p=p × ΔΦ/4 π;
2) interferometer system is adjusted:
Optical system to be measured (3) is placed between little aperture mask (2) and the first spatial light modulator (4), adjust optical system to be measured (3), little aperture mask (2) is made to be in the object plane of optical system to be measured (3), the printing opacity aperture (21) of described little aperture mask (2) be centrally located on the optical axis of interferometer, the displacement platform (7) of adjustment second space photomodulator (6), make the surface of second space photomodulator (6) perpendicular to optical axis, and be in the image planes of optical system to be measured (3), adjust the displacement platform (5) of the first spatial light modulator (4), make the surface of the first spatial light modulator (4) perpendicular to optical axis and and distance between second space photomodulator (6) be d,
3) optical system wavefront aberration is measured:
1. x direction shear interference is measured:
Controlled by computing machine (9), make the first spatial light modulator (4) for y direction grating, namely in the y-direction, screen periods is set to described p to grating lines (401,402); Controlled by computing machine (9), second space photomodulator (6) is made to be Dual-window mask in the x-direction, namely the line of centres of two windows (601,602) is parallel to x-axis, distance between two windows (601,602) center is described Δ, and makes optical axis be in the center of two windows (601, the 602) line of centres; Open light source (1), detect interference light intensity signal I by photodetector (8) x1, this I x1import computing machine (9) into preserve; Computing machine (9) controls the first spatial light modulator grating (4), and make it along the translation of+x or-x direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector (8) x2, and by I x2import computing machine (9) into preserve; Repeat n time altogether, n is the phase shift step number of phase shift algorithm, and n width interference light intensity signal I preserved by final computing machine (9) x1, I x2..., I xn; By phase shift algorithm, by computing machine (9) by interference light intensity signal I x1, I x2..., I xn,calculate, obtain the difference wavefront Δ W in x direction x;
2. y direction shear interference is measured:
Controlled by computing machine (9), the first spatial light modulator (4) is set to x direction grating, and namely in the x-direction, screen periods is set to p to grating lines (411,412); Controlled by computing machine (9), second space photomodulator (6) is set to Dual-window mask in the y-direction, namely two windows (611, the 612) line of centres is parallel to y-axis, distance between two windows (611,612) center is set to Δ, and makes optical axis be in the center of two windows (611,612) line; Interference light intensity signal I is detected by photodetector (8) y1, and by I y1import computing machine (9) into preserve; Computing machine (9) controls the first spatial light modulator grating (4), and make it along the translation of+y or-y direction, translational movement is described Δ p, detects interference light intensity signal I by photodetector (8) y2, and by I y2import computing machine (9) into preserve; Repeat n time, n is the phase shift step number of phase shift algorithm, by computing machine (9) by phase shift algorithm, calculates interference signal I y1, I y2..., I yn, obtain the difference wavefront Δ W in y direction y;
3. wavefront reconstruction:
By described x direction difference wavefront Δ W xwith the difference wavefront Δ W in y direction y, reconstruct wavefront W to be measured by wavefront reconstruction algorithm, systematic error eliminated to wavefront W to be measured, obtains the wave aberration of optical system to be measured.
4. optical system wavefront aberration measuring method according to claim 3, is characterized in that described wavefront reconstruction algorithm can be type method or field method.
CN201510216017.5A 2015-04-30 2015-04-30 Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method Pending CN104807548A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
CN201510216017.5A CN104807548A (en) 2015-04-30 2015-04-30 Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method
PCT/CN2015/080419 WO2016173079A1 (en) 2015-04-30 2015-05-29 Digital phase shift lateral shearing interferometer and optical system wave aberration measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510216017.5A CN104807548A (en) 2015-04-30 2015-04-30 Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method

Publications (1)

Publication Number Publication Date
CN104807548A true CN104807548A (en) 2015-07-29

Family

ID=53692577

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510216017.5A Pending CN104807548A (en) 2015-04-30 2015-04-30 Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method

Country Status (2)

Country Link
CN (1) CN104807548A (en)
WO (1) WO2016173079A1 (en)

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259738A (en) * 2015-11-09 2016-01-20 中国科学院上海光学精密机械研究所 Parallel detection device for multiple field point wave aberrations of lithographic projection objective lens and detection method
CN105699057A (en) * 2016-03-01 2016-06-22 中国科学院上海光学精密机械研究所 Wave aberration detection system and method through taking spatial light modulator as a detection marker
CN106644107A (en) * 2016-12-22 2017-05-10 中国科学院光电研究院 Device and method for measuring spatial coherence length of laser beams
CN106767391A (en) * 2016-12-23 2017-05-31 浙江大学 The sensitivity intensifier and method of four wavefront lateral shearing interference Wavefront sensors
CN107036789A (en) * 2017-03-16 2017-08-11 中国科学院上海光学精密机械研究所 Point diffraction wave aberration detection interferometer and its detection method
CN108431694A (en) * 2015-12-22 2018-08-21 卡尔蔡司Smt有限责任公司 The apparatus and method of wavefront analysis
CN109014499A (en) * 2018-09-25 2018-12-18 北京航空航天大学 A kind of method and apparatus measuring WELDING ARC SPECTRUM spatial information (si)
CN109470236A (en) * 2018-11-26 2019-03-15 中国科学院长春光学精密机械与物理研究所 A kind of star sensor
CN110736543A (en) * 2019-10-08 2020-01-31 中国科学院上海光学精密机械研究所 Shearing amount calibration device and method for grating shearing interference wavefront sensor
CN113624451A (en) * 2021-07-08 2021-11-09 中国电子科技集团公司第十一研究所 Poehan prism optical axis consistency detection assembly and method
CN114235023A (en) * 2021-11-18 2022-03-25 北京卫星制造厂有限公司 Phase shifter on-line calibration method and device
CN114337839A (en) * 2021-12-30 2022-04-12 苏州六幺四信息科技有限责任公司 Universal photoelectric component analysis method
CN114689281A (en) * 2022-02-28 2022-07-01 歌尔光学科技有限公司 Method for detecting pupil drift of optical module

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3652512B1 (en) 2017-07-14 2021-09-01 Wavesense Engineering GmbH Optical apparatus
CN109522573B (en) * 2017-09-20 2023-03-21 中国科学院长春光学精密机械与物理研究所 Simulation method of active optical system of optical remote sensing camera
JP7300171B2 (en) * 2019-10-07 2023-06-29 国立研究開発法人情報通信研究機構 INTERFERENCE LIGHT GENERATOR AND INTERFERENCE IMAGING DEVICE

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10260985A1 (en) * 2002-12-18 2004-05-13 Carl Zeiss Smt Ag Shearing interferometry system for measurement of a wave front for use in measuring an optical imaging system in order to quantify its quality, said system having filters to suppress unwanted higher diffraction orders
CN101451890A (en) * 2008-12-18 2009-06-10 南京大学 Three light wave transversal shearing interference apparatus and method for extracting differential phase
CN102866001A (en) * 2012-09-13 2013-01-09 中国科学院上海光学精密机械研究所 Method for measuring aberration of imaging system based on lateral shearing interference structure
CN103256991A (en) * 2013-05-08 2013-08-21 中国科学院上海光学精密机械研究所 Spatial phase shift lateral shearing interferometer

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10260985A1 (en) * 2002-12-18 2004-05-13 Carl Zeiss Smt Ag Shearing interferometry system for measurement of a wave front for use in measuring an optical imaging system in order to quantify its quality, said system having filters to suppress unwanted higher diffraction orders
CN101451890A (en) * 2008-12-18 2009-06-10 南京大学 Three light wave transversal shearing interference apparatus and method for extracting differential phase
CN102866001A (en) * 2012-09-13 2013-01-09 中国科学院上海光学精密机械研究所 Method for measuring aberration of imaging system based on lateral shearing interference structure
CN103256991A (en) * 2013-05-08 2013-08-21 中国科学院上海光学精密机械研究所 Spatial phase shift lateral shearing interferometer

Cited By (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259738A (en) * 2015-11-09 2016-01-20 中国科学院上海光学精密机械研究所 Parallel detection device for multiple field point wave aberrations of lithographic projection objective lens and detection method
CN108431694B (en) * 2015-12-22 2020-10-09 卡尔蔡司Smt有限责任公司 Apparatus and method for wavefront analysis
CN108431694A (en) * 2015-12-22 2018-08-21 卡尔蔡司Smt有限责任公司 The apparatus and method of wavefront analysis
CN105699057B (en) * 2016-03-01 2018-03-20 中国科学院上海光学精密机械研究所 Utilization space optical modulator makees the wave aberration detection system and detection method of detection mark
CN105699057A (en) * 2016-03-01 2016-06-22 中国科学院上海光学精密机械研究所 Wave aberration detection system and method through taking spatial light modulator as a detection marker
CN106644107B (en) * 2016-12-22 2019-04-12 中国科学院光电研究院 Laser beam space coherence length measuring device and its measurement method
CN106644107A (en) * 2016-12-22 2017-05-10 中国科学院光电研究院 Device and method for measuring spatial coherence length of laser beams
CN106767391A (en) * 2016-12-23 2017-05-31 浙江大学 The sensitivity intensifier and method of four wavefront lateral shearing interference Wavefront sensors
CN106767391B (en) * 2016-12-23 2019-06-14 浙江大学 The sensitivity enhancement device and method of four wavefront lateral shearing interference Wavefront sensors
CN107036789B (en) * 2017-03-16 2019-02-26 中国科学院上海光学精密机械研究所 Point diffraction wave aberration detection interferometer and its detection method
CN107036789A (en) * 2017-03-16 2017-08-11 中国科学院上海光学精密机械研究所 Point diffraction wave aberration detection interferometer and its detection method
CN109014499A (en) * 2018-09-25 2018-12-18 北京航空航天大学 A kind of method and apparatus measuring WELDING ARC SPECTRUM spatial information (si)
CN109470236A (en) * 2018-11-26 2019-03-15 中国科学院长春光学精密机械与物理研究所 A kind of star sensor
CN110736543A (en) * 2019-10-08 2020-01-31 中国科学院上海光学精密机械研究所 Shearing amount calibration device and method for grating shearing interference wavefront sensor
CN110736543B (en) * 2019-10-08 2021-11-02 中国科学院上海光学精密机械研究所 Shearing amount calibration device and method for grating shearing interference wavefront sensor
CN113624451A (en) * 2021-07-08 2021-11-09 中国电子科技集团公司第十一研究所 Poehan prism optical axis consistency detection assembly and method
CN113624451B (en) * 2021-07-08 2023-10-24 中国电子科技集团公司第十一研究所 Buchner prism optical axis consistency detection assembly and method
CN114235023A (en) * 2021-11-18 2022-03-25 北京卫星制造厂有限公司 Phase shifter on-line calibration method and device
CN114235023B (en) * 2021-11-18 2024-05-03 北京卫星制造厂有限公司 Online calibration method and device for phase shifter
CN114337839A (en) * 2021-12-30 2022-04-12 苏州六幺四信息科技有限责任公司 Universal photoelectric component analysis method
CN114689281A (en) * 2022-02-28 2022-07-01 歌尔光学科技有限公司 Method for detecting pupil drift of optical module

Also Published As

Publication number Publication date
WO2016173079A1 (en) 2016-11-03

Similar Documents

Publication Publication Date Title
CN104807548A (en) Digital phase-shifting lateral shearing interferometer and optical system wave aberration measurement method
Shimizu et al. An insight into optical metrology in manufacturing
CN102681365B (en) Projection objective lens wave aberration detection device and method
CN101236362B (en) Photo-etching machine projection objective wave aberration on-line detection method
Shimizu Laser interference lithography for fabrication of planar scale gratings for optical metrology
CN101655670A (en) On-line detection device with function of calibrating systematic error for wave aberration of projection objective of photoetching machine
CN105092056B (en) Digital phase-shifting technique point-diffraction interferometer and optical system wavefront aberration measuring method
CN104713494B (en) The dual wavelength tuning interference testing device and method of Fourier transformation phase shift calibration
CN101813894B (en) On-line detection device of wave aberration of projection lens of lithography machine with precision calibration function
TW201730622A (en) Objective lens system
CN102261985A (en) Optical system wave aberration calibration apparatus and calibration method of using apparatus to test error
CN102289152A (en) optical system wave aberration detection device
CN104165755A (en) Grating shear wave aberration detection interferometer and detection method thereof
CN102620680B (en) Detecting device and method for tri-plane absolute measurement of optical surface
CN104913730A (en) Spherical surface shape rotation and translation absolute detection method
CN102865810B (en) Orthogonal double-grating based detecting device for synchronous phase shift common-light path interference and detecting method therefor
CN103076724B (en) Projection objective wave aberration on-line detection device and method based on double-beam interference
CN204028565U (en) A kind of projection objective wave aberration on-line checkingi interferometer
CN105783780A (en) Free-form surface unconventional subaperture splicing interference detection device and method
CN110736543B (en) Shearing amount calibration device and method for grating shearing interference wavefront sensor
CN102163008B (en) Online detection method of wave aberration of projection objective of lithography machine for self-calibrating system error
Le et al. A single collimating lens based dual-beam exposure system for fabricating long-period grating
CN102269937B (en) Online detection device and method for wave aberration of projection objective of photoetching machine
Zhai et al. Pixel-based absolute surface metrology by three flat test with shifted and rotated maps
CN108254086B (en) Random optical fiber point diffraction measurement method

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
EXSB Decision made by sipo to initiate substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication
RJ01 Rejection of invention patent application after publication

Application publication date: 20150729