CN203323738U - Isoplanatic angle measurement system based on tricyclic apodization mirror - Google Patents

Isoplanatic angle measurement system based on tricyclic apodization mirror Download PDF

Info

Publication number
CN203323738U
CN203323738U CN2013203938039U CN201320393803U CN203323738U CN 203323738 U CN203323738 U CN 203323738U CN 2013203938039 U CN2013203938039 U CN 2013203938039U CN 201320393803 U CN201320393803 U CN 201320393803U CN 203323738 U CN203323738 U CN 203323738U
Authority
CN
China
Prior art keywords
apodization
ring
mirrors
light
photomultiplier
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.)
Expired - Fee Related
Application number
CN2013203938039U
Other languages
Chinese (zh)
Inventor
强希文
吴敏
宗飞
胡月宏
强蔚
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.)
63655 TROOPS OF PEOPLE'S LIBERATION ARMY
Original Assignee
63655 TROOPS OF PEOPLE'S LIBERATION ARMY
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 63655 TROOPS OF PEOPLE'S LIBERATION ARMY filed Critical 63655 TROOPS OF PEOPLE'S LIBERATION ARMY
Priority to CN2013203938039U priority Critical patent/CN203323738U/en
Application granted granted Critical
Publication of CN203323738U publication Critical patent/CN203323738U/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Abstract

The utility model discloses an isoplanatic angle measurement system based on a tricyclic apodization mirror. The isoplanatic angle measurement system comprises the tricyclic apodization mirror. Optical waves modulated through the tricyclic apodization mirror enter an optical receiving system, the optical waves received through an optical imaging system are imaged and focused on the focal plane of a photomultiplier, and analog-digital conversion, collection and processing are carried out on current signals of the photomultiplier through a data collection and processing system. According to the isoplanatic angle measurement system, isoplanatic angles can be measured in all weather at all heights, the obtained isoplanatic angles are small in relative error, and compared with an existing isoplanatic angle measurement system in China, the isoplanatic angle measurement system is higher in measurement accuracy.

Description

A kind of dizzy angle measuring system such as grade based on three ring apodization mirrors
Technical field
The utility model belongs to the atmospheric optics technical field, relates to a kind of dizzy angle measuring system such as grade based on three ring apodization mirrors.
Background technology
When light wave transmits in atmosphere, due to the impact of atmospheric turbulence, the corrugated of light wave meeting distorted, intensity can produce fluctuating.Transmission for the light wave that comprises laser in real atmosphere, atmospheric turbulence causes the random deviation of beam Propagation direction, the expansion of light beam and the random fluctuation of intensity, thereby affects the application of the optical engineering such as laser.
For the ground astronomical optics, observe, when utilizing bigbore optics receiving telescope to carry out imaging to the observed object in space, send the light wave corrugated and produce distortion because atmospheric turbulence causes the spatial observation target, thereby cause the decrease resolution of optical telescope, affect observation effect.Generally speaking, when there is no the affecting of atmospheric turbulence, the resolution of the optical telescope that bore is D is 1.22 λ/D, and wherein λ is that the received light wave-wave is long; And, for actual conditions, always have the impact of atmospheric turbulence, now, the resolution of optical telescope can be reduced to 1.22 λ/r 0, r wherein 0For describing the parameter-atmospheric coherence length of whole atmosphere turbulence characteristics.The optical telescope aperture of observing for astronomical optics at present is roughly all more than 1m, and the numerical value of whole atmosphere coherent length is generally the scope of several centimetres to ten several centimetres, but, impact due to atmospheric turbulence, in the situation that do not have adaptive optics to proofread and correct, the telescope of the telescopical resolution of heavy caliber and tens of centimetres of bores is suitable.So atmospheric turbulence has comparatively serious restriction to bigbore optical telescope imaging resolution.
In order to improve the transmission performance of the light wave such as laser in atmosphere, to improve the telescopical resolution of heavy caliber, can utilize adaptive optics to proofread and correct the corrugated that atmospheric turbulence is caused and differ and is proofreaied and correct.And the adaptive optics timing, if the beacon light wave is inconsistent with the transmission direction of proofreading and correct light wave, for example, while having certain angle, the corrugated due to the beacon light wave differs the turbulence characteristics that can not represent fully on needs correction light path, so, utilize adaptive optics to carry out timing and can have certain corrugated residual error, and the corrugated residual error caused thus is relevant to the angle of the transmission direction of beacon light wave and correction light wave.
Mean etc. dizzy angle the maximum angle that corrugated is relevant, when beacon light wave and the angle of proofreading and correct the light wave transmissions direction such as are greater than at the dizzy angle, the turbulent characteristics that corrugated of beacon light wave differs on the light path of proofreading and correct with needs is fully uncorrelated, now, utilize adaptive optics effectively to be proofreaied and correct the impact of atmospheric turbulence.So waiting dizzy angle is one of important parameter atmospheric turbulence effect carried out the required consideration of adaptive optics timing.
If the atmospheric turbulence intensity along z place on light path is C n 2(z), wait dizzy angle θ 0For
Wherein k=2 π/λ is the light wave wave number, and λ is optical wavelength;
Figure BDA00003457973800022
For zenith angle.As can be seen from the above equation, wait dizzy angle θ 0For atmospheric turbulence intensity C n 2(z) weighting function, wherein weight function is z 5/3.And the starlight intensity normalization fluctuating variances sigma of utilizing telescope to receive s 2For
Figure BDA00003457973800023
Wherein A=2 π ∫ ρ P (ρ) d ρ is the annulus glazed area.By above two formula, can be found out, if can make weighting function W (z) in formula (2)=cz 5/3, can utilize measured starlight intensity fluctuation variances sigma s 2Inverting such as provides at the dizzy angle.
Be mainly used in the measurement at the dizzy angles such as atmospheric optical parameters etc. dizzy angle measuring instrument, and one of its crucial measuring element is the apodization mirror.From the end of the seventies in last century, after Loos and Hogge propose the concept of apodization mirror, Walters has designed single-orifice type apodization mirror in nineteen eighty-three, and in 1985, that it is perfect, has designed the apodization mirror of twin nuclei, the measuring accuracy at dizzy angle such as has improved.Within 1988, USAF has successfully designed the apodization mirror of tricyclic structure in Lincoln testing laboratory, and its measurement result can reach very high precision under weak turbulent-flow conditions.The domestic unit that carries out this area research work mainly comprises Chinese Academy of Sciences's Nation Astronomical Observatory and Anhui ray machine institute, its technical merit roughly is equivalent to U.S. 1980s level, still use single aperture apodization mirror, in the comparatively elementary stage, measuring accuracy is lower, the needs of adaptive optics compensation effect assessment in the time of can not meeting astronomical optics site selection and light wave fully and transmit in actual turbulent atmosphere.
The utility model content
The problem that the utility model solves is to provide a kind of dizzy angle measuring system such as grade based on three ring apodization mirrors, this system is by measuring the starlight intensity fluctuation after propagation in atmosphere, can be good at simulating the aperture filter function, obtain the dizzy angle such as grade along measuring route, realize the high-acruracy survey at the dizzy angle of equity.
The utility model is to be achieved through the following technical solutions:
A kind of dizzy angle measuring system such as grade based on three ring apodization mirrors, comprise three ring apodization mirrors, light wave through three ring apodization mirror modulation is incident to optical receiving system, by optical imaging system by received light wave imaging and focusing on the focal plane of photomultiplier, data Collection & Processing System carries out analog to digital conversion, acquisition and processing to the current signal of photomultiplier;
Described optical receiving system comprises astronomical telescope and collimation lens, after the light wave incident astronomical telescope of three ring apodization mirror modulation, then is emitted to optical imaging system by collimation lens;
Described optical imaging system is provided with attenuator, optical filter, spectroscope and imaging len on light path;
Described photomultiplier is driven by supporting high-voltage power supply;
Described data Collection & Processing System comprises A/D converter, data collecting card and calculation processing unit, photomultiplier amplifies signal output electrical signals, and A/D converter is that digital signal sends to calculation processing unit through data collecting card by analog signal conversion.
Further, also comprise image monitoring system, the spectroscope in optical imaging system is divided into two parts by light beam, and a part is incident on photomultiplier, and another part is transmitted to image monitoring system;
Described image monitoring system comprises CCD camera and display, after optical imaging system emission light beam, images on the CCD camera, and shows on display.
Further, also comprise control system, control system connects respectively astronomical telescope, CCD camera and data Collection & Processing System, trace routine by astronomical telescope is controlled the open-loop tracking of astronomical telescope to Celestial Objects, utilizes the image information of CCD camera to communicate by letter with astronomical telescope and realizes the closed loop tracking; Control system also returns to data Collection & Processing System by telescopical zenith angle real time data.
In described optical imaging system, attenuator is regulated the light intensity of incident light, prevents that photomultiplier is saturated, and optical filter improves system signal noise ratio; And spectroscope is divided into two parts by light beam, a part is incident on photomultiplier, and another part is imaged on the CCD camera, is convenient to system light path and regulates and astronomical telescope is followed the tracks of to control.
Described attenuator is narrow band pass filter, the plated film attenuator that described attenuator is wiping out background light.
Described astronomical telescope returns to data Collection & Processing System the zenith angle φ that fixed star light source position becomes with the measurement place in real time z.
Described three ring apodization mirrors, be comprised of concentric, light tight annulus alternative arrangement and printing opacity annulus, and the printing opacity annulus is followed successively by interior ring, adapter ring and outer shroud from inside to outside, wherein in the ring least radius be 37.389mm, maximum radius is 43.840mm; The adapter ring least radius is 62.890mm, and maximum radius is 69.240mm; The outer shroud least radius is 81.940mm, and maximum radius is 101.600mm.
The transmitance of described light tight annulus is not more than 1%, and the transmitance of printing opacity annulus is not less than 99.0%.
Described collimation lens and astronomical telescope are confocal, and the direction of focused beam is adjusted, and make its normal incidence optical imaging system.
Compared with prior art, the utlity model has following useful technique effect:
The dizzy angle measuring system such as grade based on three ring apodization mirrors that the utility model provides, the apodization mirror of employing tricyclic structure, can obtain higher measuring accuracy; Utilize long wave pass filter to coordinate the dizzy angles such as photomultiplier measurement, can realize daytime measurement; Therefore the utility model can be realized the dizzy angles such as daytime measurement at all height, and the dizzy angle such as gained relative error is less, and the measuring accuracy of comparing with dizzy angle measuring system such as domestic existing grade is higher.
The dizzy angle measuring system such as grade based on three ring apodization mirrors that the utility model provides, with respect to single aperture apodization mirror, can well simulate aperture filter function W (z) ≡ cz at all height 5/3, the dizzy angle such as gained relative error is obviously less, can realize the high-acruracy survey at the dizzy angle of equity, and maximum relative error is no more than 3%.
The accompanying drawing explanation
The dizzy angle measuring system principle schematic such as Fig. 1 is;
Fig. 2 such as is at the dizzy angle measuring system composition frame chart;
Fig. 3 such as is at the dizzy angle measuring system overall layout chart;
Fig. 4 such as is at the overall index path of dizzy angle measuring system;
The structural representation that Fig. 5 is three ring apodization mirrors; Wherein, 1 is outer shroud, and 2 is adapter ring, and 3 is interior ring;
Fig. 6 is two kinds of apodization mirror aperture filter functions and " z 5/3" power weighting function consistance comparison chart;
Fig. 7 is the two kinds of analog weighted function relative error of apodization mirror comparison charts;
Fig. 8 is that the theoretical computational data of three ring apodization mirrors and matched curve are compared;
Fig. 9 is that three ring apodization mirror relative errors are with the height change curve;
The measurement instruction flow chart that Figure 10 is data Collection & Processing System;
Figure 11 the dizzy angle relative error comparison chart such as is surveyed by the dizzy angle measuring system such as grade of three ring apodization mirrors.
Embodiment
Below in conjunction with specific embodiment, the utility model is described in further detail, described is to explanation of the present utility model rather than restriction.
Light wave is after propagation in atmosphere, and atmospheric turbulence can cause the random fluctuation of light wave intensity.For the starlight light wave after the apodization mirror through particular design transmission, its intensity fluctuation with etc. dizzy angle there is certain relation, so, by measuring the fluctuating of starlight intensity, can provide dizzy angle such as needed grade.
Referring to Fig. 1, wait dizzy angle measuring system principle to be: starlight, after the turbulent atmosphere transmission, by the modulation of apodization mirror, focuses to photodetector.Its light intensity fluctuation with etc. dizzy angle definite relation is arranged, by measuring the intensity fluctuation of starlight, the dizzy angle such as can inverting provide.
Referring to Fig. 2, Fig. 3, Fig. 4, the dizzy angle measuring system such as grade based on three ring apodization mirrors that the utility model provides, comprise three ring apodization mirrors, light wave through three ring apodization mirror modulation is incident to optical receiving system, by optical imaging system by received light wave imaging and focusing on the focal plane of photomultiplier, data Collection & Processing System carries out analog to digital conversion, acquisition and processing to the current signal of photomultiplier;
Described optical receiving system comprises astronomical telescope and collimation lens, after the light wave incident astronomical telescope of three ring apodization mirror modulation, then is emitted to optical imaging system by collimation lens;
Described optical imaging system is provided with attenuator, optical filter, spectroscope and imaging len on light path;
Described photomultiplier is driven by supporting high-voltage power supply;
Described data Collection & Processing System comprises A/D converter, data collecting card and calculation processing unit, photomultiplier amplifies signal output electrical signals, A/D converter is that digital signal sends to calculation processing unit through data collecting card by analog signal conversion, calculation processing unit reads digital signal, treatedly the dizzy angle such as obtains.
Further, also comprise image monitoring system, the spectroscope in optical imaging system is divided into two parts by light beam, and a part is incident on photomultiplier, and another part is transmitted to image monitoring system;
Described image monitoring system comprises CCD camera and display, after optical imaging system emission light beam, images on the CCD camera, and shows on display.
Further, also comprise control system, control system connects respectively astronomical telescope, CCD camera and data Collection & Processing System, trace routine by astronomical telescope is controlled the open-loop tracking of astronomical telescope to Celestial Objects, utilizes the image information of CCD camera to communicate by letter with astronomical telescope and realizes the closed loop tracking; Control system also returns to data Collection & Processing System by telescopical zenith angle real time data, the dizzy angle Inversion Calculation such as supplies to analyze reference.
Be specifically described and introduce below in conjunction with each system.
1, three ring apodization mirrors
Etc. dizzy angle, be the weighted integral of air index textural constant, " 5/3 " power function that wherein weighting function is distance.In order to utilize hardware to realize " 5/3 " the power weighting function to height, need designed apodization mirror can simulate well W (z) ≡ cz 5/3Requirement.At present comparatively generally mainly containing three kinds of apodization mirrors, is respectively single hole apodization mirror, and dicyclo apodization mirror and three ring apodization mirrors also are not quite similar to the capability of fitting of " 5/3 " power of height.Wherein, the capability of fitting of the apodization mirror of tricyclic structure is much better than the apodization mirror of single hole structure and twin nuclei, and its fitting coefficient c value can reflect the weighting function of " 5/3 " power preferably at the height of 300m to 30000m.
Referring to Fig. 5, the three ring apodization mirrors that the utility model adopts, be comprised of concentric, light tight annulus alternative arrangement and printing opacity annulus, and the printing opacity annulus is followed successively by interior ring, adapter ring and outer shroud from inside to outside, wherein, the ring least radius is 37.389mm, and maximum radius is 43.840mm; The adapter ring least radius is 62.890mm, and maximum radius is 69.240mm; The outer shroud least radius is 81.940mm, and maximum radius is 101.600mm; The transmitance of described light tight annulus is not more than 1%, and the transmitance of printing opacity annulus is not less than 99.0%; This three rings apodization mirror simulation aperture filter function W (z) ≡ cz 5/3The time, its aperture filter function coefficient c=8.847e-17m 4.
Aperture filter function and z that Fig. 6 is three ring apodization mirrors and single hole apodization mirror 5/3Ratio is with the variation relation of height.Can find out, under wavelength and the certain condition of zenith angle, the aperture filter function of single aperture apodization mirror, at all height, can not be simulated shape as " z well 5/3" weighting function, be inferior to three ring apodization mirrors.As optical wavelength λ=0.5 μ m, zenith angle is 0 °, interior yardstick l 0=5mm, external measurement L 0During=10m, single aperture apodization mirror is compared with the ring of three in the utility model apodization mirror, aperture filter function and z 5/3Consistance poor, the dizzy angle such as gained relative error is larger.
Atmospheric turbulence profile model has multiple, and wherein the H-V model is a kind of atmospheric turbulence profile model commonly used.Utilize air index textural constant profile model (H-V model) commonly used to bring (2) formula into, the relative error such as dizzy angle such as grade that calculating provides two kinds of apodization mirror gained as shown in Figure 7, obviously can find out, the relative error of three ring apodization mirrors is less than the relative error of single hole apodization mirror.
Concrete when wavelength X=0.5 μ m, wait the expression formula of dizzy angle and light intensity fluctuation variance to be:
θ 0 ( φ z , λ ) = c ′ [ σ s 2 ( φ z ) ] - 3 / 5 - - - ( 7 )
Calculate the curve of W (z) as shown in Figure 8, the number percent curve of both differences as shown in Figure 9.
As can be seen here, use this apodization mirror can realize the modulation to light signal, meet etc. in dizzy angular measurement principle the requirement to light distribution.Its method for making can adopt the mode to eyeglass plating circular membrane to realize.
Method one:
The preparation method of three ring apodization mirrors, is characterized in that, comprises following operation:
On the circular substrate that be not less than 99.0% in transmitance, radius is 101.600mm, take its center of circle as benchmark, at first pasting radius is the light tight round metal of 37.389mm, and then the stickup least radius is the light tight metal ring that 43.840mm, maximum radius are 62.890mm; Finally pasting least radius is the light tight metal ring that 69.240mm, maximum radius are 81.940mm again.
Wherein, substrate is to utilize the window materials such as K9 glass, plexiglas or quartz to make the transparent substrate that radius is 101.600mm.
Method two:
The preparation method of three ring apodization mirrors comprises following operation:
1) circular below making on substrate: as to take central point as the center of circle, portray respectively the first circle, the second circle, the 3rd circle, the 4th circle, the 5th circular and the 6th circle that radius is respectively 37.389mm, 43.840mm, 62.890mm, 69.240mm, 81.940mm and 101.600mm;
Annulus between annulus, the 4th circle and the 5th circle of 2) usining between the first circle, the second circle and the 3rd circle is as lightproof part;
Annulus between annulus, the 5th circle and the 6th circle between annulus, the 3rd circle and the 4th circle of usining between the first circle and the second circle is as light transmission part;
Utilize mask plate that lightproof part is blocked, plate respectively transmitance on two surfaces, light transmission part of substrate and be not less than 99.0% anti-reflection film; Then with mask plate, light transmission part is blocked, on lightproof part two surfaces of substrate, plate respectively and increase reverse, make its transmitance be not more than 1%.
2, optical receiving system
This system mainly is comprised of astronomical telescope and collimation lens.Wherein telescope intends selecting the CGEM800GPS XLT type astronomical telescope of Xing Telang company; Collimation lens and astronomical telescope system are confocal, its role is to the direction of focused beam is adjusted, and make its normal incidence on optical filter, improve the filter effect of optical filter.Its mirror holder part need to be complementary with astronomical telescope, can entrust relevant unit to carry out precision optical machinery processing.
3, optical imaging system
This system mainly is comprised of attenuator, optical filter, spectroscope and imaging len.Wherein the light intensity of attenuator for regulating incident light, prevent that photomultiplier is saturated, and optical filter is for improving system signal noise ratio.Spectroscope is divided into two parts by light beam, and a part is incident on photomultiplier, and it is upper that another part is imaged on CCD, is convenient to the system light path adjusting and telescope is carried out to closed loop and follow the tracks of control.
4, photomultiplier
Mainly by photomultiplier and supporting high-voltage power supply, formed, specifically can adopt the 9128B of ET company.
5, image monitoring system
Mainly by CCD camera and display, formed.Its Main Function be while regulating for system state with reference to so that operating personnel grasp the telescopic system state, understand the system imaging quality, differentiate and whether can start to measure.
6, data Collection & Processing System
Data Collection & Processing System mainly is comprised of A/D converter, data collecting card and computing software.Photomultiplier amplifies low light level signal, and output electrical signals, and A/D converter is that digital signal is stored in calculator memory through data collecting card by analog signal conversion, and software for calculation reads the signal data in internal memory, processes the value at dizzy angles such as obtaining.
Referring to Figure 10, data Collection & Processing System mainly comprises: a), real-time data acquisition; B), signal de-noising; C), light intensity is calculated; D), the light intensity fluctuation variance is calculated; The dizzy angle inverting such as e); F), data Storage & Display.
7, control system
Control system connects astronomical telescope, CCD camera and data acquisition processing system.Utilize the telescopic system database to realize the open-loop tracking to Celestial Objects (fixed star) by controlling software, use the image information of CCD camera to realize the closed loop tracking.Transmitting software the dizzy angle computing software such as returns to by telescopical zenith angle (elevation angle) real time data, for the computational analysis reference.
Below provide the method at the dizzy angles such as dizzy angle measuring system measurement such as grade based on three ring apodization mirrors, it is characterized in that, comprise following operation:
The light wave of the target celestial body transmitted through turbulent atmosphere, be incident to optical receiving system after the apodization mirror, by the optical imaging system imaging and focusing on the focal plane of photomultiplier, data Collection & Processing System carries out analog to digital conversion, acquisition and processing to the current signal of photomultiplier, and last inverting such as provides at the dizzy angular measurement result;
Wherein the penetrating light intensity distribution functions of three ring apodization mirrors are P (ρ), light transmission part P (ρ)=1, and lightproof part P (ρ)=0, ρ is the radial distance of annulus, and the total light intensity by the apodization mirror is denoted as S, and S is time variable; Atmospheric turbulence can cause the starlight intensity fluctuation after transmission, by its normalization, by formula (3), provides the light intensity fluctuation variance:
σ s 2 ( φ z , λ ) = 4 ( 2 π ) 4 0.033 sec 8 / 3 ( φ 2 ) k 2 A - 2 ∫ 0 ∞ C n 2 ( z ) W ( z ) dz - - - ( 3 )
A=2 π ∫ ρ P (ρ) d ρ wherein; K[=2 π/λ] be the light wave wave number, λ is optical wavelength; φ zFor zenith angle; Z is the telescopical distance of distance on astronomical telescope and target celestial body light path; C n 2(z) be the air index textural constant at distance z place; The representation of weighting function W (z) as shown in the formula:
W ( z ) = ∫ 0 ∞ | ∫ dρρ J 0 ( Lρ ) P ( Lρ ) | 2 L - 8 / 3 sin 2 [ L 2 z 2 k ] dL - - - ( 4 )
J in formula 0(x) be zeroth order Bessel function; The spatial frequency that K is amplitude fluctuation, K max=2 π/l 0, K min=2 π/L 0, l 0, L 0Be respectively yardstick and external measurement in atmospheric turbulence; The aperture function that P (ρ) is the apodization mirror, light transmission part P (ρ)=1 wherein, lightproof part P (ρ)=0, ρ is the radial distance (radius) of annulus;
Normalization light intensity fluctuation variance is zenith angle φ zWith the function of incident wavelength λ, its scope of application is that light intensity fluctuation meets weak fluctuation condition, when normalization light intensity fluctuation variances sigma s 2z, λ) during unsaturation, think etc. that dizzy angular measurement result is effective;
Dizzy angle such as grade along measuring route z is provided by formula (5):
θ 0 ( φ z , λ ) = 0.527 k - 6 / 5 [ ∫ 0 ∞ C n 2 ( z ) z 5 / 3 dz ] - 3 / 5 - - - ( 5 )
Can show etc. that in conjunction with equation (3) and equation (5) dizzy angle computing formula is:
θ 0 ( φ z , λ ) = 12.9 A - 6 / 5 c 3 / 5 [ σ s 2 ( φ z ) ] - 3 / 5 - - - ( 6 )
Wherein, the c value can be by W (z) ≡ cz 5/3Matching provides numerical solution.
And when normalization light intensity fluctuation variance, σ s 2(0) be calculated as follows:
σ s 2 ( 0 ) = variance mean 2 = 1 N Σ i = 1 N [ α X i ] 2 - [ 1 N Σ i = 1 N α X i ] 2 [ 1 N Σ i = 1 N α X i - b ] 2 - - - ( 8 )
Wherein, the gain coefficient that α is photomultiplier; The background value that b measures while being the gauge without light source signal, obtain by repeatedly measuring the method that the institute's fixed star of surveying bias light on every side averages;
And the zenith angle φ that target celestial body light source position becomes with the measurement place z, by gps data, from astronomical telescope, return in real time.
Wherein, the sample frequency of the dizzy angle measuring system such as grade of three ring apodization mirrors are f, according to etc. the index request of dizzy angle measuring system, sample size is N, and sampling time t=N/f can be set in software, i.e. every value through a dizzy angle such as grade of t Time Calculation.Also sample size N can be set, often adopt enough N data, just once calculate, obtain and export the dizzy angle value such as.In the situation that not frame losing of system acquisition, ft=N, if can not guarantee the not frame losing continuously of N frame data, can cause ft<N, therefore, enough in order to guarantee data volume, preferentially selects sample size N that the value at the dizzy angles such as calculating is set.
Referring to Figure 11, provided the variation contrast of the relative error of the dizzy angle measuring system measurement such as grade based on three ring apodization mirrors with height in figure.Can find out, the weighting function relative error of the dizzy angle measuring system such as grade of three ring apodization mirrors is at 0.5~20km distance range, and maximum relative error is no more than 3%, and the relative error of monocycle apodization mirror can reach 15%.The visible precision at the dizzy angles such as three ring apodization mirror measurements of utilizing is significantly improved.

Claims (9)

1. the dizzy angle measuring system such as grade based on three ring apodization mirrors, it is characterized in that, comprise three ring apodization mirrors, light wave through three ring apodization mirror modulation is incident to optical receiving system, by optical imaging system by received light wave imaging and focusing on the focal plane of photomultiplier, data Collection & Processing System carries out analog to digital conversion, acquisition and processing to the current signal of photomultiplier;
Described optical receiving system comprises astronomical telescope and collimation lens, after the light wave incident astronomical telescope of three ring apodization mirror modulation, then is emitted to optical imaging system by collimation lens;
Described optical imaging system is provided with attenuator, optical filter, spectroscope and imaging len on light path;
Described photomultiplier is driven by supporting high-voltage power supply;
Described data Collection & Processing System comprises A/D converter, data collecting card and calculation processing unit, photomultiplier amplifies signal output electrical signals, and A/D converter is that digital signal sends to calculation processing unit through data collecting card by analog signal conversion.
2. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 1, it is characterized in that, also comprise image monitoring system, the spectroscope in optical imaging system is divided into two parts by light beam, a part is incident on photomultiplier, and another part is transmitted to image monitoring system;
Described image monitoring system comprises CCD camera and display, after optical imaging system emission light beam, images on the CCD camera, and shows on display.
3. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 2, it is characterized in that, also comprise control system, control system connects respectively astronomical telescope, CCD camera and data Collection & Processing System, trace routine by astronomical telescope is controlled the open-loop tracking of astronomical telescope to Celestial Objects, utilizes the image information of CCD camera to communicate by letter with astronomical telescope and realizes the closed loop tracking; Control system also returns to data Collection & Processing System by telescopical zenith angle real time data.
4. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 2, is characterized in that, in described optical imaging system, attenuator is regulated the light intensity of incident light, prevents that photomultiplier is saturated, and optical filter improves system signal noise ratio; And spectroscope is divided into two parts by light beam, a part is incident on photomultiplier, and another part is imaged on the CCD camera, is convenient to system light path and regulates and astronomical telescope is followed the tracks of to control.
5. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 4, is characterized in that, described attenuator is narrow band pass filter, the plated film attenuator that described attenuator is wiping out background light.
6. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 1, is characterized in that, described astronomical telescope returns to data Collection & Processing System the zenith angle φ that fixed star light source position becomes with the measurement place in real time z.
7. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 1, it is characterized in that, described three ring apodization mirrors, by concentric, light tight annulus alternative arrangement and printing opacity annulus, formed, the printing opacity annulus is followed successively by interior ring, adapter ring and outer shroud from inside to outside, wherein, the ring least radius is 37.389mm, and maximum radius is 43.840mm; The adapter ring least radius is 62.890mm, and maximum radius is 69.240mm; The outer shroud least radius is 81.940mm, and maximum radius is 101.600mm.
8. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 7, is characterized in that, the transmitance of described light tight annulus is not more than 1%, and the transmitance of printing opacity annulus is not less than 99.0%.
9. the dizzy angle measuring system such as grade based on three ring apodization mirrors as claimed in claim 1, is characterized in that, described collimation lens and astronomical telescope are confocal, and the direction of focused beam is adjusted, and make its normal incidence optical imaging system.
CN2013203938039U 2013-07-03 2013-07-03 Isoplanatic angle measurement system based on tricyclic apodization mirror Expired - Fee Related CN203323738U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2013203938039U CN203323738U (en) 2013-07-03 2013-07-03 Isoplanatic angle measurement system based on tricyclic apodization mirror

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2013203938039U CN203323738U (en) 2013-07-03 2013-07-03 Isoplanatic angle measurement system based on tricyclic apodization mirror

Publications (1)

Publication Number Publication Date
CN203323738U true CN203323738U (en) 2013-12-04

Family

ID=49663078

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2013203938039U Expired - Fee Related CN203323738U (en) 2013-07-03 2013-07-03 Isoplanatic angle measurement system based on tricyclic apodization mirror

Country Status (1)

Country Link
CN (1) CN203323738U (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104236520A (en) * 2014-09-26 2014-12-24 中国科学院合肥物质科学研究院 Measuring method of inclined isoplanatic angle of whole layer of atmosphere turbulence
CN103487010B (en) * 2013-07-03 2016-01-06 中国人民解放军63655部队 A kind of dizzy angle measuring system such as grade based on three ring apodization mirrors and method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103487010B (en) * 2013-07-03 2016-01-06 中国人民解放军63655部队 A kind of dizzy angle measuring system such as grade based on three ring apodization mirrors and method
CN104236520A (en) * 2014-09-26 2014-12-24 中国科学院合肥物质科学研究院 Measuring method of inclined isoplanatic angle of whole layer of atmosphere turbulence
CN104236520B (en) * 2014-09-26 2016-09-21 中国科学院合肥物质科学研究院 A kind of measuring method at the dizzy angles such as whole atmosphere turbulent flow inclination

Similar Documents

Publication Publication Date Title
Zhou et al. Design of supercontinuum laser hyperspectral light detection and ranging (LiDAR)(SCLaHS LiDAR)
CN105137415B (en) The apparatus and method that laser range finder field of view of receiver is demarcated and parallelism of optical axis is measured
CN102944312B (en) Method for measuring partially coherent vortex light beam topological charge number
CN106371102B (en) Inverse Synthetic Aperture Laser Radar receiving system based on adaptive optics
CN103308187B (en) High frequency three dimensional Shack Hartmann wavefront measuring device and measuring method thereof
CN101814952B (en) Method for testing lightwave transmission characteristics in atmospheric channel
CN203216702U (en) Focal length measuring device for long focal length optical system
CN202522516U (en) Optical transmissivity test device
CN103487010B (en) A kind of dizzy angle measuring system such as grade based on three ring apodization mirrors and method
CN102879110B (en) Adaptive optical system based on modulation and modulation-free combined pyramid wave-front sensor
CN106483530A (en) Retrosynthesis aperture laser radar system based on reflective astronomical telescope
CN107727368B (en) Device and method for calibrating focal plane position of collimator
CN1963468A (en) Method and apparatus for real time measuring permeation ratio of whole atmosphere by fixed star
CN103278045A (en) Rocket azimuth precise aiming system and rocket azimuth precise aiming method
CN103048701B (en) Atmospheric optical parameter measurer for astronomical site survey
CN102901483A (en) Measurement method based on multi-sub-aperture imaging for atmospheric isoplanatic angle
CN203323738U (en) Isoplanatic angle measurement system based on tricyclic apodization mirror
CN107389560A (en) Multiband all -fiber high spectral resolution total atmospheric spectral transmittance simultaneous measuring apparatus and measuring method
CN103487861B (en) The method at a kind of dicyclo apodization mirror and preparation method thereof and the dizzy angles such as its measurement
CN104776825A (en) Limited distance isoplanatie angle real-time measurement apparatus and method thereof
CN105158171B (en) Crop nitrogen sensor spectrum calibration method
CN103063869B (en) Measuring device and measuring method of light propagation path transverse average wind speed and wind direction
CN203350474U (en) Dual annulus apodization lens
CN203350469U (en) Tri-ring apodization lens
CN104236520A (en) Measuring method of inclined isoplanatic angle of whole layer of atmosphere turbulence

Legal Events

Date Code Title Description
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: 20131204

Termination date: 20150703

EXPY Termination of patent right or utility model