CN1411285A - Calibration method of electric charge coupler response linearity - Google Patents

Calibration method of electric charge coupler response linearity Download PDF

Info

Publication number
CN1411285A
CN1411285A CN 00132097 CN00132097A CN1411285A CN 1411285 A CN1411285 A CN 1411285A CN 00132097 CN00132097 CN 00132097 CN 00132097 A CN00132097 A CN 00132097A CN 1411285 A CN1411285 A CN 1411285A
Authority
CN
China
Prior art keywords
coupled device
charge coupled
diffraction
measured
gray level
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.)
Granted
Application number
CN 00132097
Other languages
Chinese (zh)
Other versions
CN1200453C (en
Inventor
段海峰
杨泽平
王淑青
张雨东
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.)
Institute of Optics and Electronics of CAS
Original Assignee
Institute of Optics and Electronics 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 Institute of Optics and Electronics of CAS filed Critical Institute of Optics and Electronics of CAS
Priority to CN 00132097 priority Critical patent/CN1200453C/en
Publication of CN1411285A publication Critical patent/CN1411285A/en
Application granted granted Critical
Publication of CN1200453C publication Critical patent/CN1200453C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

This invention discloses a method for calibrating the response linearity of a charge coupled device which is to sample facula lattice of back focus plane of Fourier lens with charge coupled device by Fourier lens convergence using single colour plane illumination diffraction screen to get the output array value of the facula lattice and to analyse facula strength theory distribution value and output gray value sampled by charge coupled device computed from Fraumnhofer diffraction theory to realize the calibration for response linearity of the charge coupled device.

Description

A kind of scaling method of electric charge coupler response linearity
The present invention relates to a kind of scaling method of electric charge coupler response linearity, relate in particular to a kind of by measuring the method that charge coupled device input light intensity and output gray level value response curve carry out the electric charge coupler response linearity demarcation.
Charge coupled device is a kind of new electrooptical device, can utilize its this Characteristics Detection Be Controlled object usually according to its its input intensity variations of gray scale output change detection.But because charge coupler response non-linear, and the response difference between each picture dot of charge coupled device, need demarcate to electric charge coupler response linearity.The demarcation of electric charge coupler response linearity at present mainly contains damped method and divided beams method.
Damped method is to make light pass through one group of attenuator or different diaphragm of clear aperture that transmitance is different, realization is fixed than regulating to incident light, and make this group incident light enter charge coupled device, demarcate the response linearity of charge coupled device by the charge coupled device measured value that obtains therefrom.The defective of this method is and need repeatedly samples, so stated accuracy is subjected to intensity of light source fluctuating to influence bigger.
The divided beams method is to utilize the light-dividing principle of wedge, one side at wedge is plated the film that is all-trans, one side is plated spectro-film, a branch of directional light is after wedge repeatedly reflects, form the certain light beam of a series of beam intensity ratios, assemble through a fourier transform lens again, and make charge coupled device place fourier transform lens back focal plane place, once sampling can obtain the response of one group of light intensity, can demarcate the response linearity of charge coupled device thus.The defective of this method is that processing, the plated film to wedge have relatively high expectations, and light path is difficult for adjusting, and easily introducing bigger off-axis aberration influences optical quality on the focal plane, thereby influences stated accuracy.
The objective of the invention is to overcome the deficiency of existing method and a kind of method of demarcation electric charge coupler response linearity simple in structure is provided.
For finishing above-mentioned purpose, the inventive method comprises the following steps:
Making slit diffraction screen is selected the diffraction screen parameter, makes the target surface of the primary maximum width of diffraction and charge coupled device to be measured measure-alike;
After fourier transform lens placed diffraction screen, and charge coupled device to be measured is placed the back focal plane position of fourier transform lens;
Utilize a branch of monochromatic planar light irradiation diffraction screen, carry out the sampling of charge coupled device output gray level value to be measured, obtain diffraction pattern output gray level value;
Calculate spot intensity theoretical distribution value, and with the hot spot output gray level value of charge coupled device sampling to be measured relatively, realize demarcation to electric charge coupler response linearity to be measured.
Method of the present invention can also be finished through the following steps:
Described diffraction screen can be made as double slit (single seam, many seams, square hole or circular hole) diffraction screen;
The described sampling of carrying out charge coupled device output gray level value to be measured can obtain the hot spot output gray level value of (the stitching diffraction screen) of continuous (square hole, single seam, diffraction from circular aperture screen) or serial dot matrix more.
The present invention has following advantage with respect to existing method: utilize the light distribution of double slit (single seam, many seams, square hole or circular hole) diffraction accurately to provide with the Fraunhofer diffraction theory, obtain the theoretical value of its distribution.Conversion character according to Fraunhofer diffraction and fourier transform lens, utilize a branch of monochromatic planar light irradiation diffraction screen, measure its diffraction distribution value with tested charge coupled device,, obtain the non-linear deviation of tested charge coupled device by comparing and measuring the difference of value and theoretical value.Because it is simple in structure that this method adopts, so debugging is convenient to Project Realization easily.And, be beneficial to the uniformity of test charge coupled apparatus owing to utilize monochromatic planar light light source.In addition, owing to can obtain the certain sampled value of a series of light distribution relations, demarcate the influence that electric charge coupler response linearity has avoided light source to rise and fall thereby make by single exposure.Especially this method optics processing of not needing to have relatively high expectations is so cost is lower.
The present invention is further illustrated below in conjunction with drawings and Examples (selecting the two-slit diffraction screen).
Fig. 1 is the light channel structure figure that the method for the embodiment of the invention adopts.
Fig. 2 is the spot intensity theoretical distribution figure of the embodiment of the invention.
Fig. 3 is the hot spot dot chart of the embodiment of the invention.
The embodiment of the invention comprises the following steps: as shown in Figure 1, the embodiment of the invention is utilized a branch of monochromatic planar light irradiation two-slit diffraction screen 1, assemble to its back focal plane through fourier transform lens 2, charge coupled device to be determined 3 is placed the back focal plane position of fourier transform lens 2.Select following parameter: the focal distance f=1200mm of fourier transform lens 2, the target surface 3.2 * 2.4mm of charge coupled device 3 to be determined, the wavelength X of the monochromatic planar light of incident=1.064 μ m.
Half width according to the primary maximum of single slit diffraction is: Δx = λf a
Select the diffraction screen parameter: slit stitches wide a=0.4mm, makes the primary maximum of single slit diffraction be full of the target surface of charge coupled device 3.
Spacing according to two-beam interference the two poles of the earth large spot is: Δx = λf d
Select double slit apart from d=10mm, make d=ma (m=1,2,3 ... n), thereby on the target surface of the back focal plane of fourier transform lens 2 that is charge coupled device 3, obtain one group of (m) spacing by slit centre-to-centre spacing d determine, the certain hot spot dot matrix of strength relationship, as shown in Figure 3.
Carry out the sampling of charge coupled device 3 output gray level values, obtain the gray value of a series of hot spot dot matrix outputs.
According to the conversion character of double slit Fraunhofer diffraction and fourier transform lens, derive the light spot energy relation of charge coupled device 3 samplings:
Monochromatic plane wave vertical illumination diffraction screen, the COMPLEX AMPLITUDE of aperture plane is: E ( x 1 ) = rect ( x 1 - d / 2 a ) + rect ( x 1 + d / 2 a ) - - - - ( 1 )
Behind lens, the COMPLEX AMPLITUDE of the Fraunhofer diffraction style that forms in the focal plane can be obtained by Fourier transform: E ( x ) = F ( E ( x 1 ) ) n = x / λf = F ( rect ( x 1 - d / 2 a ) ) + F ( rect ( x 1 + d / 2 a ) ) - - - - ( 2 )
By the phase shift theorem of the upright conversion of Fu Ye, 2. formula can be written as: E ( x ) = exp ( - i 2 πu ( d / 2 ) ) F ( rect ( x 1 / a ) ) + exp ( - i 2 πu ( - d / 2 ) ) F ( rect ( x 1 / a ) ) = ( exp ( - iπud ) + exp ( iπud ) ) a sin c ( au ) = 2 a sin c ( ax λf ) cos ( πxd λf ) n = x / λf - - - - ( 3 ) Intensity distributions is: I ( x ) = | E ( x ) | 2 = I ( 0 ) sin c 2 ( ax λf ) cos 2 ( πxd λf ) - - - - ( 4 ) I in the formula (O) is the intensity distributions at diffraction pattern center;
4. formula shows that the intensity distributions of two-slit diffraction is by the single slit diffraction factor and the coefficient result of the two-beam interference factor.Figure 2 shows that the intensity distributions of hot spot.
4. calculate the theoretical distribution value of hot spot dot matrix according to formula.
Analyze the theoretical distribution value of hot spot dot matrix and the hot spot dot matrix output gray level value of charge coupled device 3 samplings, realize demarcation charge coupled device 3 response linearities.

Claims (2)

1, a kind of scaling method of electric charge coupler response linearity is characterized in that comprising the following steps:
Make slit diffraction screen (1), select the diffraction screen parameter, make the target surface of the primary maximum width of diffraction and charge coupled device to be measured (3) measure-alike;
After fourier transform lens (2) placed diffraction screen, and charge coupled device to be measured (3) is placed the back focal plane position of fourier transform lens (2);
Utilize a branch of monochromatic planar light irradiation diffraction screen (1), carry out the sampling of charge coupled device to be measured (3) output gray level value, obtain diffraction pattern output gray level value;
Calculate spot intensity theoretical distribution value, and with the hot spot output gray level value of charge coupled device to be measured (3) sampling relatively, realize demarcation to charge coupled device to be measured (3) response linearity.
2, the scaling method of electric charge coupler response linearity according to claim 1 is characterized in that:
Described diffraction screen (1) can be made double slit (single seam, many seams, square hole or circular hole) diffraction screen;
The described sampling of carrying out charge coupled device to be measured (3) output gray level value, can obtain a series of dot matrix hot spot output gray level value.
CN 00132097 2000-12-18 2000-12-18 Calibration method of electric charge coupler response linearity Expired - Fee Related CN1200453C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 00132097 CN1200453C (en) 2000-12-18 2000-12-18 Calibration method of electric charge coupler response linearity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 00132097 CN1200453C (en) 2000-12-18 2000-12-18 Calibration method of electric charge coupler response linearity

Publications (2)

Publication Number Publication Date
CN1411285A true CN1411285A (en) 2003-04-16
CN1200453C CN1200453C (en) 2005-05-04

Family

ID=4594967

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 00132097 Expired - Fee Related CN1200453C (en) 2000-12-18 2000-12-18 Calibration method of electric charge coupler response linearity

Country Status (1)

Country Link
CN (1) CN1200453C (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104980734A (en) * 2015-07-20 2015-10-14 福州鑫图光电有限公司 Device for detecting image sensor performance and use method thereof
CN105890529A (en) * 2015-01-26 2016-08-24 北京师范大学 Method for measuring filament diameter and device
CN108151877A (en) * 2017-12-14 2018-06-12 西京学院 A kind of micro-hole spectrometer and spectrum reconstruction method

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105890529A (en) * 2015-01-26 2016-08-24 北京师范大学 Method for measuring filament diameter and device
CN105890529B (en) * 2015-01-26 2018-08-17 北京师范大学 The method for measuring filament diameter
CN104980734A (en) * 2015-07-20 2015-10-14 福州鑫图光电有限公司 Device for detecting image sensor performance and use method thereof
CN104980734B (en) * 2015-07-20 2017-11-28 福州鑫图光电有限公司 A kind of application method of the device of detection image sensor performance
CN108151877A (en) * 2017-12-14 2018-06-12 西京学院 A kind of micro-hole spectrometer and spectrum reconstruction method

Also Published As

Publication number Publication date
CN1200453C (en) 2005-05-04

Similar Documents

Publication Publication Date Title
DE112016007086T5 (en) SCANNING-TYPE-LASER-INDUCED SPECTRAL ANALYSIS AND DETECTION SYSTEM
CN102538969B (en) High resolution spectrometer and optical calibrating method thereof
CN109186945A (en) The measuring device and method of heavy-caliber optical grating diffraction efficiency spectrum and its uniformity
CN108801972A (en) A kind of Fourier spectrometer based on Digital Micromirror Device
CN107063456B (en) Time resolution diffraction efficiency of grating spectral measurement device in situ and method
CN109387531A (en) A kind of diffraction delustring rocking curve image measuring device and method
CN106950035A (en) The device and method of liquid crystal grating interferometry phase modulation of spatial light modulators characteristic
CN106124166A (en) The measurement apparatus of a kind of heavy-caliber optical grating diffraction efficiency and measuring method
CN100492180C (en) Projection objective detecting method
DE19911671A1 (en) Narrow band module inspection apparatus e.g. for excimer laser
CN105928688A (en) Measurement device and method of grating diffraction efficiency spectrum based on single time exposure mode
CN105572076B (en) THz wave spectrometry device and its measurement method based on scattering effect
CN101261224A (en) Optical non-linear method for measuring material based on 4f phase coherent imaging system
CN100535760C (en) On-line testing apparatus of projection objective
CN106768890A (en) For the gray scale cosine distribution optical target analogue means of modulation transfer function detection
CN100492179C (en) Interferometer
US6683691B2 (en) Method and arrangement for spatially resolved and time-resolved interferometric characterization of ultrashort laser pulses
DE10220872A1 (en) Display diffuse illumination arrangement and instrumentation for quantitative assessment of illumination of display using fiber optics and lenses in hemispherical arrangement
CN111912603B (en) Method and system for calibrating phase type spatial light modulator based on optical differentiator
CN1200453C (en) Calibration method of electric charge coupler response linearity
CN106645219A (en) Method for measuring deviation degree and direction of illuminating electron beam, deviated from optical axis, of transmission electron microscope
DE102021200109A1 (en) Method for the areal determination of a map of at least one structure parameter of a structured surface of a diffractive optical element
DE19720330C1 (en) Method and device for measuring stresses in glass panes using the scattered light method
CN110907140A (en) Device and method for measuring grating period
DE4105509C2 (en) Scattered light measuring arrangement for examining the surface roughness

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C19 Lapse of patent right due to non-payment of the annual fee
CF01 Termination of patent right due to non-payment of annual fee